OTS9 Operator Theory: Advances and Applications Vol. S9 Editor: I. Gobberg Tel Aviv University Ramat Aviv, Israel Editorial Office: School of Mathematical Sciences Tel Aviv University Ramat Aviv, Israel Editorial Board: A. Atzmon (Tel Aviv) J. A. Ball (Blacksburg) L. de Branges (West Lafayette) K. Clancey (Athens, USA) L. A. Coburn (Buffalo) R. G. Douglas (Stony Brook) H. Dym (Rehovot) A. Dynin (Columbus) P. A. Fillmore (Halifax) C. Foias (Bloomington) P. A. Fuhrmann (Beer Sheva) S. Goldberg (College Park) B. Gramsch (Mainz) J. A. Helton (La Jolla)
M. A. Kaashoek (Amsterdam) T. Kailath (Stanford) H. G. Kaper (Argonne) S. T. Kuroda (Tokyo) P. Lancaster (Calgary) L. E. Lerer (Haifa) E. Meister (Darmstadt) B. Mityagin (Columbus) J. D. Pincus (Stony Brook) M. Rosenblum (Charlottesville J. Rovnyak (Charlottesville) D. E. Sarason (Berkeley) H. Widom (Santa Cruz) D. Xia (Nashville)
Honorary and Advisory Editorial Board: P. R. Halmos (Santa Clara) T. Kato (Berkeley) P. D. Lax (New York)
Birkhauser Verlag Basel . Boston . Berlin
M. S. Livsic (Beer Sheva) R. Phillips (Stanford) B. Sz.-Nagy (Szeged)
Operator Theory and Complex Analysis Workshop on Operator Theory and Complex Analysis Sapporo (Japan) Junel991 Edited by T.Ando I. Gohberg
Birkhiuser Verlag Basel· Boston· BerUn
Editors' addresses:
Prof. T. Ando Research Institute for Electronic Science Hokkaido University Sapporo 060 Japan Prof. I. Gohberg Raymond and Beverly Sackler Faculty of Exact Sciences School of Mathematical Sciences Tel Aviv University 69978 Tel Aviv, Israel
A CIP catalogue record for this book is available from the Library of Congress, Washington D.C., USA Deutsche Bib60thek Cataloging-in-Publication Data Operator theory ad complex ualysis / Workshop on Operator Theory aild Complex Analysis, Sapporo (Japan), June 1991. Ed. by T. Ando ; I. Gohberg. - Basel ; Boston ; Berlin : Birkhiiuser, 1992 (Operator theory; Vol. 59) ISBN 3-7643-2824-X (Basel ... ) ISBN 0-8176-2824-X (Boston ... ) NE: Ando, 1Suyoshi [Hrsg.]; Workshop on Operator Theory and Complex Analysis <1991, Sapporo>; GT
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© 1992 Birkhauser Verlag Basel, P.O. Box 133, CH-4010 Basel Printed in Germany on acid-free paper, directly from the authors' camera-ready manuscripts ISBN 3-7643-2824-X ISBN (1.8176-2824-X
v
Table of Contents Editorial Introduction
..........................
v. Adamyan Scattering matrices for microschemes . . . . . 1. General expressions for the scattering matrix . 2. Continuity condition References . . . . . . . . . . . . . . . . .
1
2 7 10
D. Alpay, A. Dijksma, J. van der Ploeg, H.S. V. de Snoo Holomorphic operators between Krein spaces and the number of squares of associated kernels . . . . . . O. Introduction . . . . . . . . . . . . . 1. Realizations of a class of Schur functions 2. Positive squares and injectivity . . . . . 3. Application of the Potapov-Ginzburg transform References . . . . . . . . . . . . . . . . . . D. Alpay, H. Dym On reproducing kernel spaces, the Schur algorithm, and interpolation in a general class of domains 1. Introduction . 2. Preliminaries. . . . . . . . . . . . . . . 3. 8(X) spaces . . . . . . . . . . . . . . . 4. Recursive extractions and the Schur algorithm 5. 'Hp( S) spaces . . . . . . . . 6. Linear fractional transformations 7. One sided interpolation 8. References . . . . . . . . . . M. Bakonyi, H.J. Woerdeman The central method for positive semi-definite, contractive and strong Parrott type completion problems . 1. Introduction . . . . . . . . . . 2. Positive semi-definite completions 3. Contractive completions . . . . . 4. Linearly constrained contractive completions References . . . . . . . . . . . . . . . .
IX
..
11 11 15 20
23 28
30
31 33
39 47 57 64 67
74
78 78
79 87
89 95
VI
I.A. Ball, M. Rakowski Interpolation by rational matrix functions and stability of feedback systems: The 4-block case Introduction . . . . . . . . . . . . . 1. Preliminaries. . . . . . . . . . . . 2. A homogeneous interpolation problem . 3. Interpolation problem . . . . . . . . 4. Parametrization of solutions . . . . . 5. Interpolation and internally stable feedback systems ~erences . . . . . . . . . . . . . . . . . . .
.96 .96 100 104 109 116 131 140
H. Bart, V.E. Tsekano1Jskii Matricial coupling and equivalence after extension 1. Introduction . . . . . . . 2. Coupling versus equivalence 3. Examples . . . . . . . . 4. Special classes of operators ~erences . . . . . . . . .
143 143 145 148 153 157
1.1. Fujii Operator means and the relative operator entropy 1. Introduction . . . . . . . . . . . . . . . . . 2. Origins of operator means . . . . . . . . . . . 3. Operator means and operator monotone functions 4. Operator concave functions and Jensen's inequality 5. Relative operator entropy ~erences . . . . . . . . . . . . . . . . . . .
161 161 162 163 165 167
171
M. Fujii, T. Furuta, E. Kamei An application of Furuta's inequality to Ando's theorem 1. Introduction . . . . . . 2. Operator functions . . . . . . . 3. Furuta's type inequalities . . . . 4. An application to Ando's theorem ~erences . . . . . . . . . . . .
173
173 175 176 177 179
T. Furuta Applications of order preserving operator inequalities O. Introduction . . . . . . . . . . . . . . . . . 1. Application to the relative operator entropy . . . 2. Application to some extended result of Ando's one ~erences . . . . . . . . . . . . . . . . . . .
180 180 181 185 190
VII
1. Gohberg, M.A. Kaashoek The band extension of the real line as a limit of discrete band extensions, I. The main limit theorem O. Introduction . . . . . . . . I. Preliminaries and preparations II. Band extensions . . . . . III. Continuous versus discrete References . . . . . . . . .
191 191 193 201 205 219
K. ]zuchi Interpolating sequences in the maximal ideal space of HOC II . . 1. Introduction . 2. Condition (A 2 ) 3. Condition (A3) 4. Condition (Ad References . . .
221 221 223 227 231 232
C.R. Johnson, M. Lundquist Operator matrices with chordal inverse patterns 1. Introduction . 2. Entry formulae 3. Inertia formula References . . .
234 234 237 243 251
P. Jonas, H. Langer, B. TextoriulJ Models and unitary equivalence of cyclic selfadjoint operators in Pontrjagin spaces Introduction . . . . . . . . . . . . . . . 1. The class :F of linear functionals . . . . . 2. The Pontrjagin space associated with ¢> E :F 3. Models for cyclic selfadjoint operators in Pontrjagin spaces 4. Unitary equivalence of cyclic selfadjoint operators in Pontrjagin spaces References . . . . . . . . . . . . . . . . . . . . . . . . . . . .
252 252 253 257 266 275 283
T. Okayasu The von Neumann inequality and dilation theorems for contractions 1. The von Neumann inequality and strong unitary dilation 2. Canonical representation of completely contractive maps 3. An effect of generation of nuclear algebras References . . . . . . . . . . . . . . . . . . .
285 285 287 289 290
L.A. Sakhno'IJich Interpolation problems, inverse spectral problems and nonlinear equations References . . . . . . . . . . . . . . . . . . .
292 303
vm S. Takahashi Extended interpolation problem in finitely connected domains Introduction . . . . . . . . . . . . I. Matrices and transformation formulas II. Disc Cases . . . . . . . . . III. Domains of finite connectivity. R.eferences . . . . . . . . . . . E.B. TsekanotJskii Accretive extensions and problems on the Stieltjes operator-valued functions relations . . . . . . . . . . . . 1. Accretive and sectorial extensions of the positive operators, operators of the class C(9) and their parametric representation 2. Stieltjes operator-valued functions and their realization . 3. M.S. Livsic triangular model of the M-accretive extensions (with real spectrum) of the positive operators . . . . . 4. Canonical and generalized resolvents of QSC-extensions of Hermitian contractions R.eferences . . . . . . . . . . . . . . . . . . . . . V. VinnikotJ Commuting nonselfadjoint operators and algebraic curves 1. Commuting nonselfadjoint operators and the discriminant curve 2. Determinantal representations of real plane curves 3. Commutative operator colligations . . . . . . . . . . . 4. Construction of triangular models: Finite-dimensional case 5. Construction of triangular models: General case . . . 6. Characteristic functions and the factorization theorem R.eferences . . . . . . . . . . . . P.y. Wu AD (?) about quasinormal operators 1. Introduction . . . . . . 2. Representations 3. Spectrum and multiplicity 4. Special classes . . 5. Invariant subspaces 6. Commutant . 7. Similarity . . . . 8. Quasisimilarity . . 9. Compact perturbation 10. Open problems R.eferences . . . .
Workshop Program . List of Participants
305 305 306 309 318 326
328 329 335 345 343 344
348 348 350 353 355 359 364 370 372 372 374 377
379 380 382 385 387 391 393 394
399
402
IX
EDITORIAL INTRODUCTION
This volume contains the proceedings of the Workshop on Operator Theory and Complex Analysis which was held at the Hokkaido University, Sapporo, Japan, June 11 to 14, 1991. This workshop preceeded the International Symposium on the Mathematical Theory of Networks and Systems (Kobe, Japan, June 17 to 21, 1991). It was the sixth workshop of this kind, and the first to be held in Asia. Following is a list of the five preceeding workshops with references to their proceedings: 1981 Operator Theory (Santa Monica, California, USA) 1983 Applications of Linear Operator Theory to Systems and Networks (Rehovot, Israel), OT 12 1985 Operator Theory and its Applications (Amsterdam, the Netherlands), OT 19 1987 Operator Theory and Functional Analysis (Mesa, Arizona, USA), OT 35 1989 Matrix and Operator Theory (Rotterdam, the Netherlands), OT 50 The next Workshop in this series will be on Operator Theory and Boundary Eigenvalue Problems. It will be held at the Technical University, Vienna, Austria, July 27 to 30, 1993. The aim of the 1991 workshop was to review recent advances in operator theory and complex analysis and their interplay in applications to mathematical system theory and control theory. The workshop had a main topic: extension and interpolation problems for matrix and operator valued functions. This topic appeared in complex analysis at the beginning of this century and now is maturing in operator theory with important applications in the theory of systems and control. Other topics discussed at the workshop were operator inequalities and operator means, matrix completion problems, operators in spaces with indefinite scalar product and nonselfadjoint operators, scattering and inverse spectral problems. This Workshop on Operator Theory and Complex Analysis was made possible through the generous financial support of the Ministry of Education of Japan, and also of the International Information Science Foundation, the Kajima Foundation and the Japan Asso-
x ciation of Mathematical Sciences. The organizing committee of the Mathematical Theory of Networks and Systems (MTNS) has rendered financial help for some participants of this workshop to attend MTNS also. The Research Institute for Electronic Science, Hokkaido University, provided most valuable administration assistance. All of this support is acknowledged with gratitude.
T. Ando,
I. Gohberg
August 2, 1992
Operator Theory: Advances and Applications, Vol. 59 © 1992 Birkhauser Verlag Basel
1
SCATTERlNG MATRlCES FOR MICROSCHEMES
Vadim Adamyan A mathematical model for a simple microscheme is constructed on the basis of the scattering theory for a pair of different self-adjoint extensions of the same symmetric ordinary differential operator on a one-dimensional manifold, which consist of a finite number of semiinfinite straight outer lines attached to a "black box" in a form of a flat connected graph. An explicit expression for the scattering is given under a continuity condition at the graph vertices.
Contemporary technologies provide for the formation of electronic microschemes composed of atomic clusters and conducting quasionedimensional tracks as "wires" on crystal surfaces. Electrons travelling along such "wires" behave like waves and not like particles. The explicit expressions for the functional characteristics of simple microschemes can be obtained using the results of the mathematical scattering theory adapted for the special case when different self-adjoint extensions of the same symmetric ordinary differential operator on a one-dimensional manifold 0 are compared. The manifold 0 simulating the visual structure of a microscheme consists of m « 00) semiinfinite straight outer lines attached to a "black box" in a form of a flat connected graph. Different self-adjoint extensions of the mentioned symmetric operator distinguish only in boundary conditions at terminal points of outer lines. Having the scattering matrix for the pair of any self-adjoint operators of such kind with the special extension corresponding to the case of disjoint isolated outer lines one can immediately calculate by known formulae the high-frequency conductance of the "black box" . In the first section of this paper the general expression for the scattering matrix for two self-adjoint extensions of the second-order differential operator in L2(0) is derived on the basis of more general results obtained in [I]. The detailed version of these results is given in the second part for the most important case when functions of the extension domain satisfy the condition of continuity
Adamyan
2
at the points of connection of outer lines to vertices of the graph. This work was initiated by some ideas from the paper [2]. 1. General expressions for the scattering matrix.
Remind the known concepts of the scattering theory. Let L be a Hilbert space and Ho, H be a pair of self-adjoint operators on L. Denote by Po the orthogonal projection on the absolutely continuous subspace of Ho. If the resolvent difference
(H - zI)-l - (Ho - zI)-l at some (and, consequently, at any) nonreal point z is a nuclear operator, then by the Rosenblum-Kato theorem the partial isometric wave operators
W±(H, Ho) = s-l±im eiHte-iHot Po 1-+
00
exist and map the absolutely continuous subspace of Ho onto the same subspace of H [31. The scattering operator
is unitary on PoL and commutes with Ho. The scattering matrix SP), -00 < ,\ < 00, is the scattering operator S(H, Ho) in the spectral representation of Ho. Consider the special case when Hand Ho are different self-adjoint extensions of the same densely defined symmetric operator A in L with finite defect numbers (m, m). Let (ev)r be any basis of the defect subspace ker[A· + ill. Put
ev(z)
= (Ho + il)(Ho -
zI)-lev,
II
= 1, ... , m,
and introduce the matrix-function .1.(z),
.1."v(z)
= (Hoz + I)(Ho -
zI)-le v , e,,),
II,
p.
= 1, ... , m.
According to the M. G. Krein resolvent formula for fixed Ho and arbitrary H m
(1)
(H - zI)-l = (Ho - zI)-l -
L
([.1.(z)
+ QI- l ) "V (., ev("z»)e,,(z)
",v=l
where a parameter Q is a Hermitian matrix [4]. The following parametric representation of the scattering matrix S('\) for extensions H and Ho was derived using the formula (1) in [1].
3
Adamyan
Take any decomposition of the absolutely continuous part Lo of H0 into a direct integral
Lo = [ : ffiK(A) dA. Without loss of generality one can assume dimK(A) :::; m. Let h,,(A) be a spectral image of the vector Poe". Then
(2)
SeA) = 1+ 21ri(A2
+ 1) ~)[~ *(A + iO) + Qt1) 1''' (- , h,,(A» K(>.)hl' (A). 1'."
Now we are going to adapt (2) for the case when a given symmetric operator A is a second-order differential operator on the above mentioned one-dimensional manifold o of the graph Oint and m outer semiaxes.
All self-adjoint extensions of A in L2(0) differ only by boundary conditions at the terminals (e~)i of outer lines and the corresponding connecting points (et)i from the inside of the "black box" Oint. Take as Ho a special extension decomposing into an orthogonal sum : m
Ho = HPnt ffi
L ffiH2j 1:=1
HPnt : L 2 (Oint) H2 : L2(E+)
--+ L2(Oine)j --+
L2(E+), f'(e2) =
(H2f)(z) = !..r(z), I'
o.
As a consequence of the decomposition of Ho the Green function G~(z, y), z, YEO, of the operator Ho, i.e. the kernel of the resolvent [Ho - wlj-1 in L2(0) possesses the property: for any regular point w G",(z, y) = 0 if z E Oint and y belongs to any outer line and vice versa or if z and y are points of different outer lines. Describe the assumed properties of Hfnt. This operator can be considered as a self-adjoint extension of the orthogonal sum A int = E" ffiAi" of regular symmetric differential operators of the form
d
d
Ai" = - deP" (e) de
+ q,,(e)
Adamyan
4
on the corresponding segments (ribs) (a",~,,) of the graph with continuous real-valued functions p,,(e), q,,(e) and p,,(e) > o. The functions f(e) from the Ai" domain in L2(a",~,,) are continuously differentiable and satisfy boundary conditions
f(a,,)
= f(~,,) = OJ
I'(a,,)
= f'(~,,) = O.
Note that every Ai" has defect indices (2N, 2N) where N is the number of the graph ribs. Let B" be the "soft" self-adjoint extension of Ai", i.e. the restriction of the conjugate operator Ai" on the subset of functions f(e) such that
Consider the special self-adjoint extension B = E" €BB" of A int . The operator B can be taken as the part HPnt in the decomposition of Ho. In this case the Green function ~(z, y) on Oint X Oint coincides with the Green function ~(z, y) of Band in its turn E~(z, y) is nonzero only if "z" and "y" belong the same segments (a",~,,) of Oint and on these segments E~(z, y) coincides with the Green functions of B". Note that ~( . ,y) E L2(0) for any regular point wand any yEO. From the definition of the Green function ~(z, y) and its given properties it follows that the functions (G~i(Z, e~»~ together with the functions (G~i(Z, a,,), G~i(Z,~,,»~ form a basis in the defect subspace M == ker[A* + ill of A. Put '12,,-1
= a",
'12"
= ~'"
1/
= 1, ... , Nj
'12N+k
= e~,
k
= 1, ... , mj
and introduce the matrix-function r(w),
According to the Hilbert identity for any regular points w, z of Ho and any z, yEO
(3)
y) - ~(z, y)]. 10.r du ~(z, u)G~(u, y) = _1_[G~(z, w - z
As a consequence of (3) and the relation G~(z, y) = G&(z, y) we have
(4)
~,.,,(w) = =
In ([1 + wHo][Ho - wl]-1~i(·' '1,,»)(Z)~i(Z, r~,,(w) - ilr,.,,(-i) + r",.(-i»).
'1,.)dz
Adamyan
5
Let H be an arbitrary self-adjoint extension of A in £2(0). The Krein resolvent formula (1) and (4) yield the following expression for the Green function Gw(z, y) of H through ~(z,y):
2N+m
Gw(z,y) = ~(z,y) -
(5)
L
([rO(w) +Qtl)/",G~(Z,1/I')G~(1/",Y),
1'.,,=1
where Q is a Hermitian matrix. Now to construct the scattering matrix S('\) for the pair H, H o notice that the parts B" of H o as regular self-adjoint differential operators have discrete spectra and the parts H2 on the outer lines form the absolutely continuous component of Ho. Consequently the first 2N basis vectors G~i(Z, 1/,,) of the defect subspace M_ are orthogonal to the absolutely continuous subspace of Ho and unlike the last m basis vectors G~i(z, T/2N+k) = ~i(Z, e2) belong to this subspace. The natural spectral representation of the absolutely continuous part of Ho, i.e. of the orthogonal sum of the operator H2, is the multiplication operator on the independent variable A in the space of em-valued functions £2(0,00; em). The corresponding spectral mapping of the initial space can be defined in such way that the defect vectors G~i (z, e2) turn into the vector-functions
(6) where
A> 0, ek
E em are the columns
Using all above reasons we get immediately from (2) that S(A) is the (m x m)-matrixfunction and
Represent the parameter Q and the matrix-function rO(w) in the block-diagonal form
(8)
Q = [;.
::],
rO(w) = [r?not(W)
0
-i~lm
]
'
where W is a Hermitian (m x m)-matrix, 1m is the unit matrix of order m and the matrixfunction r?nt(w) is determined by the Green function ~ of the extension B as follows
~.(9)
Adamyan
6
Using (7) and (8) we get the formula:
(10)
S(A) = {i.[¥In
+W
- M*[L
+ r?nt(A -
iO)t 1 M } x
x {-i.[¥In + W - M*[L + r?nt(A _ iO)t 1 M}-1 This expression describes all possible scattering matrices for microschemes comprised of given m outer lines and a given set of N ribs. The parametric matrices W, M,
L contain information on the geometrical structure of the "black box" and the boundary conditions at all vertices including the connecting points to the outer lines. Without loss of generality we can consider that all connecting points are the graph vertices. Single out now the scattering matrices for microschemes which differ only by the way the outer lines are connected to the definite inputs of the "black box", i.e. to the certain vertices of the definite graph
n.
Notice that this limiting condition generally
speaking leaves the Hermitian matrix W arbitrary. The matrix can now vary only as far as the subspace ker M M* remains unchanged. In what follows we will assume that this subspace and, respectively, its orthogonal complement in
[:2N
are always invariant
subspaces of the L matrix. Let Co be the orthogonal projector on the subspace ker M M* in
[:2N.
Under the above condition and for various types of connection of outer lines to
certain graph vertices only the block CoLCo of the L matrix is modified. Notice that this block for a "correct" connection is always invertible. Consider now the connections for which the L matrix in (8) remains unchanged. This matrix is a parameter in the Krein formula when resolvents of B and a definite self-adjoint extension HPnt of Aint are compared. Let rint(w) be the matrix-function which is determined by the Green function E", of Hf:.t like r?nt(w) in (9) by E~. According to the Krein formula of the form (5) (11)
rint(W) = r?nt(w) - r?nt (w)[r?nt (w) = L[r?nt(w)
+ Lt 1r?nt(w)
+ Lt 1r?nt(w) =
L - L[r?nt(w)
+ Lt 1L.
Taking into account that by the assumption that the block CoLCo of the Hermitian matrix L is invertible on the subspace ker M M* C [:2N, denoting by Q the corresponding inverse operator in this subspace and using (11) we can write
(12)
M*[r?nt(w)
+ L1- 1 M = M*QL[r?nt(w) + L1- 1 LQM = M*QM - M*Qrint(w)QM.
Adamyan
7
Inserting the last expression into (10) we find that the scattering matrix S(A) for the connections without changing the parameter L and the subspace ker MM· has a form
(13)
where the matrix parameters
W(= W - M·QM),
M = QM
depend on the boundary conditions at those vertices of the graph 0, which are connected with the outer lines. If there are reasons to consider that as a result of the connection of outer lines to the graph 0 the matrices Land M are changed into M', L' so that ker(L - L') = ker M'· M' = ker M· M, then it is natural to use the representation (14)
S(A) = [iJ¥"In + H(A - iO)] [-iJ¥"In + H(A _ iO)] -1, H(w) = W + M'· [L + r'nt(w)(PO - QL' Po)] -1 x [por.nt(w)Qo - I] M'.
The formula (14) can be obtained from (10) using the relation (11).
2. Continuity condition. From the physical point of view the most natural are self-adjoint extensions of
A satisfying the continuity condition at the graph vertices. This condition states that all functions from the domain of any such extension possess coinciding limiting values at any vertex along all ribs incident to this vertex. Irrespective to the present problem consider now the structure of the Krein formula (5) with parameter Q for arbitrary self-adjoint extensions satisfying the continuity condition in every vertex. Take a vertex with 8 incident ribs, i.e. the vertex of degree 8. It is convenient to enumerate the extreme points of the ribs at the vertex as TJl, .. . , TJ.. Replacing x in Eq. (5) by TJ. for arbitrary y we obtain (15)
O",(TJ., y) =
L Q.,.([rO(w) + Q]-I) ,,"~(TJ", y). ,.,11
It follows from the continuity condition that
(16)
0",('110 y)
= 0",(1/2, y) = ... = 0",('1., y).
Adamyan
8
Since y and w in (15) and (16) are arbitrary it is obvious that the matrix Q in fact transforms any vector from C 2N +m into a vector with equal first 8 components. Denote by J, the matrix of order 8 all components of which are unity. As Q is Hermitian, it is nothing but the following block matrix
where h is a real constant and Q' is a Hermitian matrix of the rank 2N + m -
8.
Since the
same procedure is valid for any vertex of arbitrary degree, the matrix with the suitable enumeration of the extreme points of the ribs and outer lines takes the block-diagonal form
o o. 1 ,
(17)
o where 1 is the total number of the graph vertices and of the vertices. Thus the following lemma is valid.
h,l., 81, ... ,81
are corresponding degrees
LEMMA. The parameter Q in the Krein formula (5) for extensions satisfying
the continuity condition is the Hermitian matrix such that nonzero elements of every its row (column) are equal and situated at the very places where the unities of the incidence matrix of the graph 0 are. Let the matrix Q be already reduced to the block-diagonal form (17) by a corresponding enumeration of extreme point of ribs and terminal points of outer lines.
In this case the matrices W, M and CoLCo of the representation (8) coincide with the diagonal matrix h1 ID>= [
o where the parameters h 1 , • •. ,hm are determined by the boundary conditions in vertices to which the outer lines are connected. Using this fact and (13) we infer: THEOREM. Let H be a self-adjoint extension of A in L2(0) satisfying the continuity condition and univalently connected with the set of parameters h 1 , ••• , h, of the corresponding matrix Q of the form (17) generating H in accordance with the Krein formula and let Ho be the special extension of A decomposing into an orthogonal sum of
Adamyan
9
the self-adjoint operators on the graph and on the outer lines. The scattering matrix S(A) for the pair Ho, H admits the representation (18)
where f.k(W) = E",(f/., f/k) and E",(e, f/) is the Green function of the self-adjoint extension HPnt of A. nt satisfying the continuity condition and determined by the same set of parameters hI, ... , h, for the same vertices like H is. From the representation (18) it is obvious that the analytic properties of the scattering matrix S(A) are essentially determined by those of the matrix f(w) constructed by the Green function of the separated graph. For the regular differential operator the matrix (E",(f/., f/k))~ is the meromorphic R-function. The natural problem thus arises of the partial recovery of the graph structure and the operator on it from the matrix S(A) or, equivalently, by the matrix f. In the case when the graph is reduced to a single segment this problem is the well-known problem of recovery of a regular Sturm-Liouville operator from spectra of two boundary problems. We hope to carry out the consideration of the former problem in a more general case elsewhere. In conclusion, as an example, consider an arbitrary graph with only two outer lines connected to the same vertex. In this case S(A) is the second order matrix-function but the determining matrix f(w) is degenerate and takes the form
where
eis the internal coordinate of the vertex of the graph tangent to the outer lines. The scattering matrix according to (18) now can be put in the usual form
where
i r(A) - - - - - = = - - 2E>.(e,eh!A/1' - i' are, respectively, the reflection and transition coefficients. Notice that according to the Landauer formula the resistance of the graph is given by
where Ro is the quantal resistance, i.e. the universal constant.
Adamyan
10
REFERENCES 1.
Adamyan, V. M.j Pavlov, B. S.: Null-range potentials and M. G. Krein's formula of generalized resolvents (in Russian), Studies on linear operators offunctions. xv. Research notes ofscientific seminars of the LBMI, 1986, v.149, pp. 723.
2.
Exner, P.; Seba, P.: A new type of quantum interference transistor, Phys. Lett. A 129:8,9 (1988), 477-480.
3.
Reed, M.; Simon, B.: Methods of modern mathematical physics. III: Scattering theory, Academic Press, New York - San Francisco - London, 1979.
4.
Krein, M. G.: On the resolvents of a Hermitian operator with the defect indices (m, m) (in Russian), Dokl. Acad. Nauk SSSR 52:8 (1946), 657-660.
Department of Theoretical Physics University of Odessa, 270100 Odessa Ukraine MSC 1991: 8tU,47A40
11
Operator Theory: Advances and Applications, Vol. 59 © 1992 Birkhliuser Verlag Basel
UOWMORPIDC OPERATORS BETWEEN KREIN SPACES AND THE NUMBER OF SQUARES OF ASSOCIATED KERNElS
D. Alpay, A. Dijksma, J. van der Ploeg, U.S.V. de Snoo Suppose that e(z) is a bounded linear mapping from the Krein space 15 to the KreIn space ~, which is defined and holomorphic in a small neighborhood of z = O. Then often e admits realizations as the characteristic function of an isometric, a coisometric and of a unitary colligation in which for each case the state space is a KreIn space. If the colligations satisfy minimality conditions (i.e., are controllable, observable or closely connected, respectively) then the positive and negative indices of the state space can be expressed in terms of the number of positive and negative squares of certain kernels associated with e, depending on the kind of colligation. In this note we study the relations between the numbers of positive and negative squares of these kernels. Using the Potapov-Ginzburg transform we give a reduction to the case where the spaces 15 and ~ are Hilbert spaces. For this case these relations has been considered in detail in [DiS!]. O.
INTRODUCTION
Let (0', [.,.]1\') and
(~,
["']l!!), or 15 and ~ for short, be Krein spaces and denote by L(15,~)
the space of bounded linear operators from 15 to write
r
~
(we write L(O') for L(lJ,15)). If
TEL(lJ,~),
we
(EL(~,!J)) for the adjoint of T with respect to the indefinite inner products [.,.]1\' and
["']l!! on the spaces !J and~.
invertible) if y-l EL(~,!J,). valued functions
We say that
TEL(lJ,~)
is invertible (instead of boundedly
By S(O',~) we denote the (generalized) Schur class of all L(lJ,~)
e, defined and holomorphic on some set in the open unit disc
D={ZEC Ilzl < I};
we denote by :b(e) the domain of holomorphy of e in D. The class of Schur functions e for which OE:b(e) will be indicated by S°(O',~).
If:b is a subset of D, we write :b*={zlzE:b}.
eES(!J,~) we associate the function e defined by e(z) = e(z)*.
and if eES°(lJ,~), then eES°(lJ,~). We associate with O'e(Z,W) = I-e(w) *e(Z), l-wz
with values in L(!J) and
L(~),
z,wE:b(e),
e the
O'e(Z,W)
respectively, and the kernel
With each
Clearly, eES(~,15), :b(e) = :b(e)*
kernels
l-e(w)e(z)* l-wz
z,WE:b(e)*,
12
Alpayetal.
Sa(Z,'ID) = [
I-8~:~:8(Z)
8(Z):=:('ID)* ),
8(w)-8(z)
w-z with values in
L(lJGl~),
where
z,'IDe:b(8)n:b(8)*,
z~w,
I-8(iO)8(z)*
l-wz O'Gl~
stands for the orthogonal sum of the Krein spaces 0' and
~.
Here I is the generic notation for the identity operator on a Krein space, so in the kernels I on~.
is the identity operator on 0' or
If we want to be more specific we write, e.g., Ifj to
indicate that I is the identity operator on 0'.
In this paper we prove theorems about the
relation between the number of positive (negative) squares of the matrix kernel Sa and those of the kernels ua and ua on the diagonal of Sa. We recall the following definitions.
Let st be a Krein space.
A kernel K(z,'ID) defined for Z,'ID
in some subset :b of the complex plane ( with values in L(st), like the kernels considered above, is called nonpositive (nonnegative), if K(z,'ID)* = K('ID,z), z,'IDe:b, so that all matrices of the form ([K(zi,zj)fi,filltl7. i =1> where neN,
zl> ... ,zne:b and fl> ... ,fnest are arbitrary, are hermitian,
and the eigenvalues of each of these matrices are nonpositive (nonnegative, respectively).
More
generally, we say that K(z,'ID) has /\, positive (negative) squares if K(z,'ID)*=K('ID,z), z,'IDe:b, and all hermitian matrices of the form mentioned above have at most/\' and at least one has exactly/\, positive (negative) eigenvalues.
It has infinitely many positive (negative) squares if for each
/\, at least one of these matrices has not less than /\, positive (negative) eigenvalues.
We denote
the number of positive and negative squares of K by sq+(K) and sqJK), respectively.
If, for
example, sq_(K) =0, then K(z,'ID) is nonnegative. In the sequel we denote by ind+st and ind_st the dimensions of the Hilbert space st+ and the anti Hilbert space st_ in a fundamental decomposition .It=st+Glst_ of st. Then ind±st=sq±(K) where K is the constant kernel K(z,'ID) =1, and the indices are independent of the chosen fundamental decomposition of st.
Whenever in this paper we use the
term Pontryagin space we mean a Krein space, st, say, for which ind_st < 00. The main theorems in this paper concern the relation between the values of sq±(Sa) on the one hand and the values of sq±(ua) and sq±(ue) on the other hand.
The most general one implies
that, if /\'eNu{O}, then sq_(Sa)=/\' if and only if sq_(Ua) =sq_(ua) =/\" and sq+(Sa)=/\' if and only if sq+(ua)=sq+(ue)=/\,. To formulate this theorem we consider two fundamental decompositions lJ'=lJ'+GllJ'_ and ~=~+Gl~_ of 0' and~, and we denote by P± the orthogonal projections on 0' onto the spaces O'± and by Q± the orthogonal projections on ~ onto the spaces ~±. THEOREM
0.1. Let 0' and ~ be Krein spaces and let 8eS(0',~).
Then:
(i) sq_(Sa)
If (i) and (ii) are valid, then sq_(ua) =sq_(ue) = sq_(Sa) and Q_8(z)lfj_ eL(lJ'_,~_) is invertible for all except at most 2sq_(Sa) points ze:b(8).
Alpayetal.
13
Of course Theorem 0.1 remains valid if the minus sign is everywhere replaced by the plus sign. Note that if Q-8(zlIIJ_ eL(tJ_,~_) is invertible, then ind_tJ = ind_~.
Theorem 0.1 is closely related
to the theorem which states that if TeL(tJ,~) is a contraction (i.e, r*T~IIJ)' then it is a bicontraction (i.e., T and
1'*
are both contractions) if and only if Q1hJ_ is invertible; see
[DR] for a recent account of this result and related results.
The existence of a contraction in
a Krein space which is not a bicontraction can be used to give a counterexample to the equality in Theorem 0.1 when the kernel Se(z,w) has an infinite number of negative squares. TeL(tJ) be a contractive but not bicontractive operator, set sq_(ua) = 0, but we have that sq_(Se) = sq_(ua) = 00.
that the nxn matrix (1/(l-ZiZj)), where
~=
Indeed, let
tJ and take 8(z)=T on D. Then
In proving these equalities we used the fact
ZhZ2"",Zn
are n different points in D, is positive.
This follows for instance from the formula 1/(I-ziii) = (21rflf:7r(eiT _zfl(e- iT -iiif1dr, z,weD. In the case where tJ and ind+~,
~
are Krein spaces such that either their positive indices ind+tJ and
or their negative indices ind_tJ and
ind_~,
are finite, Theorem 0.1 can be sharpened.
We
only state the version for which the last condition on the indices holds; the one for which ind+tJ and
ind+~
are finite is mutatis mutandis the same.
THEOREM 0.2.
Let tJ and
~
be Puntryagin spaces,
8eS(tJ,~)
and let KeNu {O}.
Then the
following three statements are equivalent. (i)
sq_(Sa) = K.
(ii)
sq_(ua) = K and ind_tJ =
(iii)
sq_(Ua)=K
and
ind_~.
ind_tJ=ind_~.
If (i) - (iii) are valid then Q_8(z)IIJ_ eL(tJ_,~_) is invertible for all, except for at most
K,
points ze:b(8). Moreover, if these cunditiuns hold, then 8 can be extended to a meromorphic functiun un D, and the number of negative squares of each of the three kernels associated with the extended functiun coincides with the number of negative squares of the correspunding kernel . for the functiun 8. This theorem corresponds to the fact that if
ind_tJ=ind_~
also a bicontraction; see, for example, [IKL], [DR].
then every contraction
Theorem 0.2 implies that. if ind_tJ =
then sq_(Se) = sq_(ua) = sq-lua), which for the case where tJ and proved in [DISl].
TeL(tJ,~)
~
is
ind_~ < (Xl,
are Hilbert spaces was already
The equality here means that either all three numbers sq_(Se), sq_(ua),
SQ_(ua) are infinite, or one of them is finite in which case all three are finite and equal.
If
in
To avoid confusion with the
signs we give a counterexample to Theorem 0.2 in which all signs are reversed. Take tJ=C2 • ~=C and define the lx2 matrix function 8eSo(tJ,~) by 8(z) = (kz, I), zeD, where keC and Ikl < 1. Then ua Is a 2x2 matrix kernel, Uij is a scalar kernel and Sa is a 3x3 matrix kernel.
have that SQ+(ua)=O, but sq+(Se) = SQ+(ua) =00.
In this case we
14
Alpayetal. The proofs of Theorems 0.1 and 0.2 which we give are basically a variation of the proof of the
theorem about the characterization of bicontractions in a Krein space mentioned previously: we also make use of the Potapov-Ginzburg transform.
We show in this paper that, if the kernels
associated with 8 have a finite number of negative squares, then the Potapov-Ginzburg transformation of 8 can be defined, and, if we denote this transformation by L, then sq_(O'E)=sq_(O'e), sq_(0'L')=sq_(0'9) and sq_(5E )=sq_(5e ).
Since L is essentially a Schur function
between Hilbert spaces, the proofs of Theorems 0.1 and 0.2 are obtained through a reduction of the general case to the case where iJ and (IJ are Hilbert spaces, which was considered in [DLS1]. Theorems 0.1 and 0.2 are related to Theorem 7.6 in the excellent lecture notes by Ando [An], which contains a detailed account of the case
It =
o.
To point out the connection we state the
following related result. THEOREM
0.3. Let iJ and (IJ be Krein spaces and let 8eS(3',(IJ).
If :b(8) =D, then the follOUJing
assertions are equivalent. (a)
For each zeD: 8( z) is a bicontraction.
(b)
For each zeD: 8(z) is a contraction
(c)
For each zeD: 8(z) is a contraction and P_8(z)I~_ eL«(IJ_,iJ_) is invertible.
(d)
sq-!O'e) = 0 and sq_(O'e) = o.
(e)
sq_(5e ) = o.
and
Q_8(z)liJ_ eL(iJ_,(IJ_) is invertible.
The equivalences (a)#(b)#(c) are alluded to above.
The implications (e)-+(d), (d) ... (a) are
trivial: the first one follows from the fact that the kernels O'e(z,w) and 0'9(z,w) are on the diagonal of 5e (z,w) and the second follows by taking w=z in O'e(z,w) and 0'9(z,'IO). To prove the implication (a)-+(e), Ando in [An] uses complementation theory and the theory of operator rangesj see also [82,3].
On the other hand on account of the invertibility of Q_8(z)liJ_eL(iJ_,(IJ_) the
implication can be reduced to one where the spaces involved are Hilbert spaces, and then the implication can be and has been proved in different waysj see [SF] and [8R].
In this paper we
are interested in the equivalence (d)#(e), which has been proved by McEnnis [Mc]. The purpose of this paper is to generalize this equivalence to the case where we allow the kernels associated with 8eS(iJ,(IJ) to have negative squares.
These generalizations are formulated in
Theorems 0.1 and 0.2. Note that we do not require that :b(8) =D. The kernels associated with 8eSo(iJ,(IJ) have appeared in a number of papers, frequently in connection with the theory of (co- )isometric and unitary colligationsj of the more recent papers,
we
mention
for
[DLS1,2,3], [M] and [V].
instance
[A],
[AD1,2,3],
[AG1,2],
[An],
If iJ and (IJ are Hilbert spaces then 8
[81,2,3],
[DC],
[CDLS],
can be written as thEl
characteristic function of (a) a closely innerconnected isometric colligation, (b) a closely outerconnected
coisometric
colligation,
as
well as
of
(c)
a
closely
connected
unitary
Alpayetal.
15
colligation.
If in all three cases we denote by Sf the state space of the colligation, then Sf is
a Krein space with ind±(Sf) = sq±(ue) in case (a), ind±(Sf) = sq±(t1a) in case (b) and ind±(Sf) = sq±(Se) in case (c).
Proofs of these results can be found in, e.g., [DLSl)j see also Remark 1.1 in
Section 1 of this paper. In the general case where ij and @J are Krein spaces, 8eS°(ij,@J) can also be realized on a neighborhood of 0 as the characteristic function of a minimal unitary or (co-) isometric colligation.
In this case the state space of the colligation is uniquely determined
by 8 up to weak isomorphisms and so its positive and negative indices are uniquely determined by 8, cf. Section 1 below. We briefly describe the contents of the three sections of this paper.
In Section 1
(REALIZATIONS OF A CLASS OF SCHUR FUNCTIONS) we consider the case where ij and @J are Hilbert spaces, and we recall some facts from [DLS1).
For this case we show in Section 2 (POSITIVE
SQUARES AND INJECTIVITY) that if the kernels have a finite number of positive squares, then the operator function Q_8(z)IB'_ is invertible.
As an aside we prove a simple result about the
positivity of the Schur product of nonnegative matrices.
The main theorems of this paper,
Theorem 0.1 and Theorem 0.2, are proved in Section 3 (APPLICATION OF THE POTAPOV-GINZBURG TRANSFORM) by invoking the results of the previous sections.
There we also recall the
definition of the Potapov-Ginzburg transform. In a sequel to this paper we give an interpretation of our results from the point of view of
reproducing kernel Pontryagin spaces and operator ranges. We show how this leads to models for contractions in Pontryagin spaces in which certain maximal negative invariant subspaces can be displayed explicitly. 1. REALIZATIONS OF A CLASS OF SCHUR FUNCTIONS A colligation (system or node) is a quadruple Ll = (Sf,ij,@JjU) consisting of three Krein spaces Sf (the state space), ij (the incuming space) and @J (the outgoing space) and an operator UeL(SfEllij,SfEll@J) (the connecting operator). We often write Ll= (Sf,ij,@JjT,F,G,H) to indicate that U has the operator matrix decomposition
where TeL(Sf) (the basic operator), FeL(ij,Sf), GeL(Sf,@J) and HeL(ij,@J). The colligation is called isometric, coisometric or unitary if the connecting operator has this property. Ll=(Sf,ij,@JjT,F,G,H) is called closely innerconnected (controllable) if
Sf= V R((I-zTf1F)=V{TRFflneNu{0}, 'eij}, zaN
closely outerconnected (observable) if
Sf= V R((I-zT*f1c*)=V{T'"'c*glneNu{0}, ge@J}, ZEN
A colligation
Alpayetal.
16 and it is called closely connected if ,Il'= V (R((l-zT)-IF)uR((l-zT*f1c*)). zeN
In these cases N stands for a small neighborhood around 0 and V
signifies the closed linear
zeN
span of the sets with index zeN. if
minimal
it
is
closely
We call an isometric (coisometric, unitary) colligation
innerconnected
(closely
outerconnected,
closely
connected,
respectively). A weak isomorphism V from a Krein space .!t to a Krein space .!t' is a mapping with dense domain D(V) in ,Il' and dense range R(V) in ,Il" such that [vx,Vyl!t, = [x,y)lt, x,yeD(V). weakly
isomorphic,
then
ind±(.!t) = ind±(.!t').
Two
colligations
If.!t and .!t' are
Ll= (.!t,fj,(g;T,F,G,H)
and
Ll' = (St', fj, (g; T' , F' ,G' , H') with the same incoming and outgoing spaces fj and (g are called weakly isomorphic if H = H' and there exists a weak isomorphism V from .!t to .!t' such that
T' ( G'
0) =
F') (V0 I H'
0)
(V0 I
(T F) on G H
( D(fjV) ) .
If V can be extended to an isomorphism (unitary operator) from .!t' onto .!t, then of course the
colligations Ll and Ll' are called isomorphic or unitarily equivalent.
Associated with a
colligation Ll = (St,fj,(g;T,F,G,II) is the socalled characteristic function e(z) =e,a(z) =H+zG(l-zT)-IF,
defined for all z in some neighborhood of O.
Clearly, eeSo(fj,(g).
If for eeSo(fj,(g) there is a
colligation Ll such that e( z) = e,a (z) in a neighborhood of 0, then the colligation is called a realization of e.
Realizations in a general Krein space case are studied in, e.g., [Azl,2),
[81,2,3), [(;DLS), [DLS3), [M), [Y) and for a special class in [DLSl). REMARK
1.1. If fj and (g are Krein spaces, eeSo(fj,(g) and e=e,a on :b(e)n:b(e,a) for some isometric
(coisometric, ind±.!t~sq±(SH)'
unitary)
colligation
respectively).
If
inequality the equality sign prevails.
Ll = (.!t,fj,(gjU), the
then
colligation
ind±.!t~sq±(ua)
is minimal then
in
(ind±.!t~ sq±(ue),
the
corresponding
These (in-)equalities can easily be deduced from the
following relations between the kernels and the inner product of the state space .!t of Ll.
For
fl,fzefj and gl>gze(g we have if Ll is isometric;
(i)
[u H (z,w)fl>fz)!j = [(l-zTfIFfl>(l-wT)-IFf2)lt,
(ii)
[ue(z,w)gl,gz)l!I = [(l-zT*flC*gl,(l-wT*)-IC*gZ)lt,
(iii)
[Sa(z,w) (~:),
if Ll is coisometric;
(~:) )!jel!l= [(I -zTflFfl +(l-zT*fICx'*gl>(l-wTfIFfz+(I-w1'*flG*g2ht. if Ll is unitary.
In this section we summarize some of the results from [DLSl).
17
Alpayet al. THEOREM 1.2.
Assume that
0'
and ® are Hilbert spaces and let eES°(B',®).
Then
That is, either these three numbers are infinite or one of them is finite and then they all are finite and equal.
If one of them is finite and equal to II:EINU{O}, say, then 13 admits the
following realizations. (a) e=eLl,on :b(e) for some isometric colligation 4 1= (.R\,O',®;U1), and then ind±.R:1~sq±(us); the isometric colligation 41 can be chosen closely innerconnected, in which case it is uniquely determined up to isomorphisms and ind±.R:1 = sq±(us). (b) e=e Ll2 on :b(e) for some coisometric colligation 4 2 = (.R: 2,O',®;U 2), and then coisometric colligation 42 can be chosen closely outerconnected,
ind±.R:2~sq±(ue);
the
in which case it is
uniquely determined up to isomorphisms and ind±.R:2 = sq±(ue). (c) e=e Ll on :b(e) for some unitary colligation 4= (.R:,O',®;U), and then
ind±.R:~sq±(Ss);
the unitary
colligation 4 can be chosen closely connected, in which case it is uniquely determined up to isomorphisms and ind±.R: = sq±(Ss). One of the key tools in the proof of Theorem 1.2 given in [DLS1] is formulated in the following lemma.
A Hilbert space version of it is given by de Branges and Shulman in [BS].
It
relates isometric colligations to unitary colligations. LEMMA 1.3.
Let 41 = (.R:1,O',®;U.) be a closely innerconnected isometric colligation, in which
and ® are Hilbert spaces and .R:1 is a Pontryagin space.
0'
Then there exists a closely connected
unitary colligation 4=(.R:,O',®;U) such that ind_.R:=ind_.R: b UIB'=V and eLl=eLl,on :b(eLl)n:b(eLl,). Sketch of the proof of Theorem 1.2.
(1) We first consider the case where sq_(us) is finite,
and we briefly describe the construction of the realization described in (a). linear space £ of finite sums ['zczf., where zE:b(e), fzEO' and
Cz
Consider the
is a symbol associated with
each zE:b(e) and provide £ with the (possibly degenerate, indefinite) inner product [[,. cJ.,[,w cwgw] = ['z ,)us(z,w)f.,gw) ]B" Define the linear operators To, Fo, Go and H via the formulas 1
Toc.f =z(czf-cof), GoE:J =~(e(Z)f -e(O)f),
Hf=e(O)f,
where Z # 0 and fEB'. Then To and Go are densely defined operators on £ with values in £ and ®, respectively, Fo:O' -. £, H:O' ~ ®,
is an isometric operator on a dense set and H+zGo(I-zT of 1Fo=e(z) on
0'.
Now we consider the
18
Alpayet aI.
quotient space of £ over its isotropic part and redefine the operators on this space in the usual way. Then completing the quotient space to a Pontryagin space and extending the operators by continuity to this completion we obtain a closely innerconnected isometric colligation with the desired properties. (2) If it is given that sq_(ue) is finite we apply the above construction to realization in terms of a closely innerconnected isometric colligation .Ill =
e to
obtain a
(st'!l~,8';Utl.
Then
This uniqueness property together with
the constructions indicated in steps (1) and (2) imply that ind_.ltl = ind_st'2 = ind_.lt. in (1.1) now follow directly from the equalities in Remark 1.1.
The equalities
This completes the sketch of
the proof. The following factorization theorem is an application of Theorem 1.2. A proof can be found in [KL).
Below we sketch the proof given in [DLSl).
To formulate it we recall the notion of a
Blaschke-Potapov product. For a e [) and 8 e [0,211") we define the holomorphic bijection bn ,8: D -+ D by bo ,8(Z) = (z_a)e i8 /(1_zQ). An operator B:ID-+L(8',8') is called a (finite) Blaschke-Potapov product on 8' of degree Kell'll if B can be written as a (finite) product of factors of the form (l-P)+b o ,8(Z)P for some aeD (a is called a zero of the product), 8e[O,211") and some projection P
on 8' (of finite rank), and l:rankP=K, where the sum is taken over the projections P appearing in the factors forming B. Note that such a product assumes unitary values on the boundary I of the open unit disc D. 'THEOREM
1.4. Assume that 8' and ~ are Hilbert spaces and let eeSo(8',~). If one of the numbers
sq_(ue), sq_(ue) and sq_(Se) is finite and equal to KeNu{O}, say, then 8 admits the strongly regular factorizations e(z) = BdzfledZ) =8R (z)B R (zf\ w~re
ze:b(e),
BR :D-+L(8',8'), BL:D-+L(~,~) are Blaschke-Potapov products of degree
and e R ,
eL:D-+L(8',~)
are holomorphic contraction operators.
a meromorhpic operator function on D with
K
K
with zeros in D\{ O}
In particular, e can be extended to
poles (counting multiplicities) in D\{ O}.
In the theorem strongly regular essentially means that the zero's of 8 1• (8 R ) and the projections appearing in the Blaschke-Potapov product BL (B R ) do not cancel any of the poles of Bi l (Bi/, respectively). For the precise definition we refer to [DLS1) , Section 7, but in the sequel the above indication of what it means should be sufficient.
Alpay et al.
19
Sketch of the proof of Theorem 1.4. Apply Theorem 1.2 and let L1 =
(.It,iY,~jT,F,G,H)
be a closely
connected unitary colligation whose characteristic function coincides with e. Then.lt is a Pontryagin space with ind_.It = /C. From the equality T"T +G'G = I and the fact that G maps the Pontryagin space .It into the Hilbert space
~
exists a /C-dimensional nonpositive subspace
n of .It which is invariant under
spectrum of the restriction of T to
n
it follows that T is a contraction.
Hence there
T and such that the
lies outside Dj see [IKL) or [DLSI).
This leads to a
decomposition of L1 as the product of two unitary colligations, one of them on the left- or right-hand side corresponding to the /C-dimensional invariant subspace
no,
whose characteristic
function is a Blaschke-Potapov product. This completes the sketch of the proof. To remove the restriction "Oe:b(e)" in Theorem 1.4 we use the following lemma.
Its proof
amounts to straightforward substitution and is therefore omitted. LEMMA
1.5. Let
eeS(iY,~),
where iY and
~
are Krein spaces.
Assume that zoe:b(e), denote the
mapping b_.."o:D+D by b so that b(z)=(z+zo)/(I+zzo), zeD, and define the operator function eoeS(iY,~) by eo(z) =e(b(z)), ze:b(eo)=b.."o(:b(e)).
Then:
(i)
eoeS°(iJ,~),
(ii)
(1-lzoI2)O"a(b(z),b(w)) = (I+wzo) O"ao(z,w) (I +zzo) 2
--
(iii)
(I-izol )O"t'j(b(z),b(iO)) = (l+wzo) O"t'jo(z,w)(1+zzo)
(itl)
(I - 1Zo 12)e(b(Ui) )-e(b(z))
(I
+wzo
and sq±(O"a) = sq±O"ao), and sq±(O"t'j) =sq±(O"t'jo)'
) eo(iii) -eo(Z)(1
b(iO)-b(z)
-) +zzo .
iO-z
If zoeRn:b(e), so that b(z)=b(ZT, then
Applying Lemma 1.5 to Theorems 1.2 and 1.4, we obtain the following result. CoROLLARY
1.6. Assume that iY and
~
are Hilbert spaces and let
(toith the same interpretation as in Theorem 1.2).
eeS(iY,~).
Then
If these numbers are finite and equal to
lCeNu{O}, say, then e admits the strongly regular factorizations
e(z) =BL(z)-ledz ) =eR(z)BR(z)-\
ze:b(e),
Wlhere BR:D+L(iY,iY), BL:D+L(~,~) are Blaschke-PotapOtl produ.cts of degree /C and e R, eL:D+L(iY,~) Gre holomorphic contraction operators. In particular, e can be extended to a meromorphic
operator function on D with /C poles (coonting multiplicities) in D.
20
Alpayet aI. 2.
POSITIVE SQUARES AND INJECTIVITY
For the main theorem in this section we use the following result.
A more general version
involving Schur products will be given at the end of this section. LEMMA 2.1.
Let ZHZ2"",Zn be n different points in D and let Q= (Qij) be a nonnegative nxn
matrix with diagonal elements Qii>O,
i=I,2, ... ,n.
Then the nxn matrix (Qij/(I-zizj )) is
positive.
Let P be the matrix (Qij/(I-zizj )).
Then P= r:_oOkQDook, where O=diag(zHz2, ... ,zn)' Hence P~O, and to show that P>O, it suffices to prove that R(P)={O}, where R(P)cCn is the null Proof.
space of P. Let u=(ui)eR(P). Then O=u*Pu= r:=o(Oooku)*QDooku, and, since each summand in the series is nonnegative, the vector QD."", = 0, k = 0,1,.... with complex coefficients the vector QP(O*)u=O.
It follows that for every polynomial P
Let ie{I,2, ... ,n} and let Pi be a polynomial
with the property that P i(zj)=6ij , the Kronecker delta. Then O=(QPi(O*)U)i=QiiUi, which implies that Ui=O, since, by assumption, Qii>O. It follows that "'=(Ui)=O, i.e., R(P)={O}. Note that in the proof of Lemma 2.1 we have used the Taylor expansion 1/(I-zw)= r:=dwz)n. A similar proof can be given based on the integral representation of 1/ (1- zw) given in the Introduction just above Theorem 0.2. THEOREM
(i)
2.2. Let 0' and
~
be Hilbert spaces and let 8eS(0',~).
If sq+(O'e) <00, then for each ze:b(8), with the exception of at most sq+(O'e) points in :b(8),
there is a positive constant e(z), such that 8(z)*8(z) ~ e(z)I. (ii)
If sq+(O'a) <00, then for each ze:b(8), with the exception of at most sq+(O'a) points in :b(8),
there is a positive constant 6(z), such that 8(z)8(z)*~6(z)I.
To prove (i) we let K=sq+(O'a), and we assume that there are K+l different points
Proof.
zje:b(8), i=I,2, ... ,K+l, for which there is no positive constant e, such that 8(zi)*8(zi)~eI. Then, for each n we can find elements x~eO' such that IIx~lIiJ=1 and 118(Zi)x~lIiJ<1/n. Define the Gram matrix Qn=((Qniij) of size (K+l)X(K+l) by (Qn)ij=[x~,xjliJ' (Qn)ii = 1.
Then Qn is nOImegative and
If necessary by going over to subsequences, we see that the limit Q=lim......,Qn exists
and is a nonnegative (K+l)x(K+l) matrix with diagonal entries Qii=1.
Now consider the
(K+1)X(K+l) matrix Pn=((Pn)ij) with
(Pn)ij = [O'e(zi,zj)x7,xjliJ = ((Qn)ij/(I-zizj )) - ([8(Zi) x7,8(zj) xjlQ!)/(I-zizj ) ). Then the limit lim......,Pn exists and equals the (K+l)x(K+l) matrix P=((Qij/(I-zizj )). On account of Lemma 2.1 the matrix P has precisely K+l positive eigenvalues. However, this is impossible, since, by assumption, for each n the approximating (K+l)x(K+l) matrix Pn has at most Part (ii) follows from (i) by replacing 8 by 9. This completes the proof. K positive eigenvalues. This contradiction proves (i).
Alpay et al. LEMMA 2.3.
21 Let!)' and ® be /(re'tn spaces and eES(15,®).
but finitely many zE:b(e) and put
rJi(z)=e(zf l •
Assume that e(z) is invertible for all
Then rJiES(®,15) and
17e(z,w) = -e(W)I7~(Z,W)e(z)*,
(i)
17fl(z, w) = -e(W)*l7w(Z,W)e(z),
(ii)
Sfl(Z,W) = -diag(e(w),e(wj*j*Sw(z,w)diag(e(z),e(z)*),
(iii)
sQ±(17fl) = sq+(17w), sq±(17e) = sq+(I7~), sq±(Sfl) = sq+(Sw).
The proof of this lemma is straightforward and therefore omitted. COROLLARY 2.4. Let!)' and ® be Hilbert spaces and let eES(15,®).
Then
(i) sq+(Se)<00 if and only if (ii) sq+(17e)<00 and sq+(17e) <00. If (i) and (ii) are valid, then sq+(17fl)=sq+(17e)=sq+(Se) and for each zE:b(e)n:b(e)*, with the exception of at most 2sq+(Se) points, e(z) is invertible. Proof.
Clearly, (i) implies (ii).
Now assume (ii). Combining parts (i) and (ii) of Theorem
2.2, we obtain that e(z) is invertible for all, but at most sq+(17e)+sq+(l7e), points z in :b(e); see, e.g., Lemma 2.5 in [An].
Hence we may apply Lemma 2.3.
statement in Corollary 1.6 with rJi(z) = e(zf l sq+(17e) = sq+(17e) = sq+(Se).
Using this lemma and the first
instead of e(z),
we obtain the equalities
They imply (i) and show that in the last statement of the corollary
the number of exceptional points is at most sq+(17e)+sq+(17e) = 2sq+(l7e). Using the same kind of arguments as in the proof of Corollary 2.4 we can prove the following result.
Recall that an operator T E L(15, ®) is called expansive if rT ~ I iJ;
biexpansive if both T and COROLLARY 2.5.
r
it is called
are expansive.
Let!)' and ® be Hilbert spaces and let e:ID~L(15,®) be a holomorphic mapping.
Then the following assertions are equivalent. (i)
e(z) is a biexpansion for all
(ii)
Both kernels 17e(z,w) and 17e(z,w), z,wED, are nonpositive.
ZED.
The remaining part of this section is devoted to a generalization of Lemma 2.1 to the Schur product of two nonnegative matrices.
It is not needed in the sequel.
Recall that the Schur
product of two nxn matrices P=(Pij) and Q=(Qij) is the nxn matrix P.Q=((P.Q)ij) with
(P.Q)ij = PijQij, i,j = 1,2, ... , n.
That is, P.Q is defined as the entry-wise product of P and Q.
For example: (1)
The matrix (Qij/(1-z i z j )) in Lemma 2.1 is the Schur product of the nxn matrix (1/(1-z i z j )) and Q.
(2)
If a=(a;), b=(bi)ECn (in the sequel considered as the space of nx1 vectors) P=aa* and
(3)
Q=bb*, then P.Q=cc*, where C=(Ci)ECn with ci=aibi, i=1,2, ... n. 1 0 0 If a = (~), b = c = (~), P= aa* + bb* and Q = aa*+cc*, then P and Q are nonnegative 3x3
U),
22
Alpayetal.
101 matrices with rank P = rank Q = 2 and P..Q = ( 0 1 0) is a positive matrix. 102
The following result concerns the decomposition of nonnegative matrices.
We give a proof
without recourse to the spectral decomposition theorem for Hermitian matrices. The method makes use of the nonnegativity of the matrix and is very much like the methods of Lagrange and Jacobi which apply to general Hermitian forms; see, e.g., Gantmacher [G), p. 339.
Let P be a nonnegative nxn matrix with rankP = r.
PROPOSITION 2.6.
Then there exist r
linearly independent vectors PieCn such that P=1::=IPiP}. Consider a block decomposition of P of the form P = ( ~
Proof.
Z),
where A is a nonnegative
matrix of size kxk, say. (We actually only need the case where k=I.) If xeR(A), the null space of A, and yeCn-k is arbitrary, then the nonnegativity of P and the Cauchy-Schwarz inequality imply that
It follows that B*x=O and this shows that R(A)cR(B*). Taking orthogonal complements we see that
R(B)cR(A), where R(A) denotes the range of A. Hence there exists an kx(n-k) matrix G such that B=AG. It is straightforward to verify that P can be written as
( A B) (I
O)(A 0 P= B* D = c* I 0 D-G*AG
)(10 G) (Ai)( G*Al Ai )* (0 1 = G*Al + 0
(For more details, see for instance [Dy), Lemma A.I.)
0)
D-G*AG .
To prove the proposition we start with
the block decomposition for P=(Pij ) in which A=PJJ • Then we obtain P=Plpt+
(~
2
D_G AG)' PI = (G1!!) eCn.
Note that PI is the zero vector if PJJ = o.
We repeat the same procedure to the nonnegative
(n-l)x(n-l) matrix D-c*AG. After n steps we have constructed vectors PieCn, i= 1,2, ... ,n, such that P = 1:~=1 PiP}.
Since the first i -1 entries of each Pi e en are zero, 1 ~ i ~ n, it is clear from
the construction that the nontrivial vectors among PI' P2, ... , Pn are linearly independent.
By
deleting the trivial vectors and reordering we obtain the decomposition P = 1::=1 PiP7 for some r~n,
in which Pl>P2, ... ,Pr are linearly independent. As
P~O,
we have that x€R(P) if and only if
x*Px=O. Since this last relation holds if and only if x*Pi=O, i= 1,2, ... ,r, it follows that dimR(P)=n-r, so necessarily r=rankP. This completes the proof. Proposition
2.6
implies Schur's lemma; see [D), p.9.
prove the desired generalization. results.
The proof of. this lemma can be used to
For the sake of completeness, we give the proofs of both
23
Alpayetal.
2.7. Let P and Q be two nonnegative nxn matrices.
THgOREM
Then:
(i)
(Schur's lemma) The Schur product P.Q is nonnegative.
(ii)
If P is positive, then P.Q is positive if and only if Q ii ¢ 0 for all i = 1, ... ,no
Proof We first prove (i). P = 1::=1 PiPl, where
Put rankP=r and rankQ=s. Then by Proposition 2.6
Q = 1:1=1 qjlJ'j,
Pw .. ,Pr are linearly independent
independent vectors in
en.
vectors
in
en and
qH ... ,q.
are
also
linearly
We denote the k - th entry of the vector Pi by (P;)k, so that
Pi=((P;)k)~=I' i=1,2, ... r, and we use a similar notation for each vector qj.
It follows that
P.Q = 1::=1 1:;=1 (PiP1)*(qjlJ'j) = 1::=1 1:1=1 vijV1j' where Vij is vector in
en and the k-th entry of
Vij is given by (Vij)k=(Pi)k(qj)k.
This shows
that P.Q is nonnegative. We now prove (ii). We use the same decompositions of the matrices P and Q as in the proof of part (i).
Since P is positive, we have that r=rankP=n.
nonnegative.
Note that, on account of (i), P.Q is
The "only if" statement in (ii) follows easily from the fact that all diagonal
elements of a positive (nonnegative) matrix are positive (nonnegative, respectively). the "if" statement, we suppose that Qii ¢ 0 and hence Qii> 0 for all i = 1, ... , n. suffices to show that P.Q has a trivial null space R(P.Q).
To prove
Since P.Q ~ 0, it
Let a= (ak)~=IER(P.Q).
Then
a*P.Qa = 0, and it follows from P.Q = 1:7=1 1:1=1 VijVlj that 0= a*vij = 1:~=lak(vij)k= 1:~=1 (ak(qj)k)(Pj)k,
The linear
independence of the vectors
i = 1,2, ... ,n, j = 1,2, . .. ,s.
PHP2, ... ,Pn
implies that
ak(qjh,=O,
j=1,2, ... ,s,
k=1,2, ... ,n, and from 1:J=ll(qj)kI 2 =Qkk>0 it follows that to each k, 1~k~n, there corresponds an
.index j., 1 ~j. ~ s, such that (qj.)k ¢
o.
Hence for each k we have that ak = 0, i.e., a is the zero
vector and R(P.Q) = {O}. This completes the proof. Lemma 2.1 is a special case of Theorem 2.7 (ii): take P=(1/(1-z j zj )). Example (3) given above shows that if the Schur product of two nonnegative matrices is positive then it is not true that . at least one of these matrices is positive also. 3.
ApPLICATION OF THE POTAPOV-GINZBURG TRANSFORM
In this section we prove Theorems 0.1 and 0.2.
The basic idea behind the proofs is a
reduction of the KreIn space situation to the Hilbert space situation. obtained by applying the Potapov-Ginzburg transform.
This reduction is
Under various different names this
transform has been used in, for example, [AGl,2), [DR), [Dy), [IKL).
We first briefly describe
this transform and introduce the convenient notation used in [DR), Section 1.
Alpayetal.
24
Let !J be a KreIn space and let !J = !J+(!)!J_ be a fixed fundamental decomposition of !J.
The
operator Jfj=P+-P_, where P± is the orthogonal projection on !J onto !J±, is called the fundamental synunetry associated with the fundamental decomposition.
Note that J~ = Ifj.
The linear space !J
provided with the inner product [f,g]lfJI = [Jfjf,g]fj, f,ge!J, is a Hilbert space and will be denoted by I!JI. The definition of I!JI depends on the fundamental decomposition, I!JI =!J+(!) I!J-I and I!J-I is the anti-space of !J-.
For the Krein space @) we also fix a fundamental decomposition
@)=@)+(!)@)_ and we denote the orthogonal projection on @) onto @)± by Q±. Then
J~=Q+-Q_
is the
fundamental synunetry corresponding to the fundamental decomposition by means of which the Hilbert space I@)I is defined. By definition TeL(!J,@)) if and only if TeL( 1m, I@)I).
If TeL(!J,@)), then by
T"
we denote the
adjoint of T with respect to the KreIn space inner products on !J and @), and by
T" we denote the
adjoint of T with respect to the Hilbert space inner products on I!J I and I@)I.
It is easy to see
that
T", T" eL(@),!J)
and that
T" =JfjTxJ~,
T" =Jfj1"J~.
If TeL(!J,@)), then with respect to the fundamental decompositions of!J and @) we often write T in
following operator matrix form
where, for example, T22 = Q11fj_ eL(!J_,@)_). If T22 is invertible then the operator
is
also
invertible
and
S=(Q+T+P_)(P++Q1f1.
the
Potapov - Ginzburg
transformation
S
of T
is
the
operator
Clearly, SeL(!J+(!)@)_,@)+(!)!J_) and S has the operator matrix form
It is straightforward to verify that if we apply the Potapov-Ginzburg transform to S we get the operator T back.
For proofs of these facts we refer to [DR], where a complete survey of the
Potapov-Ginzburg transform in connection with contractions is presented. Below we consider a function 6leS(!J,@)) and we use the same notation as above. For example, 8 21 stands for the operator function 6l21 (Z) = Q_61(z) Ifj+ defined for z in a deleted neighborhood of
o.
The following theorem is an analog and a small extension of [DR], Theorem 1.3.4.
We recall
that !J and @) are KreIn spaces with fundamental decompositions !J=!J+(!)!J- and @)=@)+(!)@)_ and corresponding fundamental synunetries J fj and
J~.
AJpay et aI.
25
THEOREM 3.1. :b=:b*c:b(t9).
(i)
E(z)
Let tgeS(O',®) and assume that t922 (Z) = Q_t9(z) IlL is invertible for z in an open set
Then E defined by
= (Q+t9(z) +P_)(P+ +Q_t9(z)rl
is a well-defined and holumorphic function on :b with values in the space L(O'+E9®_,®+E9O'_) and satisfies the follO'UJing identities (ii)
E(z( = (P +t9(z)* +Q_)(Q+ +p_t9(z)*r\
(iii)
t9(z) = (Q+E(z) +Q_)(P+ +P_E(z))-\
(iv)
t9(z)* = (P+E(z( +P_)(Q++Q_E(z)xrl.
Moreover, we have (a)
J -t9(w)*t9(z) =JiJ(P++Q_t9(w))x(J -E(w(E(z))(P++Q_t9(z)),
(b)
J -t9(Ui)t9(z)* = J,,(Q+ +P_t9(Ui)*((J -E(Ui)E(z)x)(Q+ +P_t9(z)*),
(c)
t9(z)* -t9(w)* = JiJ(P++Q_t9(w)((E(z( -E(w()(Q++P_t9(z)*),
(d)
t9(Ui) -t9(z) = J,,((Q+ +P_t9(Ui)*((E(Ui) -E(z))(P+ +Q_t9(z)).
It is clear that the function E is well-defined and holomorphic on:b.
The relations
(ii)-(iv) can be verified in the same manner as the corresponding results in [DR].
To prove (a)
Proof.
we consider its right-hand side and substitute for E(z) and E(w) the expression in (i).
We
obtain (P + +Q_t9(w) )x(1_ E(w(E(z))(P+ +Q_t9(z)) = = (P + +Q_t9(w)((P dQ_t9(z)) - (Q+t9(w) +P-l"(Q+t9(z)+P_) = (P + +J~(w)*JII£2_)(P+ +Q_t9(z)) - (J'ijt9(w)*JII£2+ +P _)(Q+t9(z) +P_) = P ++J~(w)*JII£2_t9(z) -P_-JiJt9(w)*JII£2+t9(Z) = JiJ(J -t9(w)*t9(z)),
which is equivalent to (a).
Similarly, one can obtain (b) by substituting for E(z) and E(w) in
Its right-hand side the expression in (ii).
To show (c) we consider its right-hand side and
substitute for E(w) the expression in (i) with z replaced by w and for E(z) the expression in (ii) with
z replaced by z. We obtain (P + +Q_t9(w) ((E(z)x - E(w)x)(Q+ +P_t9(z)*) = = (P++Q_t9(w)((P+t9(z)* +Q_)-(Q+t9(w)+pJ(Q++P_t9(Z)*) = (P + +J~(w)*J~_)(P +t9(Z)* +Q_) - (J~(w)*J~+ +P-HQ+ +P_t9(z)*) =P +t9(z)* +J~(w)*J~_ -J~(w)*J~+ -P_t9(z)* = J iJ (t9(z)* -t9(w)*),
which is equivalent to (c).
Finally, (d) can be shown by substituting in its right-hand side
for E(z) the expression in (i) and for E(w) the expression in (ii) with z replaced by Ui. This completes the proof of the theorem. Combining the identities (a )-( d) of Theorem 3.1 we get a useful relation between the kernels
26
Alpayet al.
associated with the operator functions 8 and E. CoROLLARY 3.2.
Under the conditions of Theorem 3.1 the following kernel identities are valid
for all z,we:b. (i)
O'e(z,w) = Jfj(P + +Q_6l(w) (O'l;(Z, w) (P + +Q_8(z».
(ii)
O'e(z,w) = JQI)(Q++P_8(iii)*)" O'.t(z,w) (Q+ +P_8(2)*).
(iii)
Se(z, w) = diag (Jfj,JQI)(diag (P ++Q_8(w),Q++P_8(iii)*)"Sl;(Z,W) (diag (P ++Q_8(z),Q++P_8(Z)*).
In order to use Theorem 3.1 and Corollary 3.2, we must make sure that 8 22 is invertible on some open set :bc:b(8). We first make the following observation. LEMMA 3.3. If A and B are Hermitian matrices and
A~B,
then the number of negative (positive)
eigenvalues of A is larger (less) than or equal to the number of negative (positive) eigenvalues of B, where the eigenvalues are counted according to their multiplicities.
Lemma 3.3 is an immediate consequence of the minimax characterization of the eigenvalues of a Hermitian matrix, which implies that if
A~B,
then
Aj(A)~Aj(B),
j=I,2, ... , where the eigenvalues
and A;(B)~Aj(B)j for A simple and direct proof of the
Aj(A) and Aj(B) of A and B are ordered such that if i<j, then
details see [G], Anhang, and, in particular, p. 621, Satz 6.
Ai(A)~Aj(A)
more global statements in the lemma here can be given by showing that if E_(A) (E_(B» stands for the linear span of the eigenspaces of A (B) corresponding to all negative eigenvalues of A (B, respectively) and PA denotes the orthogonal projection onto E_(A), then the restriction PAIE_(B) to E_(B) is injective on E_(B) and hence dimE_(B) ~ dimE_(A). This implies the statement about the number of negative eigenvalues of A and Bj the other statement follows from the first one applied to the operators -A and -B.
THEOREM 3.4. Let 8eS(tl,l9) and set 8 22(z) =Q_8(z)lfj_. (i)
If SQ_(O'e)
there is a positive constant e(z), such that 8 22 (z(822 (Z) ~e(z)I. (ii)
If sq_(O'e) < 00, then for each ze:b(8), with the exception of at most SQ_(O'e) points in :b(8),
there is a positive constant 6(z), such that 822(Z)822(Z(~6(z)I. Proof.
The follOwing chain of (in-)equalities is valid.
All kernels here are defined on the
domain :b(8) anc;l in brackets we indicate on what inner product space they act. sq_(O'a) ~SQJP-O'elfjJ
=SQ-( -P-O'elfjJ = SQ+(P-O'alfjJ ~SQ+(O'~)
(on the KreIn space tl) (on the anti-Hilbert space tl-) (on the Hilbert space Itl-I) (on the Hilbert space Itl-I) (on the Hilbert space Itl-I).
27
Alpay et al. The last inequality follows from the identity P_O"e(z,w)ltL = I -e 22 (W) xe 22 (z) +e 12(w) xed z ) l-zw l-zw
O"e22 (z,w) +e 12 (W) xe12 (Z), l-zw
z,wE:b(e),
the nonnegativity of the kernel edw)xed z )
(on the Hilbert space
10'-1)
l-zw
and Lemma 3.3.
Hence the kernel O"e22 (z,w) has at most sqjO"e) positive squares on IfLI. If we replace in the above argument
(i) now follows from Theorem 2.2(i).
e
bye,
Part
0' by ® and
P
by Q, we obtain that the kernel _ ( )_I-e 22 (w)ed z( O"e22 z,w , l-zw
z,wE:b(e),
has at most sq_(O"e) positive squares on the Hilbert space I®-I. Part (ii) now follows from Theorem 2.2(ii). This completes the proof. COROLLARY 3.5. Let eES(O',®) and assume that sq_(O"e)
is
invertible
for
each
zE:b(e)n:b(e)
with
the
Then the function
exception
of
at
most
sq_(O"e)+sq_(O"e) points.
We now come to the proofs of the main theorems of the paper. Proof of Theorem
Assume (ii).
0.1.
Clearly, the inequality in (i) implies the inequalities in (ii).
Then by Corollary 3.5 the operator e 22 (z) is invertible for each zE:b(e)n:b(e)
except for at most sq_(O"e)+sq_(O"e) points.
Hence the conditions of Theorem 3.1 are satisfied,
and the operator function L'(z) in (i) of Theorem 3.1 is well defined.
Corollary 3.2 implies the
equalities
Here the kernels on the left-hand side are considered as operators on Hilbert spaces. to Corollary
1.6 their numbers
sq_(O"e)=sq_(O"e)=sq_(Se).
of negative
squares
are
equal.
It
now
According
follows
that
Hence, in particular, (i) is valid and the last statement in Theorem
0.1 holds true. This completes the proof. Proof of Theorem 0.2.
0.1. 6 22 (Z)
The implications (i)*(ii) and (i)*(iii) follow inunediately from Theorem
If (it) (or (iii)) is valid then, on account of Theorem 3.4(i) (or (it), respectively),
is invertible for all but at most
K.
points in :b(e).
Again we may apply the
Potapov-Ginzburg transform to conclude, as in the proof of Theorem 0.1, that (i) is valid.
If
E(z) is the transformation of e(z) then, by Corollary 1.6, L'(z) can be extended to a meromorphic
operator function on D with at most
K.
poles.
The lower right corner E Z2 (z) of E(z) is a square
28
Alpay et aI.
matrix function of size indJJ = ind_® and, since outside a discrete subset of O. that
e
detL'22(z)~0
on 0, it is invertible for all z
Applying the inverse Potapov-Ginzburg transform to L' we find
has the property mentioned in the last statement of the theorem.
This completes the
proof. REFERENCES
[A)
D. Alpay, "Some Krein spaces of analytic functions and an inverse scattering problem", Michigan Journal of Math., 34 (1987), 349-359. [ADl) D. Alpay, H. Dym, "Hilbert spaces of analytic functions, inverse scattering and operator models I", Integral Equations Operator Theory, 7 (1984), 589-641. [AD2) D. Alpay, H. Dym, "Hilbert spaces of analytic functions, inverse scattering and operator models II", Integral Equations Operator Theory, 8 (1985), 145-180. [AD3) D. Alpay, H. Dym, "On applications of reproducing kernel spaces to the Schur algorithm and rational J unitary factorization", Operator Theory: Adv. Appl., 18 (1986), 89-159. [AGl) D.Z. Arov, L.Z. Grossman, "Scattering matrices in the theory of dilations of isometric operators", Dokl. Akad. Nauk SSSR, 270 (1983), 17-20, (Russian) (English translation: SOY. Math. Dokl., 27 (1983), 518-522). [AG2) D.Z. Arov, L.Z. Grossman, "Scattering matrices in the theory of unitary extensions of isometric operators", manuscript. [An) T. Ando, De Branges spaces and analytic operator functions, Lecture Notes, Hokkaido University, Sapporo, 1990. [Azl) T. Ya. Azizov, "On the theory of extensions of isometric and symmetric operators in spaces with an indefinite metric", Preprint Voronesh University, 1982; deposited paper no. 3420-82 (Russian). [Az2) T.Ya. Azizov, "Extensions of J-isometric and J-symmetric operators", Funktsional. Anal. i Prilozhen, 18 (1984), 57-58 (Russian) (English translation: Functional Anal. Appl., 18 (1984), 46-48). [Bl) L. de Branges, "Krein spaces of analytic functions", J. Functional Analysis, 81 (1988), 219-259. [B2) L. de Branges, "Complementation in Krein spaces", Trans. Amer. Math. Soc., 305 (1988), 277-291. [B3) L. de Branges, Square summable power series, manuscript. [BC) J.A. Ball, N. Cohen, "De Branges-Rovnyak operator models and systems theory: a survey", Operator Theory: Adv. Appl., 50 (1991), 93-136. [BR) L. de Branges, J. Rovnyak, Square summable power series, Holt, Rinehart and Winston, New York, 1966. [BS) L. de Branges, L.A. Shulman, ''Perturbations of unitary transformations", J. Math. Anal. Appl., 23 (1968), 294-326. [CDIB) B. Curgus, A. Dijksma, H. Langer, H.S.V. de Snoo, "Characteristic functions of unitary colligations and of bounded operators in Krein spaces", Operator Theory: Adv. Appl., 41 (1989), 125-152. [D) W.F. Donoghue, Monotone matrix functions and analytic continuation, Springer-Verlag, Berlin-Heidelberg-New York, 1974. [DIBI) A. Dijksma, H. Langer, H.S.V. de Snoo, "Characteristic functions of unitary operator colligations in 11 K-spaces", Operator Theory: Adv. Appl., 19 (1986), 125-194. [D1B2) A. Dijksma, H. Langer, H.S.V. de Snoo, ''Unitary colligations in II K-spaces, characteristic functions and Straus extensions", Pacific J. Math., 125 (1986), 347-362. [D1B3) A. Dijksma, H. Langer, H.S.V. de Snoo, "Unitary colligations in Krein spaces and their role in the extension theory of isometries and symmetric linear relations in Hilbert spaces", Functional Analysis II, Proceedings Dubrovnik 1985, Lecture Notes in Mathematics, 1242 (1987), 1-42. [DR) M.A. Dritschel, J. Rovnyak, Extension theorems for contractions on Krein spaces, Operator Theory: Adv. Appl., 47 (1990), 221-305.
Alpayetal. [Dy)
[G) [IKL) [KL)
[M) [Mc) [SF) [Y)
29
Dym, J contractive matrix functions, reproducing kernel Hilbert spaces and interpolation, Regional conference series in mathematics, 71, Am~r. Math. Soc., Providence, R.I., 1989. F.R. Gantmacher, Matrizentheorie, 2nd ed., Nauka, Moscow, 1966 (Russian) (German translation: VEB Deutscher Verlag der Wissenschaften, Berlin, 1986). loS. Iohvidov, M.G. Krein, H. Langer, Introduction to the spectral theory of operators in spaces with an indefinite metric, Reihe: Mathematical Research 9, Akademie-Verlag, Berlin, 1982. M.G. Krein, H. Langer, "tIber die verallgemeinerten Resolventen und die charakteristische Funktion eines isometrischen Operators im Raume ll,.", Hilbert Space Operators and Operator Algebras (Proc. Int. Conf., Tihany, 1970) Colloquia Math. Soc. Janos Bolyai, no. 5, North-Holland, Amsterdam (1972), 353-399. S. Marcantognini, ''Unitary colligations of operators in Krein spaces", Integral Equations Operator Theory, 13 (1990), 701-727. B.W. McEnnis, "Purely contractive analytic functions and characteristic functions of non-contractions", Acta. Sci. Math. (Szeged), 41 (1979), 161-172. B. Sz.-Nagy, C. Foias, Harmonic analysis of operators on Hilbert space, North-Holland Publishing Company, Amsterdam-London, 1970. A. Yang, A construction of KreIn spaces of analytic functions, Dissertation, Purdue University, 1990. H.
D. A!.PAY DEPARTMENT OF MATHEMATICS BEN-GURION UNIVERSITY OF THE NEGEV POSTBOX 653 84105 BEER-SHEVA isRAEL
MSC: Primary 47B50, Secondary 47A48
A. DIJKSMA, J. VAN DER PLOEG, H.S.V. DE SNOO DEPARTMENT OF MATHEMATICS UNIVERSITY OF GRONINGEN POSTBOX 800 9700 AV GRONINGEN THE NETHERLANDS
30
Operator Theory: Advances and Applications, Vol. 59 @ 1992 Birkhiiuser Verlag Basel
ON REPRODUCING KERNEL SPACES, THE SCHUR ALGORITHM, AND INTERPOLATION IN A GENERAL CLASS OF DOMAINS
Daniel Alpay and Harry Dym*
This paper develops the theory of reproducing kernel Pontryagin spaces with reproducing kernels A..,(A) = X(A)JX(W)* / p..,(A) based on a k x m matrix valued function X(A), a signature matrix J and a denominator of the general form a(A)a(w)* - b(A)b(w)*. This both unifies and generalizes earlier studies of such kernels wherein the denominator was taken to be either 1 - AW* or -27Ti(A - w*). A Schur-like algorithm is then interpreted in terms of a recursive orthogonal direct sum decomposition of such spaces. Finally, these spaces, in conjunction with a corresponding class of K(8) spaces which were introduced earlier (in [AD4j), are used to solve a general one-sided interpolation problem in a fairly general class of domains.
CONTENTS
2. 3.
INTRODUCTION PRELIMIN ARIES 8(X) SPACES
4. 5. 6. 7. 8.
RECURSIVE EXTRACTIONS AND THE SCHUR ALGORITHM 'HAS) SPACES LINEAR FRACTIONAL TRANSFORMATIONS ONE SIDED INTERPOLATION REFERENCES
1.
*H. Dym would like to thank Renee and Jay Weiss for endowing the chair which supports his research.
31
Alpay and Dym
1. INTRODUCTION
In this paper we shall study reproducing kernel Pontryagin spaces of m x 1 vector valued meromorphic functions with reproducing kernels of the form
A (>.) = X(>.)JX(w)* w pw(>') , where X is a k x m matrix valued function, J is an m X m signature matrix (i.e., J and J J* = 1m), the denominator Pw(>') is of the form
(1.1)
= J*
Pw(>') = a(>.)a(w}* - b(>.)b(w)* ,
(1.2)
and it is further assumed that: I.
II.
a(>.) and b(>.) are analytic in some open nonempty connected subset 0 of CV. The sets
0+ = {w EO: Pw(w) > O}
0_ = {w EO: PIAI(w) < O}
and
are both nonempty. Because of the presumed connectedness of 0, it follows further (see [AD4] for details) that: III.
The set
00
= {w EO:
= O} o.
PIAI(w)
contains at least one point I" such that pp(>') ~
Any function PIAI(>') of the form (1.2) which satisfies I and II (and hence III) will be said to belong to 'Do. Reproducing kernel Pontryagin spaces with reproducing kernels of the form (1.1) were extensively studied in [AD3] for the special choices PIAI(>') = 1 - >.w* and PIAI(>') = -27ri(>. - w*). Both of these belong to 'Do with 0 = CV:
= 1, b(>.) = >., 0+ = ID and 00 = ']['. w*) is of the form (1.2) with a(>.) = y'i(l- i>.), b(>.) = y'i(l + i>.),
1 - >.w* is of the form (1.2) with a(>.)
-27ri(>. 0+ = CV+ and 00 = JR.
In this paper we shall extend some of the results reported in [AD3] to this new more general framework of kernels with denominators in 'Do and shall also solve a general one-sided interpolation problem in this setting. Many kernels can be expressed in the general form (1.1); examples and references will be furnished throughout the text. In addition to these, which focus on AIAI(>') as a reproducing kernel, the form (1.1) shows up as a bivariate generating function in the study of structured Hermitian matrices; see the recent survey by Lev-Ari [LA] and the references cited therein. In particular, Lev-Ari and Kailath [LAK] seem to have been the first to study "denominators" PIAI(>') of the special form (1.2). They showed that Hermitian matrices with bivariate generating functions of the form (1.1) can be factored efficiently whenever p",(>') is of the special form (1.2). The present analysis gives a geometric interpretation of the algorithm presented in [LAK] in terms of a direct sum orthogonal decomposition of the underlying reproducing Pontryagin spaces.
Alpay and Dym
32
As we already noted in [ADl], the important kernel
Kt./(A) = J - 6(A)J6(w)* Pt./(A)
(1.3)
can also be expressed in the form (1.1), but with respect to the signature matrix
. [J0
J =
0]
-J
'
by choosing X=[Im 6]. For the most part, however, we shall take J equal to
and shall accordingly write
X(A) = [A(A) B(A)] with components A E ([!kxp and B E ([!kxq, both of which are presumed to be meromorphic in n+. Then (1.1) can be reexpressed as
At./(A) = A(A)A(w)* _ B(A)B(w)* , Pt./(A) Pt./(A) which serves to exhibit At./(A) as the difference of two positive kernels on n+ (since 1/p",(A) is a positive kernel on n+, as is shown in the next section). Therefore, by a result of L. Schwartz [Sch], there exists at least one (and possibly many) reproducing kernel Krein space with At./(A) as its reproducing kernel. However, if the kernel is restricted to have only finitely many negative squares (the definition of this and a number of related notions will be provided in Section 2), then there exists a unique reproducing kernel Pontryagin space with At./(A) as its reproducing kernel. This too was established first by Schwartz, and independently, but later, by Sorojonen [So] (and still independently, but even later, by the present authors in [AD3]). If At./(A) has zero negative squares, i.e., if At./(A) is a positive kernel, then the (unique) associated reproducing kernel Pontryagin space is a Hilbert space, and the existence and uniqueness of a reproducing kernel Hilbert space with At./(A) as its reproducing kernel also follows from the earlier work of Aronszajn [Ar]. Throughout this paper we shall let 8(X) [resp. .qe)] denote the unique reproducing kernel Pontryagin (or Hilbert) space associated with a kernel of the form (1.1) [resp. (1.3)]. The reproducing kernel Hilbert spaces 8(X) and K(9), but with p",(A) restricted to be equal to either 1- AW* or -27ri(A -w*), originate in the work of de Branges, partially in collaboration with Rovnyak; see [dBl], [dBR], [dB3], the references cited therein, and also Ball [Bal]. Such reproducing kernel Hilbert spaces were applied to inverse scattering and operator models in [AD 1] and [AD2], to interpolation in [Dl] and
Alpay and Dym
33
[D2], to the study of certain families of matrix orthogonal polynomials in [D3] and [D4], and to the Schur algorithm and factorization in [AD3]; the latter also extends a number of basic structural theorems from the setting of Hilbert spaces to Pontryagin spaces. In [AD4] and [AD5], the theory of K(8) spaces was extended beyond the two special choices of p mentioned above, to the case of general p E Do. The parts of that extension which come into play in the present analysis (as well as some other prerequisites) are reviewed in Section 2. In this paper we shall carry out an analogous extension for the spaces 8(X). This begins in Section 3. Recursive reductions and a Schur type algorithm are presented in Section 4. Section 5 treats the special case in which Aw{A) is positive and of the special form Aw(A) = {Ip - S(A)S(w)*}jPw(A). Section 6 deals with linear fractional transformations, and finally, in Section 7, we apply the theory developed to that point to solve a general one-sided interpolation problem in f!+. The basic strategy for solving the interpolation problem in f!+ is much the same as for the classical choices of the disc or the halfplane except that now we seek interpolants S for which the operator Ms of multiplication by S on an appropriately defined analogue of the vector Hardy space of class 2 is contractive: IIMsll :5 1. Although this implies that S is contractive, the converse is not generally true; see the examples in Section 5. Moreover, f!+ need not be connected. Interpolation problems in nonconnected domains have also been considered by Abrahamse [Ab], but both the methods and results seem to be quite different. Finally, we wish to mention that there appear to be a number of points of contact between the interpolation problem studied in this paper and the interpolation problem described by Nudelman [N] in his lecture at the Sapporo Workshop. However, we cannot make precise comparisons because we have not yet seen a written version. The notation is fairly standard: The symbols rn. and ([; denote the real and complex numbers, respectively; ID = {A E ([; : IAI < 1}, 11' = {A E ([; : IAI = 1}, IE = {A E ([; : IAI > 1} and ([;+ [resp. ([;_] stands for the open upper [resp. lower] half plane. ([;pxq denotes the set of p x q matrices with complex entries and ([;P is short for ([;Px 1. A * will denote the adjoint of a matrix with respect to the standard inner product, and the usual complex conjugate if A is just a number.
2. PRELIMINARIES To begin with, it is perhaps well to recall that a vector space V over the complex numbers which is endowed with an indefinite inner product [ , ] is said to be a Krein space if there exist a pair of subspaces V+ and V_ of V such that
(1)
V+ endowed with [ , ] and V_ endowed with -[ ,
(2)
V+ n V_ = {OJ.
(3)
V+ and V_ are orthogonal with respect to [ ,
I and
I are Hilbert
spaces.
their sum is equal to V.
V is said to be a Pontryagin space if at least one of the spaces V+, V_ is finite dimensional. In this paper, we shall always presume that V_ is finite dimensional. In this instance, the dimension of V_is referred to as the index of V.
Alpayand Dym
34
A Pontryagin space P of m x 1 vector valued meromorphic functions defined on an open nonempty subset 6 of cr:, with common domain of analyticity 6', is said to be a reproducing kernel Pontryagin space if there exists an m x m matrix valued function Lw(.~) on 6' x 6' such that for every choice of W E 6', v E cr: m and I E P;
(1)
Lwv E P, and
(2)
[I, Lwv]p = v* I(w).
The matrix function Lw(,x) is referred to as the reproducing kernel; there is only one such. Moreover, for every choice of a and j3 in 6'. The kernel Lw(,x) (or for that matter any Hermitian kernel) is said to have negative squares in 6' if (1) for any choice of points WI, . .. ,W n in 6' and vectors V}, •• . , Vn in cr: m the n x n matrix with ij entry equal to vi LWj (wdvj has at most II negative eigenvalues and, (2) there is a choice of points WI, . .. ,Wk and vectors VI, • •. ,Vk for which the indicated matrix has exactly II negative eigenvalues; it should perhaps be emphasized here that n is also allowed to vary. In a reproducing kernel Pontryagin space, the number of negative squares of the reproducing kernel is equal to the index of the space. II
For additional information on Krein spaces and Pontryagin spaces, the monographs of Bognar [Bo], lohvidov, Krein and Langer [IKL], and Azizov and lohvidov [AI] are suggested. Next, it is convenient to summarize some facts from [AD4] about the class 'Do which was introduced in Section 1 and on some associated reproducing kernel spaces. First, it is important to note that the definition of the class 'Do depends only upon p and not upon the particular choice of functions a and b in the decomposition (1.2). In particular, if Pw(,x) can also be expressed in terms of a second pair of functions c(,x) and d(A): if
PW(,x) = c(,x)c(w)* - d(,x)d(w)* , then there exists a Jll unitary matrix M such that [c(,x) d(,x)]
= [a(,x)
b(,x)]M
for every ,x E n;see Lemma 5.1 of [AD4]. We have already remarked that the functions Pw(,x) -211"i(A - w*) belong to 'Do. So does the less familiar choice
=1-
,xw* and Pw(,x)
PW(,x) = -271"i(,x - w*)(1 - ,xw*) .
=
(2.1)
The latter is of the form (1.2) with
a(,x)
= Ji"p + i(,x2 + I)}
Moreover, in this case,
and b(,x)
= Ji"p -
i(,x2
+ I)}
.
(2.2)
35
Alpay and Dym
is not connected.
S(A)
Now if p E Do. with decomposition (1.2), then a(A) f:. 0 for A E Q+ and strictly contractive in Q+. Therefore, the kernel
= b(A)/a(A) is
kw(A)
1
1
~
=( ') = ( \ L pwA aA)
1
s(A) s(w)
1=0
*1
1 aw)*
-(-
is positive on Q+: for every positive integer n, and every choice of points Q+ and constants CI,' .. , Cn in a:: ,
WI, ... ,W n
in
n
L
cjkw;(Wj)Ci ~ 0 .
i,j=1
Thus, by one of the theorems alluded to in the introduction, there f'xists a unique reproducing kernel Hilbert space, with reproducing kernel kw(A) = l/(h... (>..). We shall refer to this space as Hp and shall designate its inner product by ( )f1p' Recall that this means that, for every choice of W E Q+ and f E H p, (1) 1/ pw belongs to H p, and (2) (f, 1/ Pw) f1p = f(w). The space Hp plays the same role in the present setting as the classical Hardy spaces H2(ID) for the disc and H2( a::+) for the open upper half plane. Indeed, it is identical to the former [resp. the latter] when Pw(A) = 1- AW* [resp. Pw(A) = -27l"i(A-
w*)]. More generally,
H;:'
will denote the space of m x 1 vector valued functions
f with coordinates /; and 9i, i
9
= 1, ... ,m,
in Hp and inner product m
L(fi,9i)f/p i=1
From now on, we shall indicate the inner product on the left by (f, g) f1p (i.e., we drop the superscript m), in order to keep the notation simple. For allY m x Tn sigllature matrix J, the symbol Hp,J will denote the space H',;' endowed with the indefinite inner product
The space H;:' is a reproducing kernel Hilbert space with reproducing kernel Kw(A) = 1m/ Pw(A), whereas Hp,J is a reproducing kernel Krein space with reproducing kernel Kw(.~) = J/Pw(A).
36
Alpay and Oym
Because 1/ Pw(>.) is jointly analyticfor A and w* in out in more detail in [AD4]) that
n+, it follows (as is spelled
a
k 1 1 'Pw,k = -k'. uW ~ *kPw
belongs to H p for every integer k ;::: 0 and that
for every
I
E H p and every w E
n+.
We shall refer to the sequence 'Pw,O,· .. ,'Pw,n-l
n+.
as an elementary chain of length n based on the point w E
ft, ... , In
More generally, by a chain of length n in of the m X n matrix valued function
H;:'
we shall mean the columns
F("\) = Vq,w,n(..\) , wherein V is a constant m x n matrix with nonzero first column and
!
'PW'O(A)
41",n( A)
~
[
'Pw,n-l (..\)
1 (2.4)
o
'Pw,o(..\)
is the n x n upper triangular Toeplitz based on 'Pw,o(..\), ... , 'Pw,n-l("\) as indicated just above. It is important to note that
(2.5) where Aw and Bw are the n x n upper triangular Toeplitz operators given by the formulas
o
o
r1 *
and
Bw
!l' ,
(2.6)
130
00
where a(j)(w)
OJ = --.,}.
and
13j
b(j)(w) = --.,- . }.
These chains are the proper analogue in the present setting of the chains of rational functions considered in [A03] and [02]. They reduce to the latter in the classical cases, i.e., when Pw(A) = 1 - AW* or Pw(A) = -21ri(A - w*).
37
Alpay and Dym
In the classical cases, every finite dimensional space of vector valued meromorphic functions which is invariant under the resolvent operators (RoJ)()..) = f()..) - f(o) )..-0
(2.7)
(for every a in the common domain of analyticity) is made up of such chains. An analogous fact holds for general p E Vn, but now the invariance is with respect to the pair of operators a()..)f()..) - a(o)f(o) {r( a, b; a )f}()..) = a( a )b()..) _ b( o)a( )..)
(2.8)
b()..)f()..) - b(o)f(o) {r(b,a;o)f}()..) = b(o)a()..) _ a(o)b()..) ,
(2.9)
and
see [AD5] for details. Just as in the classical cases, a non degenerate finite dimensional subspace of Hp,J with a basis made up of chains is a reproducing kernel Pontryagin space with a
reproducing kernel of the form (1.3). More precisely, we have: THEOREM 2.1. Let p E Vn and let A E ([;nxn, B E ([;tlxn and V E ([;mxn be a given set of constant matrices such that
(1)
det{a(",)A - b(",)B} =I- 0 for some point", E no, and
(!)
the columns of
F()")
= V{a()")A -
b()")B}-1
(2.10)
are linearly independent (as analytic vector valued functions of)..) in n~, the domain of analyticity of F in n+. Then, for any invertible n X n Hermitian matrix P, the space
:F = span {columns of F()")} , endowed with the indefinite inner product
(2.11)
is an n dimensional reproducing kernel Pontryagin space with reproducing kernel K..,()..) = F(),,)P- I F(w}* .
The reproducing kernel can be expressed in the form
K ()..) = J - 9()")J8(w)*
'"
p",()..)
(2.12)
Alpay and Dym
38
for some choice of m x m signature matrix J and m x m matrix valued function 6(..\) which is analytic in n~ if and only if P is a solution of the equation A * P A - B* P B = V* JV .
(2.13)
Moreover, in this instance, 6 is uniquely specified by the formula (2.14)
with JJ as in (1), up to a J unitary constant factor on the right. PROOF. This is Theorem 4.1 of [AD4]. An infinite dimensional version of Theorem 2.1 is established in [AD5]. Therein, the matrix identity (2.13) is replaced by an operator identity in terms of the operators r( a, b, a) and r( b, a, a). In the sequel we shall need two other versions of Theorem 2.1: Theorems 5.2 and 5.3 of [AD4], respectively. They focus on the special choice of A = Aw and B = Bw. THEOREM 2.2. Let JJ and F be as in Theorem 2.1, but with A = Aw and B = Bw for some point wE n+. Then the columns II, ... '/n of F belong to H;: and the n x n matrix P with ij entry
is the one and only solution of the matrix equation (2.15)
THEOREM 2.3. Let p E Do., JJ E no and w E n+ be such that p,..(w) =f. 0 and suppose that the n x n Hermitian matrix P is an invertible solution of (2.15) for some m X m signature matrix J and some m X n matrix V of rank m with nonzero first column. Then the columns II, ... ,fn of
F(>.) = V{a(..\)Aw - b(..\)Bw}-1 are linearly independent (as vector valued functions on n~) and the space:F based on the span of II, ... , fn equipped with the indefinite inner product
e
(for every choice of and TJ in a: n ) is a K(6) space. Moreover, 6 is analytic in n+ and is uniquely specified by formula (2.14), up to a constant J unitary factor on the right. the class in 0'+.
From now on we shall say that the m x m matrix valued function 6 belongs to if it is meromorphic in n+ and the kernel (1.3) has v negative squares
'P~(n+)
Alpay and Oym
39
3. 8(X) SPACES is an m
X
Throughout this section we shall continue to assume that p E Vn and that J m signature matrix.
A k x m matrix valued function X will be termed (S1+, J,p)v admissible if it is meromorphic in S1+ and the kernel
Aw(-\) = X(-\)JX(w)* Pw(,\)
(3.1)
has v negative squares for -\ and w in S1~, the domain of analyticity of X in S1+. Every such (S1+, J, p)v admissible X generates a unique reproducing kernel Pontryagin space of index v with reproducing kernel Aw(-\) given by (3.1). When v = 0, X will be termed (S1+, J, p) admissible. In this case, the corresponding reproducing kernel Pontryagin space is·a Hilbert space. We shall refer to this space as SeX) and shall discuss some of its important properties on general grounds, in the first subsection, which is devoted to preliminaries. A second description of SeX) spaces in terms of operator ranges is presented in the second and final subsection. The spaces SeX) will play an important role in the study of the reproducing kernel space structure underlying the Schur algorithm which is carried out in the next section. It is interesting to note that the kernel K S -\
_
w( ) -
Ip - S(-\)S(w)* 1 - -\w· [ S(-\*)* _ S(w)* -\ - w"
S(-\) - S~w*) -\-w Iq - S(-\*)* S(w*) 1 - -\w"
1 ,
based on the p x q matrix valued Schur function S can be expressed in the form (3.1) by choosing -\S(-\) S(-\) ] Ip X(-\) = y'2; 271' [ Up ,\l , S(,\ *)* -\S(,\ *)* Iq q
~
-~ql
0 0 J (-i) 0 Iq and Pw(-\) as in (2.1). This kernel occurs extensively in the theory of operator models; see e.g., [Ba2j, [OLSj and [dBSj.
[-i'
Ip 0 0 0
3.1. Preliminaries. THEOREM 3.1. If the k x k matrix valued function Aw(-\) defined by (9.1) ha", v negative ",quare", in S1~, the domain of analyticity of X in S1+, then there exi",~ a unique reproducing kernel Pontryagin "'pace P with index v of k x 1 vector valued function$ which are analytic in S1+. Moreover, Aw(-\) u the reproducing kernel ofP and {Awv: w E S1+
and
v E CC k }
Alpay and Dym
40
is dense in P.
PROOF. See e.g., Theorem 6.4 of [AD3].
•
Schwartz [Sch] and independently (though later) Sorojonen [So] were the first to establish a 1:1 correspondence between reproducing kernel Pontryagin spaces of index v and kernels with v negative squares. We shall, as we have already noted, refer to the reproducing kernel Pontryagin space P with reproducing kernel given by (3.1), whose existence and uniqueness is established in Theorem 3.1, as SeX). THEOREM 3.2. If X is a k x m matrix valued function in S1+ which is (S1+, J, p)v admissible and if f belongs to the corresponding reproducing kernel Pontryagin space SeX) and W E S1~, then, for j = 0,1, ... and every choice of v E a:: k ,
belongs to SeX) and (')
If, A,J
vectors
PROOF. in
VI, ... , Vn
(3.2)
vjB(X)
By definition there exists a set of points wI. . .. , Wn in S1~ and such that the n x n Hermitian matrix P with ij entry
a:: k
has v negative eigenvalues A}, ... , Av. Let Ul, •• corresponding to these eigenvalues and let
• , Uv
be an orthonormal set of eigenvectors
j=l,oo.,II.
Then, for any choice of constants
not all of which are zero,
C}, ••• , Cv
v
=
LAilcil2 <
O.
i=1
Thus the corresponding Gram matrix Q with ij entry
qii = [fi, hlB(X)
,
i,j = 1, ... ,v,
is negative definite and the span N of the columns ft, ... , fv of F = dimensional strictly negative subspace of SeX) with reproducing kernel Nw(A)
= F(A)Q-l F(w)*
,
A,w E S1~.
[ft ... fvl is a
v
Alpay and Dym
41
Consequently, 'H = 8(X)BN,
the orthogonal complement of N in 8(X), is a reproducing kernel Hilbert space with reproducing kernel Hw(>') = Aw('\) - Nw('\) , '\,w E n~ . Clearly Hw{'\) is jointly analytic in n~ x n~ since Aw('\) is (by its very definition) and N w{'\) is (since it involves only finite linear combinations of vector valued functions which are analytic in n~). Therefore, since'H is a Hilbert space,
H~j>v
E 'H
and
[g,H~PV]8(X) = v*g(i)(w)
for every choice of w E n~, v E ([!k and 9 E 'Hj see e.g., [AD4] for more information, if need be. Similar considerations apply to N since it is a Hilbert space with respect to -[ , ]8(X), or, even more directly by explicit computation:
and hence, since every hEN can be expressed as h = Fu for some u E ([!",
[h, N~PV]8(X) = [Fu, FQ-I F(i)(w)*V]8(X) = v* F(i)(w)Q-IQu = v*h(i)(w) . Thus
AY)(,\)v = H~j>(,\)v + N~P('\)v
clearly belongs to 8(X) for every choice of w E n~ and v E ([!k. Moreover, as every E 8(X) admits a decomposition of the form
!
!=g+h with 9 E 'H and hEN it follows readily that
(') (') (') [!,Ad V]8(X) = [g,H,] V]8(X) + [h,N,] V]8(X) = v*/i)(w)
+ v*h(i)(w)
= v* !(i)(w) , as claimed.
•
In order to minimize the introduction of extra notation, the last theorem has been formulated in the specific Pontryagin space 8(X) which is of interest in this paper. A glance at the proof, however, reveals that it holds for arbitrary Pontryagin spaces with
42
Alpay and Dym
kernels AC4I('x) which are jointly analytic in ,X and w· for ('x,w) E the decomposition
~ x~.
In particular
which continues to hold in this more general setting, exhibits AC4I (.x) as the difference of two positive kernels both of which are jointly analytic in ,X and w· for ('x, w) E ~ x ~. The conclusions of Theorem 3.2 remain valid for those points a E no at which AC4I('x) is jointly analytic in ,X and w· for ,X and w in a neighborhood of o. This is because, if W},W2, ••• is a sequence of points in which tends to a, then
n+
(k) v, H C4In (k)] [H C4In v stays bounded as n
8(X)
(k)] = [(k) AC4In v, A C4In v 8(X)
[(k) (k)] N C4In v, N C4In v
8(X)
T00. Thus at least a subsequence of the elements H~:)v tends weakly
to a limit which can be identified as Hik) v since weak convergence implies pointwise convergence in a reproducing kernel Hilbert space. Thus Hik)v belongs to B(X), as does
and hence also
A~)v
It remains to verify (3.2) for w
= Hik)v
= a, but
+ Nik )v .
that is a straightforward evaluation of limits.
3.2. B(X) Spaces
In this subsection we give an alternative description of B(X) under the supplementary hypothesis that the multiplication operator
Mx: ! __ X! is a bounded operator from
H': into H;.
Then
X is automatically analytic in n+ and
r=MxJMx'
(3.3)
H;
is a bounded selfadjoint operator from into itself. The construction, which is adapted from [AI], remains valid even if the kernel AC4I('x) defined in (3.1) is not constrained to have a finite number of negative squares. However, in this instance the space B(X) will be a reproducing kernel Krein space, i.e., it will admit an orthogonal direct sum decomposition
where B+ is a Hilbert space with respect to the underlying indefinite inner product [ , ]8(X) and B_ is a Hilbert space with respect to -[ , ]8(X) and both B+ and B_ are presumed to be infinite dimensional. Moreover, in contrast to kernels ·with a finite number of negative squares, there may now be many different reproducing kernel Krein spaces with the same reproducing kernel. Examples of this sort were first given by Schwartz
Alpay and Dym
43
[Sch). For another example see [A2), and for other constructions of reproducing kernel Krein spaces, see [A3), [dB4), [dB5) and [Y). Let
Rr = {rg: 9 E H;} and let Rr denote the closure of Rr with respect to the metric induced by the inner product (3.4) (r f, rg}r = (r*r)~ f, g) Hp . It is readily checked that Rr is a pre-Hilbert space:
(r f, r f) r
=0
rf
if and only if
=0,
and hence that Rr is a Hilbert space. Next let C(X) = Rr endowed with the indefinite inner product (3.5) [rf,rg)r = (rf,9}H p which is first defined on Rr and then extended to Rr by limits. LEMMA 3.1. If wE f!+ and v E
Mx~ Pw
PROOF. U
E
Let kw(A)
=
= X(w)*~ Pw
.
(3.6)
l/Pw(A). Then, for every choice of a E f!+ and
= {v*X(w)ko:(w)u}* = u*kw(a)X(w)*v .
On the other hand, by direct calculation, the left hand side of the last equality is equal to u*(MXkw)(a)v. This does the trick since both u and a are arbitrary.
•
THEOREM 3.3. C(X) is a reproducing kernel Krein space (of k x 1 vector valued analytic functions in f!+) with reproducing kernel
Aw(A)
=
X(>.)JX(w)* Pw(A)
(3.7)
for every choice of wand A in f!+.
H;
PROOF. Since r is a bounded selfadjoint operator on the Hilbert space it admits a spectral decomposition: r = J~oo tdEt with finite upper and lower limits. Let
r-
=
1:00 tdEt
and
r+ =
100
tdEt .
44
Alpay and Dym
Then
r _ and r + are bounded selfadjoint operators on
H:,
It now follows readily that
'R.r
=
'Rr + [+I'R.r _
is a Krein space since the indicated sum decomposition is both direct and orthogonal with respect to the indefinite inner product [ , Ir given in (3.5), and 'R.r ± is a Hilbert space with respect to ±[ , Ir. It remains to show that
(1)
Awv E C(X) and
(2)
[f, Awvlr = v* f(w)
for every choice of v E a:;k, wE fl+ and
f
E C(X). The identification
= MxJX(w)*.3:.... , Pw
which is immediate from Lemma 3.1, serves to establish (1). Suppose next that f = rg for some g E
H:.
Then
=v*f(w). This establishes (2) for f E limiting argument. •
'R.r.
The same conclusions may be obtained for
f
E
'R.r
by a
THEOREM 3.4. If X is a k x m matrix valued function which is (fl+, J,p)v admissible and if also the multiplication operator M X is bounded on H;', then
8(X) = C(X) .
PROOF. Under the given assumptions, both 8(X) and C(X) are reproducing kernel Pontryagin spaces with the same reproducing kernel. Therefore, by the results of Schwartz [Schl and Sorojonen [Sol cited earlier, or Theorem 3.1, 8(X) = C(X). •
n+
LEMMA 3.2. Let X be a k x m matrix valued function which is analytic in such that Mx is a bounded linear operator from H;J' to H:. Then
(3.8)
Alpay and Dym
45
for j = 0,1, ... and every choice of v E
a:: k
and wE
n+.
PROOF. It is convenient to let .
D} Then, for every choice of u E
oi = --. Ow*}
a:: m
v
and
f=-· Pw
and a E n+,
= Di {v* X(W)u}*
Po«w) = u*DiX(w)*_v_
Pw(o)
= u* Di(M'Xf)(o) ,
where the passage from line 2 to line 3 is just a special case of (3.2) applied to the Hilbert Therefore, space
H:.
as claimed. and
r
•
COROLLARY 1. If X,W and v are as in the preceding lemma and if Aw(.X) are as in (9.1) and (9.9), respectively, then oiv
r--.ow*} Pw
=
{)i
v
--.row*} Pw
oi = --.Awv. ow*}
(3.9)
COROLLARY 2. If X, wand v are as in the preceding lemma and if fi
= J M'X'Pw,iv
,
j = 0,1, ...
,
then li()..) = J
i X(i-s)(w)* L (._ )1 'Pw,s()..)v s=o J s.
(3.10)
and
* Jx(n-l)(w)*v] [/0'" In-I] = [ JX(w) v ... ct»w n (n -I)!
'
.
(3.11)
46
Alpay and Dym
PROOF. Let ni =
ai jaw*i. fi
Then, by Lemmas 3.2 and 3.1,
1 niJ M xV'w,ov * = ]!
=
~ni JX(w)*.!.
J.
Pw
which, by Leibnitz's rule, is readily seen to be equal to the right hand side of (3.10). Formula (3.11) is immediate from (3.10) and the definition (2.4) of ~w,n. • Suitably specialized versions of formulas (3.8)-(3.10) playa useful role in the study of certain classes of matrix polynomials; see Section 11 of [D1] and Section 6 of
[D4]. LEMMA 3.3. If X is as in Lemma 9.2 and if f = J MxV'O/,iu and 9 = J MxV'p,iV for some choice of n, f3 in n+ and u, v in (Vk, then (3.12)
[Mxf,Mxg]8(X) = {Jf,g)H p .
PROOF. This is a straightforward calculation based on the definitions:
= (rV'O/,i u , V'p,i V) Hp = {MxJMxV'O/,iu,V'p,iV)Hp = (Jf,g)H p .
•
Formula (3.12) exhibits Mx as an isometry from the span M of fi = JMxV'O/,ju, j = 0, ... , n in H; into 8(X). This is an important ingredient in the verification of the orthogonal direct sum decomposition
(3.13)
8(X) = 8(X8)[+]XK:(8)
which holds when M = K:(8). In fact M = K:(9) when M is a nondegenerate subspace of Hp,J, as follows from Theorems 2.2 and 2.l.
THEOREM 3.5. Let X = [F G] be a k x m matrix valued meromorphic function on n+ with components F('\) E (Vkxp and G(.\) E (Vkxq such that Mx is a bounded operator from H';: into H;. Then X is analytic on n+ and the following are equivalent:
(1) X is (n+,J,p) admissible.
(2) (9)
r
= MFM} - MaMa is positive semidefinite on
There is a p Ma=MFMs.
X
H;.
q matnz valued analytic function S on
n+ such that IIMslI
~
1 and
47
Alpay and Dym
PROOF. X is analytic on
n+ because v k Mx- E Hp a
for every choice of v E
<em.
The equivalence of (1) and (2) is an easy consequence of the evaluation
* (wi)Vj = [Vj ViAwj r-, PWj
r Vi- ]
PWi 8(X)
Vj vi ) = (r - , - H PWj PWi P
and the fact that finite sums of the form
~Awj Vj
are dense in 8(X).
Suppose next that (2) holds. Then, by a (slight adaptation - to cover the case p", q of a) theorem of Rosenblum [Ro], there exists an operator Q from H3 to H: such that: where, in the last item Ms denotes the (isometric) operator of multiplication by s = b/a on regardless of the size of the positive integer r. Thus, by Theorem 3.3 of [AD4], Q = Ms for some p x q matrix valued function S which is analytic on n+, as needed to complete the proof that (2) => (3). The converse is selfevident. •
H;,
A more leisurely exposition of the proof of this theorem for Pw(A) = 1 - Aw* may be found e.g., in [ADD].
4. RECURSIVE EXTRACTIONS AND THE SCHUR ALGORITHM In this section we study decompositions of the form (3.13) of the reproducing kernel Pontryagin space 8(X) based on a k x m (n+, J,p)v admissible matrix valued function X; the existence and uniqueness of these spaces is established in Theorem 3.l. Such decompositions originate in the work of de Branges [dB2, Theorem 34], [dB3], and de Branges and Rovnyak [dBR] for the case v = 0 (which means that 8(X) is a Hilbert space) and Pw(A) = -21ri(A - w*) for a number of different classes of X and S. Decompositions of the form (3.13) for finite v (i.e., when 8(X) is a reproducing kernel Pontryagin space) and the two cases Pw(A) = I - Aw* and Pw(A) = -21ri(A - w*) were considered in [AD3]; such decompositions in the Krein space setting were studied in [AI] and, for Hilbert spaces of pairs, in [A4]. If B(X) is a nonzero Hilbert space, then it is always possible to find a one dimensional Hilbert space K: (81) such that X K:( 8 t} is isometrically included inside 8 (X). This leads to the decomposition
8(X) = 8(X9t} EB XK:(9t} .
48
Alpayand Dym
Then, if 8(Xet) is nonzero, there is a one-dimensional Hilbert space K(e2) such that X8tK(82) sits isometrically inside 8(Xed, and so forth. This leads to the supplementary sequence of decompositions
8(Xf>t)
= 8(Xele2) EB XetK(e2)
8(Xete2) = 8(Xete2ea)EBXf>te2K(ea)
which can be continued as long as the current space 8(X8t ... en) is nonzero. In this decomposition, the i are "elementary sections" with poles (and directions) which are allowed to vary with j.
e
The classical Schur algorithm corresponds such a sequence of decompositions for the special case in which Pw( A) = 1- AW*, X = [1 S) with S a scalar analytic contractive function in ]I) and all the ei have their poles at infinity. For additional discussion of the Schur algorithm from this point of view and of decompositions of the sort considered above when 8(X) is a reproducing kernel Pontryagin space, see [AD3). In particular, in this setting it is not always possible to choose the K(ei) to be one-dimensional, but, as shown in Theorem 7.2 of [AD3) for the two special choices of p considered there, it is possible to choose decompositions in which the K(ei) are Pontryagin spaces of dimension less than or equal to two. The same conclusions hold for p E Vn also as will be shown later in the section.
THEOREM 4.1. Let X be a k x m matrix valued function which is (f!+, J,p)v admissible and let 8(X) be the (unique) associated reproducing kernel Pontryagin space with reproducing kernel given by (9.1). Let 0' E f!~, the domain of analyticity of X in f!+, let M denote the span of the functions
*
1
ai-t
*v
I
fi = JMX'POI..i-I V = (. -1)1 8w*i- 1 JX(w) , J. Pw W=OI. j
= 1, ... ,n,
(4.1)
endowed with the indefinite inner product
and suppose that the n x n matrix P
= (Pii)
is invertible. Then:
(1)
M is a K(e) space.
(It)
The operator Mx of multiplication by X is an isometry from K(f» into 8(X).
(9)
xe is (f!+, J,p)1'
admissible, where J.I. = v - the number of negative eigenvalues of
P.
(4) 8(X) admits the orthogonal direct sum decomposition 8(X) = 8(Xe)[+JXK:(e) . PROOF. Let
(4.2)
Alpay and Dym
49
denote the m x n matrix with columns JXU-l)(a)*v Vj
=
(j _ I)!
j
'
= 1, .. . ,n
.
Then, by Leibnitz's rule, it is readily checked that
F=[h,···,jn]
= VclIa,n' By (2.4), this can be reexpressed as F(>.) = V{a(>')Aa - b(>.)Ba}-1 ,
where Aa and Ba are as in (2.6). Therefore, by Theorems 2.2 and 2.3, M is a K(8) space. Next, since X Ij
= (.J
1
(j -1)
)' Aa
-1 .
v
in terms of the notation introduced in Section 3, it follows from Theorem 3.2 that X Ii E
8(X) and 1 1 a i - 1 ai-I v*X(>.)JX(w)*vl [Xlj, XIi]8(X) = (i -I)! (j - I)! a>.i-l aw*j-l Pw(A) A=w=a .
(4.3)
But the last evaluation is equal to
as follows by writing j-l k~)
Ij
=L
t=o
-, t. Vj-l-t
with kw(>') = 1/Pw(>') and applying Theorem 3.2 to H~. This completes the proof of
(2). The proofs of (3) and (4) are much the same as the proofs of the corresponding assertions in Theorem 6.13 of [AD3] and are therefore omitted. •
If n = 1, then the matrix P in the last theorem is invertible if and only if X(a)*v is not J neutral. In this case, the 8 which intervenes in the extraction can be expressed in the form 8(>')
= Im + {b a (>') -
l}u(u* Ju)-lu* J ,
where u = JX(a)*v and
bereA) =
s(>.) - sea) 1 - s(A)s(a)*
Alpay and Dyhl
50
with s(..\) = b(..\)/a(..\)j see (2.24) of [AD4J, and hence
v* X(a)S(a) = 0 . Thus it is possible to extract the elementary Blaschke-Potapov factor
from the left of XS to obtain
which is analytic at a and is (Q+,J,p),. admissible, where p. = v ifu* Ju if u· Ju < O.
> 0 and p. =
v-I
THEOREM 4.2. Let X be a k x m matrix valued function which i3 (Q+,J,p)v admi33ible and 3upp03e that 8(X) =I- {O} and Q+ i3 connected. Then X(..\)JX(,,\)* ¢. 0 in nt., the domain of analyticity of X in Q+. any
PROOF. Suppose to the contrary that X(..\)JX(,,\)* == 0 in there exists a h > 0 such that the power series
wEnt.,
Qt..
Then, for
00
X(A) =
L Xs(..\ -
w)S
s=O with k x m matrix coefficients converges, and 00
L
Xs(A _w)sJ(..\* _w*)tx; = 0
s,t=O for 1..\ -
wi < h.
Therefore 00
L
c s+t e i {s-t)6 XsJX; = 0,
s,t=O for 0:5 c < hand 0:5 (J < 271". But this in turn implies that XsJX; = 0 for s,t = 0,1, ... , and hence that X(a)JX({3)* = 0 for la - wi < h and 1{3 - wi < h. Since n+ is connected, this propagates to all of n+ and forces 8(X) = {O}, which contradicts the given hypotheses. Thus X(..\)JX(,,\)* ¢. 0 in as claimed. •
nt.,
COROLLARY 1. If, in the 3etting of Theorem 4.1, n+ i3 connected, then there exi3u a point a E n+ and a vector v E (CAl 3uch that v* X(a)JX(a)*v =I- O. COROLLARY 2. If, in the 3etting of Theorem 4.1, n+ i3 connected, then the 3et of poinu in nt. at which the extraction procedure of Theorem 4.1 can be iterated arbitrarily often (up to the dimemion of 8(X») with one dimen3ional K:(8) 3pace3 i3 deme in n+.
51
Alpay and Dym
If f!+ is not connected, then it is easy to exhibit nonzero 8(X) spaces for which X(,x)JX(,x)* = 0 for every point ,x E f!+. For example, if f!+ has two connected components: f!1 and f!2, let
X(,x) = [a(,x)Kj
and
b(A)Kj] ,
. _ [JpP
J-
o
0]
-Jpp
,x E f!j ,
for
.
Then, for ,x E f!j and we f!i, X(,x)JX(w)* = Pw(,x)KjJppK;
-
Thus X(,x)J X(,x)* space of index p.
{
0 Pw(,x)Ip
if if
i=j ifj·
= 0 for every point ,x E f!+, while 8(X) is a 2p dimensional Pontryagin
THEOREM 4.3. Let X be a k x m matrix valued function which is (f!+, J, p)v admissible such that 8(X) f {OJ and yet X(a)*v is J neutraljor every choice oja E f!~ and v E (I; k, then there exist a pair oj points 0', {3 in f!~ and vectors v, W in (l;k s'IJ.ch that
(1) w*X({3)JX(a)*v
f O.
(£) The two dimensional space M
= span {JX(a)*v POt
, JX({3)*w} P/3
endowed with the J inner product in H;;' will be a x:(e) space. (S) The space 8(X) admits the direct orthogonal sum decomposition 8(X) = 8(Xe)[+]Xx;ce) .
(4) xe is (f!+,J,p)v-1 admissible. PROOF. The proof is easily adapted from the proof of Theorem 7.2 in [AD3] .
•
There is also a nice formula for the e which intervenes in the statement of the last theorem: upon setting 'lJ.l = JX(a)*v, 'lJ.2 = JX({3)*w and
52
Alpay and Dym
we can write
SeA) - s(f3) } ) ( {S(A) - sea) } SeA) = ( 1m + { 1 _ s(A)s(a)* - 1 W12 1m + 1 _ S(A)S(f3)* - 1
W21
)
•
(4.4)
This the counterpart of formula (7.5) of [AD3] in the present more general setting; for more infonnation on elementary factors in this setting, see [AD4]. The reader is invited to check for himself that
J - 8(A)J8(w)* = F(A) Pw(A)
[0,* ,]
-I
0
F( )* w,
where with
A- [a(a) 0
0]* ,
a(f3)
b(a) B = [ 0
0]* ,
b(f3)
and 'Y = UiJu2/p(3(a). The formula
Pw(A)POt(f3)_l {S(A)-S(f3)}{ s(w)-s(a)}* POt(A)Pw(f3) - - 1- s(A)s(a)* 1 - s{w)s(f3)* '
(4.5)
which is the counterpart of (7.3) of [AD3], plays an important role in this verification. The matrix valued function
CIA\ ... c2v-IA\2V-I]
1
with c; =
(~) 2
is (n+,J,p)v admissible with respect to Pw(A) = 1 - AW* and
J = J v+1,v. The corresponding space SeX) is a 2v dimensional Pontryagin space (of polynomials) of index v with reproducing kernel Aw(.X) = (1 - AW*)2v-I. It does not isometrically include a one dimensional K:(8) space such that X8 is (n+, P, J)v-I admissible, since X(A)JX(A)* > 0 for every point A E n+ = ID. This serves to illustrate the need for the two dimensional K:(8) sections of Theorem 4.3. We remark that Theorem 4.1 can be extended to include spaces M in which the chain I;, j = 1, ... , n, is based on a point a E no such that Aw (A) is jointly analytic in A and w* for (A, w) in a neighborhood of the point (a, a) E no x no. In this neighborhood Aw(A) admits a power series expansion (Xl
Aw(A) =
L i,;=O
Ai;(A - a)i(w* - a*);
Alpay and Dym
53
with the k x k matrix coefficients Aij. Now if
v* Aoov P = [
v*AO,n-l V
: V*An-l,OV
...
1
v* An-:l,n-l v
and if Aa and Ba are defined as in (2.6), and
v =
[JX(a)*v", Jx(n-l)(a)*v] (n-1)! '
then A~P Aa - B~P Ba = V* JV .
(4.6)
Formula (4.6) may be verified by differentiating
{a(A)a(w)* - b(A)b(w)*}Aw(A) = X(A)JX(W)* i times with respect to A, j times with respect to w* for i, j = 0, ... , n - 1 and then evaluating both sides with A = w = a. Therefore, by Theorem 2.3, the span M of the columns of F(A) = V{a(A)Aa - b(A)Ba}-1
endowed with the indefinite inner product
is a K:(E» space, whenever the hypothesis of Theorem 2.3 are satisfied. It is important to hear in mind that the indefinite inner product M is now defined in terms of derivatives of Aw(A) and not in terms of evaluations inside Hp which are no longer meaningful since the columns of F (which are just the Ij of (4.1)) do not belong to H;J" when a E no. Nevertheless formula (4.3) is still valid (as follows from the remarks which follow the proof of Theorem 3.2) and serves to justify the assertion that Mx maps K:(E» isometrically into 8(X) in this case also. Recall that a subspace M of an indefinite inner product space is said to be nondegenerate if zero is the only element therein which is orthogonal to all of M. It is readily checked that if M is finite dimensional with basis II, ... , In, then M is nondegenerate if and only if the corresponding Gram matrix is invertible.
THEOREM 4.4. Let P be a reproducing kernel Pontryagin space of k x 1 vector valued functions defined on a set 6. with reproducing kernel Lw{A). Suppose that M = span{Lau}, . .. , Laun} is a nonderenerate .,.,,,b,,pace of P for some choice of a E 6. and Ul," ., Un in a:: k , let [Ul ..... un] denote the k x n matrix with. columm U}, . . . . Un. Th.en:
.N = M[.l and let U =
Alpay and Dym
54
(1)
The matrix U* L OI ( a)U is invertible.
(~)
The sum decomposition P=M[+j...v is direct as well as orthogonal.
(9)
Both the spaces M and...v are reproducing kernel Pontryagin spaces with reproducing kernels (4.7) and (4.8)
respectively. PROOF. The matrix U* LOI(a)U is the Gram matrix of the indicated basis for M. It is invertible because M is nondegenerate. The fact that M is nondegenerate further guarantees that M = {O} and hence that assertion (2) holds.
n...v
Next, it is easily checked that L~(oX), as specified in formula (4.7), is a reproducing kernel for M and hence that M is a reproducing kernel Pontryagin space. Finally, since Lwu - L~u belongs to...v for every choice of w E ~ and u E a:;k and
(J,Lwu - L~uj"p = [f,Lwuj"p = u* few) for every f E ...v, it follows that ...v is also a reproducing kernel Pontryagin space with reproducing kernel L~(oX). • THEOREM 4.5. If, in the setting of Theorem
4.4, P = 8(X) and
Aw(oX) = X(oX)JX(w)* Pw(.A) for some choice of P E Vn and k x m matrix valued function X which is (n+, J, P)II admissible, and if a E n+ (the domain of analyticity of X in n+), then there exists an m x m matrix valued function 8 E p:;(n+) for some finite v such that
(1) M = XK(8). (!) ...v = 8(X8).
(9) L~(oX)
=X(oX) { J-e~:)(~)(w)*} X(w)*.
(4) A~(oX)
= X(oX)8(oX)J8(w)* X(w)* / Pw(oX).
PROOF. To begin with, let
v
= JX(a)*U
and
F(oX) = V POI(oX)-1 .
Then, upon setting A = a(a)* In
and
B
= 6(01)* In
,
55
Alpay and Dym
F can be expressed in the form
F()")
= V{a()")A -
b()")B}-1 ,
which is amenable to the analysis in Section 4 of [AD4J. The latter is partially reviewed in Section 2. In particular, hypotheses (1) and (2) of Theorem 2.1 (above) are clearly met: (1) holds for any /l E no for which la(/l)1 = Ib(/l)1 i- 0 since 0 rf. no, whereas (2) holds because M (which equals the span of the columns of X F) is nondegenerate by assumption. Thus since V*JV P:=--
Po-(o)
is a Hermitian invertible solution of the matrix equation A *P A - B* P B = V* JV ,
it follows from Theorem 2.1 that the span F of the columns of F endowed with the indefinite inner product [Fu, FVJF
= v* Pu
is a K(8) space. This proves (1) and further implies that F(),,)P-1 F(w)
=
J - 8()")J8(w)*
Pw()..) Thus AM()..) = X()..)V {v* JV w
Po-()..)
Po-( 0)
}-l
V*X(w)*
Po-(w)
= X()")F()..)p-1 F(w)* X(w)*
,
which proves (3). The remaining two assertions follow easily from the first two.
•
We remark that if the matrix U which appears in the statement of Theorem 4.4 is invertible, then (4.9) and
(4.10) Conclusion (4) of the last theorem exhibits the fact that (whether U is invertible or not) A~()..) has the same form as Aw()..). Fast algorithms for matrix inversion are based upon this important property. Lev-Ari and Kailath [LAKJ showed that if a kernel Aw()..) is of the form Aw()..) = X()")JX(w)*
Pw()..) for some Pw()..) with Pw()..)* = p.x(w), then the right hand side of (4.10) will be ofthe same form if and only if Pw()..) admits a representation of the form (1.2). The present analysis
56
Alpay and Dym
gives the geometric picture in terms of the reproducing kernel spaces which underlie the purely algebraic methods used in [LAK]. We complete this section with a generalization of Theorem 3.5. THEOREM 4.6. Let X = [C D] be a k x m matriz l1alued function which il
(0+,1, p)" admillible and for which Mx iI a bounded operator from H;:a into H:. Then there eziltl a p X q matriz l1alued meromorphic function 8 on 0+ luch that (1) [Ip - S] iI (O+,J,p)" admillible, and
(£) D = -C8. PROOF. IT v = 0, then the assertion is immediate from Theorem 3.5. IT v > 0, then, by repeated applications of either Theorem 4.1 or 4.3, whichever is applicable, there exists an m X m matrix valued function 6 E 1'j(O+) which is analytic in 0+ such that X 6 is (0+, J, p) admissible and the multiplication operator Me is bounded on H;:a. The last assertion follows from Theorem 6.1 and the formulas for 6 which are provided in and just after the proofs of Theorems 4.1 and 4.3, respectively. Thus, the multiplication operator Mxe is also bounded on H;:a and so, by Theorem 3.5, there exists a p x q matrix valued analytic function 8 0 on 0+ with IIMso II ~ 1 such that
Therefore,
D(821 8 0
+ 622) =
-C(61180
+ 612) ,
which in tum implies that D=-C8 with The indicated inverse exists in 0+ except for at most a countable set of isolated points because det(62180 + 622) is analytic and not identically equal to zero in 0+. Indeed, since 6 is both analytic and J unitary at any point I' E 00 at which la(JJ)1 = Ib(JJ)1 #:. 0, it follows by standard arguments that 671621 is strictly contractive at I' and so too in a little disc centered at 1'. This does the trick, since every such disc has a nonempty intersection with 0+ (otherwise la(..\)/b(..\) 1 ~ 1 in some such disc with equality at the center; this forces b(..\) = ca(..\) , first throughout the disc by the maximum modulus principle, and then throughout all of since it is connected) and 8 0 is contractive in 0+.
°
Now, let F = [II··· fn] be an m X n matrix valued function whose columns form a basis for X:(6), let Q denote the invertible n x n Hermitian matrix with ij entry
and finally, let Y = IIp - S)
and G
= 611 -
S621 .
57
Alpay and Dym
Then it follows readily from the decomposition Y(A)JY(W)* = Y(A) J - 8(A)J8(w)* Y(w)* p",(A) p",(A) = Y(A)F(A)Q-l F(w)*Y(w)*
+ Y(A) 8(A)J8(w)* X(w)* p",(A)
+ G(A) Ip - S;~~l~o(W)* G(w)*
that the difference between the kernel on the left and the first kernel on the right is a positive kernel. Therefore, for any set of points aI, ... , at in the domain of analyticity of S in 0+ and any set of vectors 1, ... , in CV k, the txt matrices
e
et
l.J = 1, ... , t, are ordered: PI 2: P2. Thus, by the minimax characterization of the eigenvalues of a Hermitian matrix, j = 1, ... ,t ,
in which Aj denotes the j'th eigenvalue of the indicated matrix, indexed in increasing size. In particular, AII+I (P2) 2: 0 and hence the kernel based on S has at most 1/ negative squares. On the other hand, since X is (0+, J, P)II admissible, there exists a set of points fJl, ... , fJr in 0+ and vectors 1/1, ... ,1/r in CV k such that the 1· X r matrix with ij entry equal to
1/i X(fJdJ X(fJj )*1/j = 1/iC(fJi) Ip - S(fJi)S(fJj )* C(fJ.)*1/. P{3j(fJi) P{3j(fJi) 3 3 .has exactly 1/ negative eigenvalues. This shows that the kernel based on S has at least 1/ negative eigenvalues, providing that the exhibited equality is meaningful, i.e., providing that the points fJI. ... , fJr lie in the domain of analyticity of S. But if this is not already the case, it can be achieved by arbitrarily small perturbations of the points fJI,.·., fJr because S has at most count ably many isolated poles in 0+. This can be accomplished without decreasing the number of negative eigenvalues of the matrix on the left of the last equality because the matrix will only change a little since X is analytic in 0+, and therefore its eigenvalues will also only change a little. In particular, negative eigenvalues will stay negative, positive eigenvalues will stay positive, but zero eigenvalues could go either way. This can be verified by Rouche's theorem, or by easy estimates; see e.g., Corollary 12.2 of Bhatia [Bh] for the latter. •
5. 'H.p(S) SPACES
In this section we shall first obtain another characterization of the space 'R.r endowed with the indefinite inner product (3.5) in the special case that r = MxJMx is positive semidefinite. We shall then specialize these results to
X = [Ip
-8]
(5.1)
Alpay and Dym
S8
and
(5.2) where S is a p x q matrix valued function which is analytic in f2+ such that the multiplication operator Ms from to is contractive. The resulting space C([Ip - Sj) will then be designated by the symbol1ip (S).
HZ
H:
THEOREM 5.1. If X is a k x m matrix valued function which is analytic in
f2+ such that the multiplication operator Mx from H;;' to H; is bounded and if
then
(1) C(X) = ran
1
r'2
with norm
where P denotes the orthogonal projection of
(£) ran
r
is dense in ran
1
rI
H; onto the kernel of r.
and
{rg, rh}r = (rg, h}Hp for every choice of 9 and h in H;.
(9) C(X) is the reproducing kernel Hilbert space with reproducing kernel given by (9.1).
(,0 X is (f2+, p,J) admissible. (5) C(X) = 8(X). 1
PROOF. Since ker r = ker n, it is readily checked that II Ilr, as defined in 1 1 (1), is indeed a norm on ran r'2. Moreover, if r'2 fn, n = 1,2, ... , is a Cauchy sequence in 1 ran r I , then (I - P)fn is a Cauchy sequence in the Hilbert space H;, and hence tends to a limit 9 in H; as n 1 00. Therefore, since 1- P is an orthogonal projector, it follows by standard arguments that 9 = lim (I - P)fn = lim (I - p)2 fn = (I - P)g nloo
and hence that
nloo
1
IIr I fn
1
-
rIglir = 11(1 -
P)(fn - g)IIHp
= 11(1 - P)fn - gllHp . 1
Thus ran rI is closed with respect to the indicated norm; it is in fact a Hilbert space with respect to the inner product
Alpay and Dym
59
For the particular choice 9 = v/Pw with v E ([!k and wE fl+, the identity 1
(n f, n
1
g)r
= (I -
1
P)f, n 9)Hp
1
= (nf,g)H p =
V
*( nf)(w), 1
serves to exhibit
fg = XJX(w)* v = Aw v Pw 1
as the reproducing kernel for ran f'2. This completes the proof of (1), since there is only 1
one such space. (2) is immediate from (1) and the fact that ker f'2 = ker fj (3), (4) and (5) are covered by Theorems 3.3, 3.5 and 3.4, respectively. • For ease of future reference we summarize the main implications of the preceding theorem directly in the language of the p x q matrix valued function S introduced at the beginning of this section.
THEOREM 5.2. If S is a p x q matrix valued function which is analytic in fl+ such that the multiplication operator Ms from H$ to H: is contractive and if X and J are given by (5.1) and (5.£), respectively, then:
(1) f
= MXJM'X = 1- MsMs
(£) 'Hp(S) = ran
n
1
with 1
IIf'2 fll'Hp(S) = II(I - P)fllHp , 1
where P designates the orthogonal projection of H: onto ker f'2 . 1
(9) ran f is dense in ran f'2 and (fg, fh)'Hp(s) = (fg, h) Hp for every choice of 9 and h in H:.
(4) 'Hp(S) is a reproducing kernel Hilbert space with reproducing kernel Aw(.\) = Ip - S(.\)S(w)* Pw(.\)
(5.3)
The next theorem is the analogue in the present setting of general p E Do of a theorem which originates with de Branges and Rovnyak [dBR1] for Pw(.\) = 1 - .\w*. in
f
n+
E
H:
THEOREM 5.3. Let S be a p x q matrix valued function which is analytic such that the multiplication operator Ms from H' to H: is contractive and for let K,(J) = sup{ltf + MSgllt-p - IIg/lt-p : 9 E Hpq} •
Alpay and Dym
60
Then 1ip (S)
= {f E Hg:
"-u) < oo}
and
(5.4)
PROOF. Let X and J be given by (5.1) and (5.2), respectively. Then clearly Theorem 5.1 is applicable since
r=MXJMX =I-MsMs ~O. 1
Moreover, since r ~ I, it follows that r2 is a contraction and hence, by Theorem 4.1 of 1 Fillmore and Williams [FW], that I E ran n if and only if II
1
2
2
sup { III + (I - nn)2gllHp -lIgliHp : 9 E HpP} <
00 ,
or equivalently, if and only if
(5.5) Therefore, since
*
__~~~l
1
+ ker(MsMs)2
Hg = ran(MsMsp
,
any 9 E Hg can be approximated arbitrarily well by the elements of the form
* 1 (MsMsFu+v 1
with u E Hg and v E ker(MsMs)2. Thus the sup in (5.5) can be reexpressed as
1
.u E Hg and v E ker(MsMsF} = sup{1I1 + MsMsullk p -1I(MsMs)tullkp: u E = sup{1I1 + MsMsullk p - IIMsullkp: u E = sup{1I1 + Ms(Msu
This proves that
f
E ran
Hg}
+ w)lIk p -IiMsu + wllkp:
= sup{lIf + Mshllkp :... IIhllkp: hE
Hn u E Hg and wE ker Ms}
Hg} .
rt = 1ip (S) if and only if K.(f) < 00.
61
Alpay and Dym 1
Next, if f = rlh for some h E H:, then (as is also shown in [FW)) 2 * 1 = f} K,(f) = inf{lIhllH : (I - MsMS)Ih p = 11(1 - P)hll~p ,
where P denotes the orthogonal projection of H: onto the kernel of r. This serves to establish (5.4), thanks to item 2 of Theorem 5.2. •
n+ (1)
THEOREM 5.4. Let S be a p X q matrix valued function which is analytic in such that IIMsll ~ 1 and let J be given by (5.2). Then [I
- Mslf E 1ip(S), and
(£) 11[1 - Mslfll1lp(s) ~ (Jf,f)Hp for every choice of
f with components
9E H:
and h E
Hg,
=
[~]
E
H;' ,
if and only if
(5.6)
PROOF. Suppose first that (1) and (2) hold. Then, by Theorem 5.3,
11[1 - Mslfll~p(s) = IIg - MShll~p(s) = sup{lIg - Msh
+ Msull~
= sup{lIg + Msvll~p -lih
p
- lIull~p : u E Hpq}
+ vll~p:
vE
H3} .
Therefore, by the prevailing assumptions,
IIgll~p + 2Re(g,Msv}Hp + IIMsvll~p -lIhll~p - 2Re(h,v}Hp -lIvll~p
=~ IIgll~p - IIhll~p for every v E
Hg.
for every v E
H$
But this in turn implies that
and hence in particular, upon choosing
v = e( Msg - h). with e > 0 , that
Alpay and Dym
62
for every e > O. The desired conclusion (5.6) now follows easily upon first dividing through by e and then letting e ! o. Next, to obtain the converse, suppose that (5.6) holds. Then, by Theorem
5.2, [1 - Mslf = (1 - MsMs)g = rg belongs to 1ip(S) and
11[1 - Mslfll~p(s) = (rg, rg)'Hp(S) = (r9,9)H p =
IIgllhp-
=
(Jf, J)H p
Thus (1) and (2) hold and the proof is complete.
IIMsgllh p •
•
We remark that the inequality in (2) of the last theorem can be replaced by equality. Finally, to complete this section we observe that if S is a p x q matrix valued function which is analytic in 11+, then the multiplication operator Ms is contractive if and only if the kernel (5.3) is positive, i.e., if and only if it has zero negative squares. THEOREM 5.5. Let S be a p x q matrix valued function which i8 analytic on 11+. Then the kernel
Aw,(A) = Ip - S(A)S(W)*
Pw(A) is p08itive on 11+ if and only if IIMs II :5 1. PROOF. Suppose first that IIMsll :5 1 and let f = ~j=l ~i/ PWj for any choice of points WI. ••• ,Wn E 11+ and vectors 6, ... , ~n E a:: p. Then it is readily checked that n
L
~;AWi(wi){i = IIfllhp -IIMsfllhp ~ 0
i,j=l
which establishes the positivity of the kernel. form
f
Next, to go the other way, we define a linear operator T on finite sums of the given above by the rule
T.i. = S(w)*.i. . Pw Pw By the presumed positivity of the kernel Aw(A), T is well defined and contractive on finite sums of this form and hence, since such sums are de~ iii ·1J1ii~', CiDIl be extended by .
' , .. ·.l.\r,:·;·
Alpay and Dym
63
limits in the usual way to a contractive operator (which we continue to call T) on all of Hp. Finally the evaluation
~*(T*g)(w) =
(T*g, .i.)H Pw p
~ = (9,T-)H p
pw
= (g,S(W)*.i.)H p
Pw
= CS(w)g(w) ,
which is valid for every choice of ~ E (J;P, w E 11+ and 9 E H$ serves to identify T* with the multiplication operator Ms. Therefore
IIMsll = IIT*II as claimed.
$ 1 ,
•
COROLLARY. If S is a p x q matrix valued function which is analytic on 11+ such that IIMsl1 $ 1, then
Ip - S(w)S(w)*
~
(5.7)
0
for every choice of w E 11+. It is important to bear in mind that even through (5.7) implies that IIMsll $ 1 for Pw(A) = 1- AW* and Pw(A) = -21Ti(A - w*), the last corollary does not have a valid converse for every choice of P E 'Do, as we now illustrate by a pair of examples.
EXAMPLE 1. Let a(A) = 1 and b(A) = A2 so that 11+ = ID and let S be any "I O. Then scalar contractive analytic function from ID into ID such that S( ~) = -S( Ms is not a contraction.
-!)
DISCUSSION. It follows from the standard Nevanlinna-Pick theory (see e.g. [D2]) that there exists an S of the desired type with S( ~) = c if and only if the 2 x 2 matrix [ 1-S(Wi )S(Wj )*] , (5.8) i,j=I,2, Pw;(Wi) with WI = -W2 =~, S(wt} = -S(W2) = c, and Pw(A) = 1 - Aw* is positive semidefinite. The matrix of interest:
is readily seen to be positive semidefinite if and only if
lei $
!.
Alpay and Dym
64
On the other hand, if IIMsll ~ 1, then the matrix (5.8) must be positive semidefinite for the same choice of points and assigned values as before but with Pw(..\) = 1 - ..\2w*2. But this matrix:
[*'*']
1+1,1 2 ~ 1-1 16 t=I7f6 is not positive semidefinite for any c f= 0 as is readily seen by computing its determinant. EXAMPLE 2. Let Pw(..\) = -211"i("\ - w*)(1 - ..\w*) with a(..\) and b(..\) as in (R.!), and let S(w) = c for w E ID n
f= O.
DISCUSSION. If IIMsll ~ 1, then the matrix (5.8) will be positive semidefinite for any pair of points Wl,W2 in f!+. For the particular choice WI = i/Ot, W2 = -iOt with Ot > 1, the matrix of interest is equal to
411"(1-0 )/0
which is not positive semidefinite if c
f= o.
6. LINEAR FRACTIONAL TRANSFORMATIONS In this section we shall recall a number of well-known properties of the linear fractional transformation
(6.1) for
8 = [8 11 8 12 ] 821 822 which is analytic and J = Jpq contractive in f!+. In particular it is well known that the indicated inverse exists if (the p x q matrix valued function) So is analytic and contractive in f!+ and that in this case TalSo] is also analytic and contractive in f!+. THEOREM 6.1. If8 is given by (2.14) and the matrices A and B in (2.10) are such that A is invertible and the spectral radius of BA -\ is less than one, then 8 is analytic in f!+ and the multiplication operator Ma is bounded on H~ . _PROOF .
.1~y
(2.14) and (2.1O),
9(..\) = Im - a(J.t)*{I- s(..\)s(J.t)*}VA-l{Im - s(A)BA-l}-1 p-l F(J.t)* J , where, as before, s(..\) = b(..\)/a(..\). In particular 00
{Im - s("\)BA-l}-l =
L
n=O
s(..\)n(BA-l)n
Alpay and Dym
65
and since by assumption 00
E II(BA- 1)nll <
00
n=O
it is easily seen that 8(A) admits a representation of the form 00
8(A)
=E
s(A)n8 n
n=O
with m
X
m matrix coefficients 8 n which are summable: 00
E 118
n
ll < 00.
n=O
It now follows readily by standard estimates that if
belongs to
H;:, i.e., if the m x 1 vector coefficients Uj are norm square summable, then 00
IIMefll~p =
2
n
E8 E j=O
n -juj
n=O
But this proves that 00
IIMell :5
L 118
n
ll < 00
j
n=O
as claimed.
•
THEOREM 6.2. Let So be a p x q matrix valued function which i8 analytic in .n+ such that the multiplication operator Mso is contractive, let 8 E 'P~(n+) be analytic in n+, and let S = Ta[Sol. Then IIMsll :5 1. PROOF. IT S = Ta[Sol, then it is readily checked that
[Ip -
SJ8 =
E[Ip - Sol,
Alpay and Dym
66
where
E = 811 - S821 . Now let
x = [Ip
- S].
Then
Ip - S( a )S(~)*
X(a)JX(~)*
pf3(a)
pf3(a) = X(a) J - 8(a)J8(~)** X(~)* Pa(~) = X(a) J -
+ X(a)8(a)J8(~)* X(~)* pf3(a)
8(a)J8(~)** X(~)* + E(a) {Ip - So(a)So(~)*} E(~)* .
pf3(a)
Pa(~)
(6.2) By Theorem 5.5,
IIMsl1 :::;
1 if and only if (6.3)
for every choice of points al, ... ,an in 11+ and vectors 6, ... ,~n in ([;p. Since II Mso II :::; 1 by assumption, the inequality (6.3) holds with So in place of S. Therefore, by (6.2) it • holds for S also, since 8 E pJ(11+). Thus IIMsll :::; 1. Now as
8 = [8 11 821
8 12 ] 822
is J = Jpq contractive in 11+, it can be expressed in the form
(6.4) where
e2 = 822 is invertible in 11+, 0"1
= 81282"l,
0"2
= 82"l821
,
el = 811 - 81282"i 821 and et, O"t, 0"2 and e2"l are all contractive in 11+; see e.g., p.15 of [D2]. THEOREM 6.3. Its is as in Theorem 6.~, then the multiplication operators M U2 , MU1 and M €2-1 are all contractive. Moreover, MU2 is a strict contraction. PROOF. Since
KW(A) = J - 8(A)J8(w)* Pw(,\)
67
Alpay and Dym
has zero negative squares in fl+, the same holds true for its 22 block:
(6.5) for every choice of aI, ... , ak in fl+ and 111, ... ,11k in CV q . Thus clearly
and
for every such choice of al , ... , ak and 111, ... ,11k. Thus, by Theorem 5.5, the multiplication operators M -1 and MCT2 are both contractive. E2
The proof that MCTI is contractive is immediate from Theorem 6.2 and the observation that 0"1 = Ta[O] . To check that MCT2 is strictly contractive, it suffices to note that (6.5) implies that
• 7. ONE-SIDED INTERPOLATION In this section we study the following general one-sided interpolation problem for a fixed p E Vn. The data for this problem consists of a set of (not necessarily distinct) points WI , •.. , Wn in fl+ and two sets of associated vectors ~I," ',~n
1111,· .. , 11lrl j 1121,· .. , 112r2 j
in ••• j
CV P
11nl, ... ,11nrn
In
cvq
such that are linearly independent. The problem is to find necessary and sufficient conditions on the data for the existence of a p x q matrix valued function S such that: (1) (2)
S is analytic in fl+ (which is actually automatic from (3»,
e'!' J
5('-I)(""j) -
(t I)!
•
- Tljt '
t
= 1•... ,rj j
j
= 1, ... ,n ,
Alpay and Dym
68
(3)
The operator Ms of multiplication by S is a contractive map of H3 into
H:.
It is also desirable to give a description of the set of all solutions to this problem when these conditions are met. We shall solve this interpolation problem by adapting the strategy of Section 7 of [D3] to the present setting. We begin by introducing the auxiliary notation
Vj = [Vjl···Vjrj]' Fj
[II··· fv]
= Vjc)wj,rj' = [Fl··· Fn]
j = l, ... j
,
,n,
= 1, ... ,n . v = T} + ... + rn
,
and t = 1, ...
where 9t E
Juch that if
,v,
H: and ht E H3. LEMMA 7.1. Let S be a p x q matrix valued function which iJ analytic in n+ 1. Then S iJ a Jolution of the Jtated interpolation problem if and only
IIMsll $
(7.1) for
t = 1, ... , v.
PROOF. In order to keep the notation simple we shall deal with the first block, i.e., the columns in Fl, only. The rest goes through in just the same way. By definition, t
ft =
L
ct'Wl ,t-jVlj ,
t = 1, ... , rl
.
j=l
with components 9t
and
= ct'wl,t-16 t
ht =
L ct'wt ,t-jT/lj . j=l
Thus, by the evaluation in Corollary 2 to Lemma 3.2,
The rest is selfevident since the functions ct'wt ,0, ... ,ct'wl,t-l are assumed to be linearly independent in the formulation of the problem. •
Alpay and Dym
69
THEOREM 7.1. The one-$ided interpolation problem which wa$ formulated at the beginning of thi$ $ection i$ $olvable if and only if the 11 x 11 matrix P with ij entry
(7.2) i$ pO$itive $emidefinite. PROOF. Suppose first that the interpolation problem is solvable, and let S be a solution. Then, by the preceding lemma, the components gt and ht of ft are related by formula (7.1). Thus if v
v
f = LCjli
and
9 = LCjgj
j=l
for some choice of constants
Therefore
C}, ••• , C v ,
j=l
then
v
CiPijCj = {Jf,f)H p
L i.i=l
~
since
0,
IIMsll = IIMsll ::; 1. Now suppose conversely that P> 0 and let
M =span{h, ... ,fv} endowed with the J inner product
Then, with the help of Theorem 2.3, it is readily checked that conditions (1) and (2) of Theorem 2.1 are met. Now let
A = diag{Awl' ... , Awn}
and
B = diag{Bw1 ,· .. , Bwn}
be the block diagonal matrices with entries Awj and BWj of size Then F{A} = V{a{A}A - b(A)B}-l
rj x rj
given by (2.6).
{7.3}
and, by Theorem 2.2,
A*PA - B*PB = V· JV .
(7.4)
Alpay and Dym
70
Therefore, by Theorem 2.1, M is a finite dimensional reproducing kernel Hilbert space with reproducing kernel Kw('x) = J - 6('x)J6(w)*
Pw(A) where
e is uniquely specified up to a right J unitary factor by (2.14).
Moreover, since
it follows easily from (2.14) that 6 is analytic in all of 11 except at the union of the zeros of the functions PWI , ••• , PWn' In particular, 6 is analytic in 11+ and is both analytic and invertible at the special point J.I. E 110 which is used in the definition of 6. Thus 6 is invertible in all of 11 except for an at most countable set of isolated points. Moreover, it is readily checked that Theorem 6.1 is applicable for the current choices of A and B, and hence that the multiplication operator Me is a bounded mapping of H;: into itself. Next, since
is a reproducing kernel for
H;:, it is easily seen that
v *ft () a
= (Jft, J =
- 6J6(a)*v) Hp
POt
(f~) - (Jft, 6J6(a)*v) Hp t, Hp POt
POt
-- v *ft ( a ) - (Jf t , 6J6(a)*v) H ,
POt
p
and hence that v* J6(a)J(Me J Jt}(a) = (MeJ/t, J6(a)* JV)H
POt
p
= (Jf 6J6(a)*v) t, Hp
POt
=0 for every choice of a E 11+ and v E «::m. Therefore, since 6 is invertible except for at most a set of isolated points in 11+, it follows that (the analytic vector valued function)
(7.5) Now, by (6.4), where
1111 --
[e01
and
Alpay and Dym
71
By Theorems 6.1 and 6.3, M\f!l and M\f!2 are both bounded multiplication operators on Thus it is meaningful to write
H;J'.
and therefore, since M(,2 is clearly invertible, it follows from (7.5) that
M(,Jft = O. But this in turn reduces to the pair of constraints
(7.6) and
M:2 {M;19t - ht} = 0 . But now as
M:
2
is invertible (with inverse (Me -I)*) the latter constraint implies that 2
This exhibits 0"1 as a solution to the given interpolation problem, thanks to Lemma 7.1 and Theorem 6.3. This completes the proof of the existence of a solution to the stated interpolation problem when P > o. It remains to show that the interpolation problem is also solvable when P ;::: 0, by passage to limit. To this end, let us first write
P=G-H
with entries corresponding to the decomposition
By assumption G > O. Now, just as in [D2], let us replace the 'lij ill the formulation of the problem by "lij(l the perturbed data,
I
+ £)-2"
with £ >
o.
Then the new Pick matrix, corresponding to
1 Pe =G---H 1+£ £ 1 =--G+--P 1+£ 1+£
>_£-G>O -1+£ for every choice of £ > o. Therefore, by the preceding analysis, there exists a p x q matrix valued analytic function Se with IIMsc II ~ 1 such that
Alpay and Dym
72
for j = 1, ... , /I. The proof is completed by letting e ! 0 and invoking the fact that the unit ball in the set of bounded operators from H: to H$ is compact in the weak operator topology (see e.g., Lemma 2.3 on p.102 of [Be]). This means that there exists a contractive operator Q from H: to H$ such that
for every choice of f E H: and g E H$ as e ! 0 through an appropriately chosen subsequence (which we shall not indicate in the notation). In particular,
= (ht,U)H
p •
Now let T = Ms denote the operator of multiplication by s = bl a on H;, regardless of the size of r. Then since MScT = TMSc for every e > 0, it is readily checked that Q*T = TQ* and hence, by Theorem 3.3 of [AD4], that there exists a p x q matrix valued function S which is analytic in n+ such that Q* = Ms. This completes the proof, since S is a solution to the one-sided interpolation problem. • THEOREM 7.2. If the /I x /I matrix P with entries given by (7.2) is positive definite and if is specified by (2.14) for the space M considered in the proof of the last theorem, then
e
{Ta[So]: So is analytic in
n+
and
IIMsoil
$;
I}
is a complete list of the set of solutions to the given interpolation problem. PROOF. The proof is divided into steps. STEP 1. If S is a solution of the interpolation problem, then
Y = [Ip
- SIS
is (0+, J,p) admissible. PROOF OF STEP 1. The argument is adapted from the proof of Theorem 6.2 in [D2]. Let X = [Ip - S] and let
Aw(A) = X(A)JX(W)* Pw(A) denote the reproducing kernel for 'Jtp(S). Then it is readily seen that
Y(a)JY(,B)* = _X~(a...:...)J....,..X-:"(::...,B~)* p~(a)
p~(a)
X(a){J - 9(a)JS(,B)*}X(,B)* p~(a)
= Ap(a) - X(a)F(a)p-lF(,B)* X(,B)*
Alpay and Dym
73
for a and j3 in f2+. Thus if n
f = LAat~t t=1 for any choice of aI, ... ,an in f2+ and (}, ... ,~n in (Vm and if 'Yij denotes the ij entry of p-l, then
n
v
- L L ~;X(as)li(ashij/j(at)* X(at)*~t . s,t=1 i,j=1 Moreover, since S is an interpolant, it follows from Lemma 7.1 and Theorem 5.4 that X Ii E Ji p ( S) and hence that the right hand side of the last equality is equal to v
n
Ilfll~p(S) - L
L (X/;,Aas~shlp(S)'Yij(Aat6,Xfjhlp(S) s,t=1 i,j=1 v
= Ilfll~p(S)
-
L (X/;,fhtp(S)'Yij(f,X/jhlp(S) . i,j=1
But this in turn is equal to
Ilfll~p(S) - IIIIfll~p(S) in which II denotes the orthogonal projection of f onto the span of the Xli in B(X). This last evaluation uses the fact that Mx is an isometry from K(0) into B(X), as noted in the remark following Theorem 5.4. The rest is selfevident since
STEP 2. If S is an interpolant, then
[Ip
- Sl0
= ClIp
- Sol
where C and So are analytic in f2+, and Me is bounded and
IIMsJ ::; 1.
PROOF OF STEP 2. This is immediate from Theorem 3.5 since My is bounded (because both Ms and Me are; the former by assumption and the latter by Theorem 6.1), and Y is (f2+, J,p) admissible, by Step l. for some p
STEP 3. If S is a solution of the given interpolation problem, then S = Te[Sol matrix valued function So with IIMSo II ::; 1.
xq
PROOF OF STEP 3. By Step 2,
011 - Se21 = C
Alpay and Dym
74 and Therefore
S(821So
+ 822) = 811 So + 812
,
which is the same as the asserted formula. The term 821 So + 822 is invertible in n+ by standard arguments which utilize the fact that 8 is J contractive and So is contractive, both in n+. STEP 4. If S = Ta[So] for some pxq matrix valued function So with 1, then S is a solution of the given interpolation problem. PROOF OF STEP 4. By Theorem 6.2, 7.1 it is shown that 0"1 = Ta[O]
IIMsll :5 1.
IIMso II :5
In the proof of Theorem
is a solution of the interpolation problem. This means that
for t = 1, ... , v, and hence that S is a solution of the given interpolation problem if and only if for t = 1, ... , v. But now as
(Ms - M;1)9t = M:;lM(lq+tT2S0)-lMSoM:19t
=0, by (7.6). The calculation is meaningful because all of the indicated multiplication operators are bounded thanks to Theorem 6.3. This completes the proof of the step and the theorem. •
8. REFERENCES [Ab]
M.B. Abrahamse, The Pick interpolation theorem for finitely connected domains, Michigan Math. J. 26 (1979), 195-203.
[AI]
D. Alpay, Krein spaces of analytic functions and an inverse scattering problem, Michigan Math. J. 34 (1987), 349-359.
[A2]
- , Some remarks on reproducing kernel Krein spaces, Rocky Mountain Journal of Mathematics, in press.
[A3]
- , Some reproducing kernel spaces of continuous junctions, J. Math. Anal. Appl. 160 (1991),424-433.
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[A4]
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- , On linear combinations of positive functions, associated reproducing kernel spaces and a non-Hermitian Schur algorithm, Archiv der Mathematik (Basel), in press.
[AD1]
D. Alpay and H. Dym, Hilbert spaces of analytic functions, inverse scattering, and operator models I, Integral Equations and Operator Theory 7 (1984), 589641.
[AD2]
- , Hilbert spaces of analytic functions, inverse scattering, and operator models II, Integral Equations and Operator Theory 8 (1985), 145-180.
[AD3]
- , On applications of reproducing kernel space", to the Schur algorithm and rational J unitary factorization, in: I. Schur Methods in Operator Theory and Signal Processing (I. Gohberg, ed.), Operator Theory: Advances and Applications OTI8, Birkhauser Verlag, Basel, 1986, pp. 89-159.
[AD4]
- , On a new class of reproducing kernel spaces and a new generalization of the Iohvidov law"" Linear Algebra Appl., in press.
[AD5]
, On a new class of structured reproducing kernel spaces, J. Functional Anal., in press.
[ADD]
D. Alpay, P. Dewilde and H. Dym, On the existence and convergence of solutions to the partial lossle",s inverse scattering problem with applications to estimation theory, IEEE Trans. Inf. Theory,35 (1981), 1184-1205.
[Ar]
N. Aronszajn, Theory of reproducing kernel"" (1950), 337-404.
[AI]
T.Ya. Azizov and I.S. Iohvidov, Linear Operator", in Spaces with an Indefinite Metric, Wiley, New York, 1989.
[Ba1]
J.A. Ball, 235-254.
[Ba2]
- , Factorization and model theory for contraction operators with unitary part, Memoirs Amer. Math. Soc. 198, 1978.
[Be]
B. Beauzamy, Introduction to Operator Theory and Invariant Subspaces, North Holland, 1988.
[Bh]
R. Bhatia, Perturbation bounds for matrix eigenvalues, Pitman Research Notes in Math., 162, Longman, Harlow, UK, 1987.
[Bo]
J. Bognar, Indefinite Inner Product Spaces, Springer-Verlag, Berlin, 1974.
[dB1]
L. de Branges, Hilbert "'paces of analytic functions, I, Trans. Amer. Math. Soc. 106 (1963), 445-468.
[dB2]
- , Hilbert Spaces of Entire Functiona, Prentice Hall, Englewood Cliffs, N.J. . 1968.
[dB3)
- , The expansion theorem for Hilbert spaces of entire functions, in: Entire Functions and Related Topics of Analysis, Proc. Symp. Pure Math., Vol. 11, Amer. Math. Soc., Providence, R.I., 1968.
Trans. Amer. Math. Soc. 68
Models for non contractiona, J. Math. Anal. Appl. 52 (1975),
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[dB4)
- , Complementation in Krein spaces, Trans. Amer. Math. Soc. 305 (1988), 277-291.
[dB5)
- , Krein spaces of analytic functions, J. Functional Anal. 81 (1988), 219-259.
[dBR)
L. de Branges and J. Rovnyak, Canonical models in quantum scattering theory, in: Perturbation Theory and its Applications in Quantum Mechanics (C. Wilcox, ed.), Wiley, New York, 1966, pp. 295-392.
[dBS)
L. de Branges and 1. Shulman, Perturbations of unitary transformations, J. Math. Anal. Appl. 23 (1968), 294-326.
[DLS)
A. Dijksma, H. Langer and H. de Snoo, Characteridic functions of unitary operator colligations in 'Irk spaces, in: Operator Theory and Systems (H. Bart, I. Gohberg and M.A. Kaashoek, eds.), Operator Theory: Advances and Applications OT19, Birkhauser Verlag, Basel, 1986, pp. 125-194.
[D1)
H. Dym, Hermitian block Toeplitz matrices, orthogonal polynomials, reproducing kernel Pontryagin spaces, interpolation and extension, in: Orthogonal MatrixValued Polynomials and Applications (I. Gohberg, ed.), Operator Theory: Advances and Applications OT34, Birkhauser Verlag, Basel, 1988, pp. 79-135.
[D2)
- , J Contractive Matrix Functions, Reproducing Kernel Hilbert Spaces and Interpolation, CBMS Regional Conference Series in Mathematics, No. 71, Amer. Math. Soc., Providence, 1989.
[D3)
- , On reproducing kernel spaces, J unitary matrix functions, interpolation and displacement rank, in: The Gohberg Anniversary Collection (H. Dym, S. Goldberg, M.A. Kaashoek and P. Lancaster, eds.), Operator Theory: Advances and Applications OT41, Birkhauser Verlag, Basel, 1989, pp. 173-239.
[D4)
- , On Hermitian block Hankel matrices, matrix polynomials, the Hamburger moment problem, interpolation and maximum entropy, Integral Equations and Operator Theory 12 (1989), 757-812.
[FW)
P.A. Fillmore and J.P. Williams, On operator ranges, Adv. Math. 7 (1971), 254-281.
[IKL)
I.S. Iohvidov, M.G. Krein and H. Langer, Introduction to the Spectral Theory of Operators in Spaces with an Indefinite Metric, Mathematische Forschung, Vol. 9, Akademie-Verlag, Berlin, 1982.
[LAK)
H. Lev-Ari and T. Kailath, Triangular factorization of structured Hermitian matrices, in: I. Schur Methods in Operator Theory and Signal Processing (I. Gohberg, ed.), Operator Theory: Advances and Applications OT18 (1986), 301-324.
[Nu)
A.A. Nudelman, Lecture at Workshop on Operator Theory and Complex Analysis, Sapporo, Japan, June 1991.
[Ro)
M. Rosenblum, A corona theorem for countably many functions, Integral Equations and Operator Theory 3 (1980), 125-137.
[Sch]
L. Schwartz, Sow espaces hilbemens d'espaces vectoriels topologiques et ooyaw: ~socies (noyauz reproduisants), J. Analyse Math. 13 (1964), 115-256.
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[So]
P. Sorjonen, Pontrjaginrii:ume mit einem reprod'Uzierenden Kern, Ann. Acad. Sci. Fenn. Ser. A Math. 594 (1973), 1-30.
[Y]
A. Yang, A con8troction of Krein 8pace8 of analytic junction8, Ph.D. Thesis, Purdue University, May, 1990.
D. Alpay Department of Mathematics Ben Gurion University of the Negev Beer Sheva 84105, Israel
MSC: Primary 47A57, Secondary 47A56
H.Dym Department of Theoretical Mathematics The Weizmann Institute of Science Rehovot 76100, Israel
78
Operator Theory: Advances and Applications, Vol. 59 © 1992 Birkhiiuser Verlag Basel
THE CENTRAL METHOD FOR POSITIVE SEMI-DEFINITE, CONTRACTIVE AND STRONG PARROTT TYPE COMPLETION PROBLEMS
Mihaly Bakonyi and Hugo J. Woerdeman
In this paper we obtain a new linear fractional parametrization for the set of all positive semi-definite completions of a generalized banded partial operator matrix. As applications we obtain a cascade transform parametrization for the set of all contractive completions of a triangular partial operator matrix satisfying possibly an extra linear constraint (thus extending the results on the Strong Parrott problem). In each of the problems also a maximum entropy principle appears.
1. Introduction. In this paper we establish a new parametrization for the set of all positive semi-definite completions of a given "generalized banded" operator matrix. Before we elaborate on this problem we start with.an important application, namely a generalization of the Strong Parrott problem introduced by C. Foia.!l and A. Tannenbaum. It concerns the following. For 1 :5 i :5 j :5 n let Bij : 'Hj ---+ Ki be given bounded linear operators acting between Hilbert spaces. Further, let also be given the operators
(1.1)
We want to find contractive completions of the following problem:
(1.2)
i.e., we want to find Bij, 1 :5 j < i :5 n, so that B = (B;j)f.j=l is a contraction satisfying the linear constraint BS = T. The introduction of the Strong Parrott problem was a consequence of questions arising in the theory of contractive intertwining dilations (see, e.g., the recent book by C. Foia.!l and A.E. Frazho [10]).
Bakonyi and Woerdeman
79
For the problem (1.2) we derive neccessary and sufficient conditions for the existence of a contractive solution. In case these conditions are met we build a so-called "central completion", a solution with several distingueshed properties. From the central completion we construct a cascade transform parametrization for the set of all solutions. As we mentioned before the above results appear as application of our results on positive semi-definite completions. The (strictly) positive definite completion problem is a well studied subject. The first tesults in this domain were by H. Dym and I. Gohberg in [8]. These results were in many ways generalized by H. Dym and I. Gohberg (see the references in [12]) and I. Gohberg, M.A. Kaashoek and H.J. Woerdeman in [12], [13], [14]. A complete Schur analysis of positive semi-definite operator matrices was given by T. Constantinescu in [7], and these results were later used by Gr. Arsene, Z. CeaUi~escu and T. Constantinescu in [1] in positive semi-definite completion problems. An analysis of positive semidefinite completions in the classes of so-called U· DU- and L* DL-factorable positive semi-definite operator matrices was recently given by M. Bakonyi and H.J. Woerdeman in [3]. The methods in [3] cover the finite dimensional case, but do not extend to the general case described in this paper. In the study of positive semi-definite" generalized banded" completions, we first develop some distingueshed properties which uniquely characterize a so called central completion, a notion that appeared in different settings and with different names in [8], [1], [12] and [3]. Next we present a result on which the rest of the paper is based, namely a linear fractional transform parametrization for the set of all solutions. The coefficients of the transformation are obtained from the Cholesky factorizations of the central completion. This is a generalization of results in [12], where the positive definite case was considered, and of results in [3]. Our paper is organized as follows. In Section 2 we treat positive semi-definite completions and in Section 3 contractive completions. Section 4 is dedicated to the study of a generalized Strong Parrott problem. 2. Positive Semi-Definite Completions. Consider the following 3 x 3 problem:
(2.1 ) where (2.2) By this we mean that we want to find the (1,3) entry Al3 of the operator matrix in (2.1) such that with this choice (and with A3l = Ai3) we obtain a positive semi-definite 3 x 3 operator matrix. Note that the positivity of the 2 x 2 operator matrices in (2.2) implies that
Bakonyi and Woerdeman
80
where G I : R(A 22 ) -+ R(A 11 ) and G 2 : R(A 33 ) -+ R(A 22 ) are contractions. For a linear operator A we denote by R(A) its range and by R(A) the closure of its range, and if A ~ 0 then AI/2 is its square root with AI/2 ~ O. Let also for a contraction G : C -+ Ie denote Do = (Ie - G*G)I/2 : C -+ C and 'Do = R(D o ). It was proved in [1] that there exists a one-to-one correspondence between the set of all positive semi-definite completions of (2.1) and the set of all contractions G: 'D02 -+ 'Do~ via
(2.3) With the choice G
= 0 we obtain the particular completion A 13
(2.4)
I/2 = A 11I/2G 1 G2 A33·
We shall call this the central completion of (2.1), referring to the fact that in the operator ball in which A I3 lies (namely the one described by (2.3)) we choose the centre. If F is a positive semi-definite operator matrix it is known that there exist an upper triangular operator matrix V and a lower triangular matrix W such that
F
(2.5)
= V"V = wow.
The factorizations (2.5) are called lower-upper and upper-lower Cholesky factorizations, respectively. Moreover if V and Ware upper (lower) triangulars with F = V"V = W·W, then there exists block diagonal unitaries U : R(V) -+ R(V) and 0 : R(W) -+ R(W) with UV = V and Ow = W. This implies that if F is a positive semi-definite n x n operator matrix, then the operators
(2.6)
6. u (F) := diag(l';iVii)i'=I
and
(2.7) do not depend upon the particular choice of V and W in (2.5). Returning to our problem (2.1), if F is an arbitrary completion corresponding to the parameter G in (2.3) then F admits the factorization (2.5) with
AI/2
(2.8)
V
=
(
11
0
o
l/2 G 1 A 22 (G I G2 + Do~ G D02 )A;~2 ) I/2 (Do, G - GjGD )A;~2 D0, A 22 2 02 o DoD02A;~2
and
o
(2.9)
I/2 D O A 22 2 G * AI/2 2
22
Bakonyi and Woerdeman
81
Further, using relations like GiCDaj) ~ Va" one easily obtains that R(V;i) ~ R(V;i) and R(Wii) ~ R(Wii), for all i and j. The triangularity of V and W now yields
(2.10)
-
'R.(V)
1/2 = 'R.(An ) EB Val
-
EB Va, 'R.(W)
= V a * EB Va,
-
1/2
EB'R.(A33 ).
One immediately sees from these equalities that when G = 0 the closures of the ranges of the Cholesky factors of the completion are as large as possible. Relation (2.5) implies the existence of a unitary U : R(W) ~ R(V) with UW = V. A straightforward computation gives us the explicit expression of U, namely
(2.11)
Note that the (3,1) entry in U is zero if and only if G = O. As it will turn out, this will be a characterization for the central completion, thus providing a generalization of the banded inverse characterization in the invertible case, discovered in [8]. We will state the result precisely in the n x n case. Before we can do this we have to recall the following. We remind the reader of the Schur type structure of positive semi-definite matrices obatined in [7]: There exists an one-to-one correspondence between the set of positive semi-definite matrices (Aij )7,j=1 with fixed block diagonal entries and the set of all upper triangular families of contractions 9 = {fiih:5i:5i:5n, where fii = I1?(Aii)' i = 1, ... , n, and f ij : Vr'+I.J ~ Vr,.J-1 for 1 :5 i < j :5 n. The family of contractions 9 is referred to as the choice triangle corresponding to (Aii )7,i=I' In [7] it is also proven that if A ;::: 0 and 9 = {fij h
(2.12) upper triangluar and (2.13) lower triangular. The operators V and W have dense range, and their block diagonal entries are given by
(2.14)
TI:. - Dr Ii ... Dr i-I.. A1(2 Vil u
and (2.15) Let us now consider the n x n generalized banded positive semi-definite completion problem. Recall that S ~ 11 x 11 (11 = {I, ... , n}) is called a genemlized banded pattern if (1) (i,i) E S, i = 1, ... ,nj (2) if (i,j) E S then (j,i) E Sj and (3) (i,j) E Sand
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82
i :5 p,q :5 j imply (p,q) E S. The problem is the following. Given are Aij : 'Hj -+ 'Hi for (i,j) in a prescribed generalized banded pattern S. We want to find Aij, (i,j) E (ll X 1l)\S such that A = (Aij )f,j=l 2: o. Such an operator matrix A will be called a positive semi-definite completion of the band {Aij, (i,j) E S}. It is known (see [8]) that a positive definite completion of {Aij, (i,j) E S} exists if and only if
(2.16)
(Aij )i,jEJ 2: 0
for all J ~ II with J x J ~ S. When {A ij , (i,j) E S} verifies condition (2.16) we shall call this band positive semi-definite In [1] a parametrization was given for the set of all positive semi-definite completions of {Aij, (i,j) E S} as follows. This parametrization is based on the result in [7] quoted above and the fact that making a completion of {Ai;' (i,j) E S} precisely corresponds to choosing the parameters {rij,1 :5 i :5 j :5 n, (i,j) ¢ S}. Thus there exists an one-to-one correspondence between the set of all positive semi-definite completions of {Ai;' (i,j) E S} and the completions of {rij, 1 :5 i :5 j :5 n, (i,j) E S} to a (Aii)i':l choice triangle. This parametrization is recursive in nature, because of the way the choice triangles are constructed. The completion corresponding to the choice rij = 0 whenever 1 :5 i :5 j :5 n with (i,j) ¢ S is called the central completion of {A ij , (i,j) E S}. It shall be denoted by Fe, where the subscript" c" stands for central. An alternative way to obtain the central completion is described below. For a given n x n positive generalized band {Aij, (i,j) E S} one can proceed as follows: choose a position (io, jo) ¢ S, io :5 jo, such that S U {( i o, jo), (io, io)} is also generalized banded. Choose AiD,jD such that (Aij)1~j=io is the central completion of {Ai;' (i,j) E Sand io :5 i,j :5 jo}. This is a 3 x 3 problem and AiD,jD can be found via a formula as in (2.4). Proceed in the same way with the thus obtained partial matrix until all positions are filled. It turns out (see [1]) that the resulting positive semi-definite completion is the central completion Fe. Note that for (io,jo) ¢ S, io :5 jo, the entry AiD,jD only depends upon {Aij , (i,j) E Sand io :5 i,j :5 jo}. This implies that the submatrix of Fe located in the rows and columns {k, k + 1, ... , I} is precisely the central completion of {Aij , (i,j) E Sn {k,k+ 1, ... ,1} x {k,k+ 1, ... ,I}}. This principle is referred to as the "inheritance principle". Our first result gives four equivalent conditions which characterize the central completion. This is a positive semi-definite operator analogue of Theorem 6.2 in [81. THEOREM 2.1. Let S be generalized banded pattern and F a positive semi-definite completion of {Aij, (i,j) E S}. Let F = V·V = W·W be the lower-upper and upperlower Cholesky factorizations of F. Then the following are equivalent: (i) F is the central completion of {A ij , (i,j) E S}. (ii) ~u(F) 2: ~u(p) for all positive semi-definite completions P of {A ij , (i,j) E S}; (iii) ~L(F) 2: ~L(P) for all positive semi-definite completions P of {A ij , (i,j) E S}; (iv) The unitary U : 'R.(W) -+ 'R.(V) with UW = V verifies Uij = 0 for i 2: j,(i,j)¢S.
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Note that the uniqueness of the central completion implies that t.u(F) = t.u(F) (or t.L(F) = t.L(F)) yields F = F. The maximality of t.u(F) (t.L(F)) can be viewed as a maximum entropy principle (see, e.g., [6]). Proof. The equivalence of (i) and (ii) can be read off immediately from (2.14), and similarly the equivalence of (i) and (iii) can be read off immediately from (2.15). We prove the equivalence if (i) and (iv) by induction on the number of missing entries in the pattern S. For the 3 x 3 problem (2.1), discussed at the beginning of this section, formula (2.11) proves immediately the equivalence. Let S ~ n x n be a generalized banded pattern and {Aij , (i,j) E S} positive semidefinite. Let Fe denote the central completion of {Aij, (i,j) E S}, and let v;, and We be upper and lower triangular operator matrices such that
(2.17)
R(v;,) so that UWe = v;,. Let 5 F = (h)n~1 obtained from Fe by IJ=I Fij = (Fe)ij for i,j ::; n - 1,
Consider the unitary operator matrix U : R(We) denote the pattern
5 = S n (n -
-+
1 x n - 1), and
compressing its last two rows and columns. So,
and
Fn-I,n-I
=
((P(pe)n)-I,n-I e n,n-I
(P(pe)n)-I,n). e nn
Consider the data {Fij , (i,j) E 5}. From the way the central completion is defined one sees that F(= Fe) is the central completion of {Fih(i,j) E 5}. Now, in the same way, consider the operator matrices U = (Uij )i,j=I' V = O%j )i,j=1 and W = (Wij)i,j=1 obtained by the compression of the last two rows and columns of U, v;, and We, respectively. We obtain by the induction hypothesis that Uij = 0 for (i,j) f/- 5 with i > j. Thus it remains to show that Unj = 0 for j with (n,j) f/- Sand (n - l,j) E S. For this purpose let I = min{j, (n,j) E S} and consider the decomposition
with Ell = (UiJrr~I' E22 = (uiJ·)n-:-2 and E33 = Unn . Consider also the corresponding 1,)",)_,,( decomposition of Fe = (
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But then from the 3 x 3 case we obtain that E 13 = 0 and, consequently, Unj = 0 for j ~,- 1, proving (iii). Implication (iii) -+ (i) can be proved by the same type of induction process. One needs to use the observation that if SI and S2 are two generalized banded patterns and F is the central completion of both {Aii> (i,j) E Sd and {Aij, (i,j) E S2}, then F is the central completion of {Aij, (i,j) E SI n S2}. We omit the details. 0 THEOREM 2.2. Let S ~ 1l x 1l be a generalized banded pattern and {Aii> (i,j) E S} be positive semi-definite. Let Fe denote the central completion of {Aij, (i,j) E S}, and v;, and We be upper and lower triangular operator matrices such that (2.18) Further, let U : R(We )
-+
R(v;,) be the unitary operator matrix so that
(2.19) Then each positive semi-definite completion of {Aij, (i,j) E S} is of the form
(2.20)
where G = (G ij )7,j=1 : R(v;,) -+ R(We ) is a contraction with G ij = 0 whenever i ~ j or (i,j) E S. Moreover, the correspondence between the set of all positive semi-definite completions and all such contractions G is one-to-one. The decompositions of R(V) and R(W) are given by
(2.21 ) and (2.22) Before starting the proof, we need additional results. PROPOSITION 2.3. Let S ~ 1l x 1l be a generalized banded pattern and {Aij, (i, j) E S} positive semi-definite. Let Fe denote the central completion and F an arbitrary positive semi-definite completion of {A ij , (i,j) E S}. Then (2.23) We remark first that if > is an operator on 11. and A = >* > then there exists a unitary U on 11. such that Al/2 = U>, and thus R(>*) = R(Al/2). Thus (2.23) is equivalent with the fact that if Fe = E~Ee and F = E*E with Ee and E upper (lower) triangular then R(E*) ~ R(E~).
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Proof. We start the proof with the 3 x 3 problem (2.1). Let F be the positive semi-definite completion of (2.1) corresponding to the parameter Gin (2.3). Then, as we have already seen, F = V*V where V is given by (2.8). Thus
(2.24)
V
=(
I 0 DGoG) 0 I -GiG Vc, o 0 DG
which yields R(V*) ~ R(Y.,*). The result now follows from the remark preceeding the proof. Consider now a given generalized banded pattern S ~ D x D. We prove our result by induction assuming the statement is correct for all generalized banded patterns 5 which have S as a proper subset. The case S = 11 x 11\{(l,n),(n,l)} reduces to the 3 x 3 problem. Let (io,jo) f/. S, io < jo, be such that 5' = S U {(io,jo)'(jo,i o)} is also generalized banded. Let {Ai;' (i,j) E S}, Fe and F be as in the statement of the proposition. Consider the partial matrix {Bij , (i,j) E 5}, where Bij = Fij for (i,j) E 5. Let Fe denote the central completion of this latter partial matrix. By the induction hypothesis, since clearly F is a completion of {Bij , (i,j) E 5} we have that (2.25) Observe that the matrices Fe and Fe differ only on the positions (i,j) and (j, i), where 1 :5 i :5 io and jo :5 j :5 n. Moreover, defining 5 = (11 x 11)\ {(i, j), (j, i), 1 :5 i :5 i o, jo :5 j :5 n} and the partial matrix {Cij , (i,j) E 5}, where Cij = (Fe)ij for (i,j) E 5, we have that Fe is also the central completion of this latter partial matrix. We can now use the 3 x 3 case to conclude that (2.26) since Fe can be viewed as a completion of {Cij , (i,j) E 5}. Now (2.23) is a consequence of (2.25) and (2.26), and the remark preceeding the proof. D PROPOSITION 2.4. Let S ~ 7! x 7! be a generalized banded pattern and {A ij , (i, j) E S} positive semi-definite. Let Fe denote the central completion and F an arbitrary positive semi-definite completion of {A ij , (i,j) E S}, and let (2.27) be lower-upper and upper-lower Cholesky factorizations of Fe. Then, if F - Fe = 0* + 0, where = (Oij)ij=l with Oij = 0 whenever i ~ j or (i,j) E S, there exists an operator matrix Q = (Qij)iJ=l : ft(l/;,) --.. ft(Wc ), with
n
(2.28) and Qij = 0 wheneveri
~
j or (i,j) E S.
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Proof We prove the proposition by induction in a similar way as Proposition 2.3. The 3 x 3 case is straightforward to check. (Using (2.3), (2.8) and (2.9), we obtain that only the (1,3) entry of Q is nonzero, and equals G.) Consider an arbitrary generalized banded pattern S ~ n x n and assume that the proposition is true for all generalized banded patterns S which have S as a proper subset. The case S = (n. x n.)\{(I, n), (n, In reduces to the 3 x 3 problem. Let (io, jo) ¢ s, io < jo, be such that S = S u {( io, jo), (jo, io)} is also generalized banded. Let {Aij, (i,j) E S}, Fe, F, We and Vc be as in the statement of the proposition. Consider the partial matrix {Bij, (i,j) E S}, where Bij = Fij for (i,j) E S. Let Fe denote the central completion of this latter partial matrix. By the induction hypothesis,
n = W;QVc
(2.29) where nand
Q are
upper triangular with support outside the band
S,
n*
+n
R(We), and Fe = v.;Vc = We*We are lower-upper and upper-lower Cholesky factorizations of Fe. By Proposition 2.3 and the remark preceeding proof of Proposition 2.3 we have that R(v,,*) ~ R(v,,*) and R(We*) ~ R(W;). But this yields that there exists an upper triangular a and a lower triangular fJ such that Vc = aVc and We = fJWe. Now, taking QI = fJ*Qa we obtain from (2.29) that F - Fe, Q : R(Vc)
-+
(2.30) and clearly QI is upper triangular with support outside S. As in the proof of Proposition 2.3, Fe is also the central completion of the partial matrix {Cij,(i,j) E S}, where S = (n x n)\{(i,j),(j,i),1 :0:; i:O:; io,jo:O:; j :0:; n} and Cij = (Fe)ij for (i,j) E S. By the 3 x 3 case we may conclude that (2.31 ) where nand Q2 are upper triangular with support outside the band S, n* +n = F - Fe, Q2 : R(Vc) -+ R(We). Since F - Fe = (F - Fe) + (Fe - Fe), we have that = n + n, and thus (2.30) and (2.31) imply the desired relation (2.28) with Q = QI + Q2, which clearly is of the desired form. 0 We are now ready to prove the parametrization result. Proof of Theorem 2.2. Write Fe = C + C·, where C is upper triangular with C;; = 1/2F;;, i = 1, ... , n, and define for a contraction G = (Gij)~j=1 : R(We) -+ R(Vc) with G;j = 0 whenever i > j or (i,j) E S,
n
(2.32)
£(G)
=C -
W;(I + GU)-lGVc.
Since Uij 0 for (i,j) f/. S with i > j, one easily sees that GU is strictly upper triangular and so (I + GU)-l exists and is upper triangular. Since We" and Vc are both also upper triangular one readily obtains that (2.33)
(£(G));j
= C;j, (i,j) E S.
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Further, using (2.32) and the unitarity of U it is straightforward to check that C(G) + C( G)* = T( G). This together with (2.33) yields that T( G) is a completion of {Aij , (i, j) E S} and since IIGII ~ 1 the operator matrix T(G) is positive semi-definite. Assume that for two contractions G 1 and G 2 (of the required form) we have that T( Gd = T( G 2 ). Then also C( G1 ) = C( G 2 ) and since We* and are injective on R(We) and R(Vc), respectively, equation (2.32) implies that (I + G1U)-lG 1 = (I + G 2 U)-lG 2 • Thus G1(I + UG 2 ) = (I + G 1 U)G 2 which yields G1 = G 2 • Conversely, let F be an arbitrary positive semi-definite completion of {Aij, (i, j) E S}. Considedl = (Oij)7,j=l such that Oij = 0 wheneveri ~ j or (i,j) E S, and Fe-F = 0+0*. Then by Proposition 2.4 there exists an operator Q = (Qij)~ : R(We) -+ R(Vc) with Qij = 0 whenever i > j or (i,j) f/. Sand 0 = W;QVc. Since UQ is strictly upper triangular, we can define
v,;
G
= Q(I -
UQ)-l,
which will give that 0 = W;(I + GU)-lGVc. Since F = Fe - 0 - W, and taking into account (2.32) we obtain that F = T(G). Since F = T(G) is positive semi-definite, the relation (2.20) implies that G is a contraction. This finishes our proof. n 3. Contractive Completions. Consider the following 2 x 2 problem:
(3.1 ) where
Note that the contractivity of the latter operator matrices implies that
where G 1 and G 2 are contractions. It was proved in [2] and [9] that there exists a one-to-one correspondence between the set of all contractive completions of (3.1) and the set of all contractions G : V G, -+ VGj given by
(3.2) With the choice G = 0 we obtain the particular completion BI2 = -G 1 B~I G2 . We shall call this the central completion of (3.1). Let {Bij , 1 ~ j ~ i :5 n} be a n x n contractive triangle, i.e., let Bij : K j -+ Hi, 1 ~ j ~ i :5 n, be operators acting between Hilbert spaces with the property that
In order to make a contractive completion one can proceed as follows: choose a position (io,jo) with io = jo-l, and choose Bio.io such that (Bij)~io:j=l is the central completion
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of {Bij,i ~ io,j ~ jo} as in the 2 x 2 case. Proceed in the same way with the thus obtained partial matrix (some compressing of columns and rows is needed) until all positions are filled. We shall refer to Fc as the central completion of {Bii> (i,j) E T}. THEOREM 3.1. Let {Bij, 1 ~ j ~ i ~ n} be a contractive triangle. Let Fc denote the central completion of {Bij , 1 ~ j ~ i ~ n} and let ~c and \II c be upper and lower triangular operator matrices such that
(3.3) Further, let that
WI :
VFc
--+
ft( ~c) and W2 : V F;
--+
R(\II c) be unitary operator matrices so
(3.4) and put
(3.5) Then each contractive completion of {Bij, 1
~
j
~
i
~
n} is of the form
(3.6)
rt
where G = (GiJ"t-I : R(~c) --+ R(\IIc) is a contraction with G iJ" = 0 whenever (i,j) I,}_ T. Moreover, the correspondence between the set of all positive semi-definite completions and all such contractions G is one-to-one. Furthermore, S( G) is isometric (co-isometric, unitary) if and only if Gis. The decompositions of R(~c) and R(\II c) are simply given by
Proof We apply Theorem 2.2 using the correspondence (3.7)
(;.
~) ~ 0 if and only if IIBII ~ 1.
Consider the (n+n) x (n+n) positive semi-definite band which one obtains by embedding the contractive triangle {Bij, 1 ~ j ~ i ~ n} in a large matrix via (3.7). It is easy to check that when applying Theorem 2.2 on this (n + n) x (n + n) positive semi-definite band one obtains
(use Fc·DF; = DF;Fc). It follows now from Theorem 2.1 that (Tc)ij Further, it is easy to compute that
=
0 for i > j.
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where we have
and (3.10) We obtain the first part of the theorem from (3.8) and Theorem 2.2. From relation (3.9) one immediately sees that G is an isometry if and only if S(G) is. Similarly, one obtains from (3.10) that G is a co-isometry if and only if S(G) is. This proves the last statement in the theorem. 0 The existence of an isometric (co-isometric, unitary) completion is reduced to the existence of a strictly upper triangular isometry (co-isometry, unitary) acting between the closures of the ranges of iPe and We. Taking into account the specific structures of iP e and We one recovers the characterizations of existence of such completions given in [5] and [1] (see also [3]). REMARK 3.2. We can apply Theorem 2.1 to characterize the central completion. We first mention that for an arbitrary completion F of {Bij , 1 :::; j :::; i :::; n} one can define iP, Wand T analogously as in (3.3), (3.4), and (3.5). The equivalence of (i), (ii) and (iii) in Theorem 2.1 implies that the central completion is characterized by the maximality of diag(~iiiPi;)l'::l or diag(WiiWi;)i=l' This is a so-called "maximum entropy principle". From the equivalence of (i) and (iv) in Theorem 2.1 one also easily obtains that the uppertriangularity of T characterizes the central completion. 4. Linearly Constrained Contractive Completions. We return to the problem (1.2). The next lemma will reduce this linearly constrained contractive completion problem to a positive semi-definite completion problem. The lemma is a slight variation of an observation by D. Timotin [15]. LEMMA 4.1. Let B: 1i -+ IC, S : g -+ 1i and T : g -+ IC be linear operators acting between Hilbert spaces. Then IIBII :::; 1 and BS = T if and only if (4.1)
I S B*) ( S* S*S T*
~
O.
BTl
Proof. The operator matrix (4.1) is positive semi-definite if and only if
(4.2)
(S*) ( S*T S T*) I B (S B*)
=
(0
T _ BS
T* - S* B* ) 1- BB*
~
0,
and this latter inequality is satisfied if and only if IIBII :::; 1 and BS = T. 0 THEOREM 4.2. Let Bij : 1ij -+ lC i, 1 :::; i :::; j :::; n, Si : 1-{ -+ 1ii, i = 1, ... , nand Tj : 1i -+ ICj be given linear operators acting between Hilbe7't spaces and Sand T be as
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in (1.1). Then there exist contractive completions B of {Bij , 1 $ i $ j $ n} satisfying the linear constraint BS = T if and only if S*S - S(i)*S(i) T(i)* - S(i)*B(i)* ) 1- B(i)B(i)* ~0 T(i) _ B(i)S(i)
(
(4.3)
for i = 1, .. , n,where
Bli
(4.4)
B(i)
=
:
. . . BIn) : ,SCi) . ..
Bii
Bin
(
=
( Si ) S:n ,T(')
=
( TI )
:
T.
fori=I, ... ,n. Proof. By Lemma 4.1 there exists a contractive completion B of {Bij , 1 $ i $ j $ n} satisfying the linear constrained BS = T if and only if there exists a positive semi-definite completion of the partial matrix
(4.5)
I 0
0 I
0
?
0 S*2 BI2 B21
S*n BIn B 2n
?
?
Bnn
S*I Bll
0 0
I
Bil
?
Bi2
Bi2
Sn Bin S*S T*I I TI 0 T2
Bin T*2 0
SI S2
Tn
0
? ? B~n T*n
I
0 0
0
I
As it is known, the existence of a positive semi-definite completion of (4.5) is equivalent to the positive semi-definiteness of the principal submatl'ices of (4.5) formed with known entries. This latter condition is equivalent with (4.3). 0 Let us examine the 2 x 2 case a little further, i.e.,
(4.6) The necessary and sufficient conditions (4.3) for this case reduce to
(4.7) and
(4.8)
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Assume that (4.7) and (4.8) are satisfied. Similar to Section 3, let G 1 : 'HI -+ 'VBi2 and G 2 : 'VB12 -+ K2 be contractions such that (4.9) Any solution of the constrained problem (4.6) is in particular a solution of the unconstrained problem (the lower triangular analogue (3.1)), and therefore we must have that (use the analogue of (3.2))
(4.10) where r : 'Val -+ 'Va-2 is some _contraction. The equation B 21 S 1 + B 22 S 2 = T2 implies that r is uniquely defined on R(Dal Sd by (4.11)
We define ro : 'Val -+ 'Va; t.o be the contraction defined on n(DalSd as above, and 0 on the orthogonal complement, i.e.,
ro I 'Val e n(DalSd = 0
(4.12)
We let B~~) denote the corresponding choice for B 21 , that is, (4.13) We shall refer to
B12) ( BBn (O) B 21 22
(4.14)
as the central completion of problem (4.6). In the n x n problem (1.2) (assuming conditions (4.3) are met) we construct step by step the central completion of (1.2) as follows. Start by making the central completion of the 2 x 2 problem
~:
B12 ... Bin) ( ) ( Bn ? B22 ... B 2n : Sn
(4.15)
=(
T1 ) T2
and obtain in this way B~~). Continue by induction and obtain at step p, 1 ::; p ::; n - 1, B~~), . .. ,B~?J-1 by taking the central completion of the 2 x 2 problem
B1,,,-1 ( (4.16)
Bu B (0) _
1' 1,,, ?
.
B(O)
B 1"
.1'-1,1'-1 B"-l,,, ? B,,1'
~.
i·
)
Sl S,,-l S1' S"
~
(i, ).
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The final "result Bo of this process is the central completion of the problem (1.2). LEMMA 4.3. Let Bo be a contractive completion of (1.2). Then Bo is the central completion of (1.2) if and only if (4.17)
( I*
S
BO)
S*S T* I Bo T
is the central completion of the positive semi-definite completion problem (4.5). Proof. By the inheritance principle and the way the central completion is defined it suffices to prove the lemma in the 2 x 2 case. Take an arbitrary contractive completion B of (4.6), corresponding to the parameter r in (4.10), say. The lower-upper Cholesky factorization of the corresponding positive semi-definite completion problem is given by
S
B* )
S*S T* T I
(4.18)
,
where (4.19)
V
=
I S B*) ( 0 0 0 o 0 cpo
and cP is lower triangular such that 1- BB* (4.20)
= CPCP·.
It is straightforward to check that
0) .
cP = (DBi.DGj -G2 B12DGj - DG' rGi DG' Dr.
Since for r = ro the operator D¥-. is maximal among all r satisfying (4.11), the lemma follows from the equivalence of (i) and (ii) in Theorem 2.1. 0 THEOREM 4.4. Let Bo be the central completion of the linearly constrained contractive completion problem (1.2) (for which the conditions (4.3) are satisfied). Let p : 'HI (f] 'H2 - n«s* S - T*T)I/2) be such that (4.21)
and Wand cP lower triangulars such that (4.22)
W*W = I - pOp -
B~Bo
and (4.23)
Consider the contraction WI : VBo - 'R.( w) and the unitary W2 : 'R.( cp.) - VB. with the properties (4.24)
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and
(4.25) Finally, define
(4.26) Then there exists an one-to-one correspondence between the set of all contractive solutions of the problem (1.2) and the set of all strictly lower triangular contractions G: R.(III) -+ R.(~*) given by (4.27)
V(G)
= Bo -
~(I
+ Grt 1 GIII
Moreover, V (G) is a co-isometry if and only if G is a co-isometry and V (G) is an isometry if and only if S* S = T*T and G is an isometry. The decompositions of R.(~*) and R.(III) are simply given by
R.(~*)
= ffii'=1 R.(~:i)' R.(III) = ffii'=1 R.(lIIii).
Proof. We shall obtain our results by applying Theorem 2.2 for the positive semidefinite completion problem (4.5). Straightforward computation yield that
Vc=
(4.28)
( 0IS0 Bo) 0 o
0
~*
and (S* S - o T*T)I/2 T
(4.29)
o~ )
We remark here that the relation (4.30)
S* S - T*T
= S* D2Bo S > S* D4Bo S -
gives the existence of the contraction p with (4.21). Now we have to determine the unitary U = (Uij)~,j=1 so that UWc = Vc. Note that the existence of WI and W2 is assured by the relations (4.22) and (4.23). An immediate computation shows that
U= ( .umtary . ·h h were WI IS WIt ( WI)
111* 0
p*
-w;BoWj
-w;Bowj
o
Bo) 0 ~*
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Bakonyi and Woerdeman
Substituting these data in the first equality of (2.20) gives
(4.31 )
T( (
OOG*) 0 0 0 o0 0
)=
(I
S V(G)* ) , S*S T* V(G) T Q(G) ~
where V( G) is given by (4.27) and (4.32)
1= Q(G)
= V(G)V(G)* + ~(I + Gr)-I(I -
GG*)(I + Gr)*-I~*
The first part of the theorem now follows from (4.31) and Lemma 4.1. Further, (4.32) implies that V(G) is a co-isometry if and only if Gis. If the contractive solution V(G) to the constrained problem (1.2) is isometric, then clearly we must have that S* S = T*T and thus p = O. In this case, 111
0 0) .
Wc= ( 0 00 Eo T I
(4.33)
Using the second inequality in (2.20) in this special case, we obtain that 0 0
T( ( 0 0
(4.34)
o
0
G* )
o )= o
S V(G)* ) ( Q(G) T* S* S*S I V(G) T
where (4.35)
1= Q(G)
= V(G)*V(G) + 111*(1 + Gr)-I(1 -
G*G)(I + Gr)*-IIII.
Relation (4.35) implies that when S*S = T*T, the spaces VV(G) and VG have the same dimensions and thus V(G) is isometric if and only if G is. This finishes the proof. 0 In the 2 x 2 case another parametrization was derived in [4]. REMARK 4.5. By Theorem 4.4 we can reduce the existence of a co-isometric completion of the problem (1.2) to the existence of a strictly lower triangular co-isometry acting between R(III) and R(~·). Also, when S*S = T*T, the existence of a isometric completion of the problem (1.2) reduces to the existence of a strictly lower triangular isometry acting between R(III) and R( ~*). REMARK 4.6. There exists a unique solution to (1.2) if and only if 0 is the only strictly lower triangular contraction acting R( 111) --+ R( ~*). This can be translated in the following. If io denotes the minimal index for which lIIioio =I 0, then there exists a unique solution if and only if ~kk = 0 for k = io + 1, ... , n. REMARK 4.7. As in Remark 3.2 the upper triangularity of r characterizes the central completion. For this one can simply use Theorem 2.1 and Lemma 4.3. Also the maximality of diag(~ii~ii)f=I or diag(lIIiillli;)f=I characterizes the central completion (a maximum entropy principle). For a different analysis in the 2 x 2 case we refer to [4] ..
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REFERENCES [1) Gr. Arsene, Z. Ceau§escu, and T. Constantinescu. Schur Analysis of Some Completion Problems. Linear Algebra and its Applications. 109: 1-36, 1988. (2) Gr. Arsene and A. Gheondea. Completing Matrix Contractions. J. Operator Theory. 7: 179-189, 1982. (3) M. Bakonyi and H.J. Woerdeman. Positive Semi-Definite and Contractive Completions of Operator Matrices, submitted. (4) M. Bakonyi and H.J. Woerdeman. On the Strong Parrott Completion Problem, to appear in Proceedings of the AMS. (5) J .A. Ball and I. Gohberg. Classification of Shift Invariant Subspaces of Matrices With Hermitian Form and Completion of Matrices. Operator Theory: Adv. Appl. 19: 23-85, 1986. (6) J.P. Burg, Maximum Entropy Spectral Analysis, Doctoral Dissertation, Department of Geophysics, Stanford University, 1975. (7) T. Constantinescu, A Schur Analysis of Positive Block Matrices. in: I. Schur Methods in Operator Theory and Signal Processing (Ed. I. Gohberg). Operator Theory: Advances and Applications 18, Birkhauser Verlag, 1986, 191-206. (8) H. Dym and I. Gohberg. Extensions of Band Matrices with Band Inverses. Linear Algebra Appl. 36: 1-24, 1981. (9) C. Davis, W.M. Kahan, and H.F. Weinberger. Norm Preserving Dilations and Their Applications to Optimal Error Bounds. SIAM J. Numer. Anal. 19: 444-469, 1982. (10) C. Foias and A. E. Frazho. The Commutant Lifting Approach to Interpolation Problems. Operator Theory: Advances and Applications, Vol. 44. Birkhauser, 1990. (11) C. Foias and A. Tannenbaum. A Strong Parrott Theorem. Proceedings of the AMS 106: 777-784, 1989. (12) I. Gohberg, M. A. Kaashoek and H. J. Woerdeman. The Band Method For Positive and Contractive Extension Problems. J. Operator Theory 22: 109-155,1989. (13) I. Gohberg, M. A. Kaashoek and H. J. Woerdeman. The Band Method For Positive and Contractive Extension Problems: an Alternative Version and New Applications. Integral Equations Operator Theory 12: 343-382, 1989. . (14) I. Gohberg, M. A. Kaashoek and H. J. Woerdeman. A Maximum Entropy Priciple in the General Framework of the Band Method. J. Funct. Anal. 95: 231-254, 1991. (15) D. Timotin, A Note on Parrott's Strong Theorem, preprint.
Department of Mathematics The College of William and Mary Williamsburg, Virginia 23187-8795
MSC: Primary 47 A20, Secondary 47 A65
96
Operator Theory: Advances and Applications, Vol. 59 © 1992 Birkhauser Verlag Basel
INTERPOLATION BY RATIONAL MATRIX FUNCTIONS AND STABILITY OF FEEDBACK SYSTEMS: THE 4-BLOCK CASE
Joseph A. Ball and Marek Rakowski
Abstract. We consider the problem of constructing rational matrix functions which satisfy a set of finite order directional interpolation conditions on the left and right, as well as a collection of infinite order directional interpolation conditions on both sides. We set down consistency requirements for solutions to exist as well as a normalization procedure to make the conditions independent, and show how the general standard problem of Hoo control fits into this framework. We also solve an inverse problem: given an admissible set of interpolation conditions, we characterize the collection of plants for which the associated Hoo-control problem is equivalent to the prescribed interpolation problem. Key words: Lumped and generic interpolation, homogeneous interpolation problem, stabilizing compensators, 4-block problem, HOO control.
Introduction The tangential (also called directional) interpolation problem for rational matrix functions (with or without an additional norm constraint) has attracted a lot of interest in the past few years (see [ABDS, BGRI-6, BH, BRan, D, FF, Ki]); much of this work was spurred on by the connections with the original frequency domain approach to Hoo-control theory (see [BGR4, BGR5, DGKF,
Fr, Ki, V]). The simplest case of the interpolation problem is of the following sort. We are given points
Zl, ••• ,ZM
in some subset u of the complex plane
and 1 X n row vectors 111,' .. ,11M and seek a rational m
ee, nonzero 1 X m row vectors Xl, ••• ,XM X
n matrix function W( z) analytic on u
which satisfies
(0.1)
X.W(zt)
= 11.,
i
= 1,,,, ,M.
In the two-sided version of the problem, we are given additional points
n X 1 column vectors
1.11, ••• ,UN
and m X 1 column vectors VI, •••
,VN
WI,' •• ,WN
in u, nonzero
and demand in addition that
W satisfy
(9·2)
W(Wj)Uj
= Vj,
If for some pair of indices (i, j) it happens that zt
j
= 1,,,, ,N.
= Wj, in applications a third type of interpolation
condition arises (0.3)
Z.W'({ij)Uj = Pi; whenever zt =
Wj
=: {ij
Ball and Rakowski
and where
and
r
Pij
97
is a given number. By introducing matrices
= hijh~i~M.l~j~N where "Yij
={
Pij (Wi - Zj)-lZiUj
if Zi = Wj if Zi '" Wj
the conditions (0.1)-(0.3) can be written in the streamlined compact form
(0.1') zoEa'
(0.2') ..DE ..
LRes..=..o(z - Ad-1 B+W(z)C_(z - A"yl
(0.3')
=r
ZoED'
where Res ..= ..oX(z) is the residue of the meromorphic matrix function X(z) at zoo Interpolation conditions of higher multiplicity can be encoded by allowing the matrices A, and A". to have a more general Jordan form. This is the formalism developed in [BGR4). If (T is either the unit disk or the right half plane, one can also consider the problem with an additional norm constraint
sup IIW(z)1I < 1
(0.4)
..E..
to arrive at a matrix version of the classical Nevanlinna-Pick or Hermite-Fejer interpolation problem. In [BGR4) a systematic analysis of the problem (0.1')-(0.3'), with or without the norm constraint (0.4), is presented, including realization formulas (in the sense of systems theory) for the set of all solutions. In [BR5), in addition to the
1Jl.mJu:d interpolation conditions (0.1)-(0.3) or (0.1 ')-(0.3')
there was imposed a generic (or infinite order) interpolation condition
(P+ W)(i)(zo) for some
(0.5)
zo E
(T,
= p~)(zo) for j = 0,1,2""
or equivalently
P+(z)W(z)
= P_(z) for all z,
98
Ball and Rakowski
where P+ and P_ are given polynomial matrices of respective sizes K x m and K x n.
In
[BR5) the theory developed in [BGR4) for the problem (0.1')-(0.3') was extended to handle the
problem (0.1 ')-(0.3') together with (0.5) (with or without the additional norm constraint (0.4», with the exception of the explicit realization formulas for the linear fractional parametrization of the set of all solutions. The features obtained include: an admissibility criterion for data sets
(C+, C_, A,.., A" B+, B_, r, P+(z), P_(z» which guarantees consistency and minimizes redundancy in the set of interpolation conditions (0.1 ')-(0.3') and (0.5), reduction of the construction of the linear fractional parametrizer of the set of all solutions to the solution of a related homogeneous interpolation problem, and a constructive procedure for solving this latter homogeneous interpolation problem. The associated homogeneous interpolation problem is of the following form. In general, we let 'R denote the field of rational functions and 'Rmxn denotes the set of m x n matrices over 'R
w
= (C+, C_, A,.., A"
B+, B_, r, P+(z), P_(z» we construct an 'R(u)-module S C 'R(m+n)xl given
by
S
= {[ g~] (z -
A,.. )-lx + [~~~;n
:x E
h+ E 'Rmxl(u),L E 'RnXl(u) such that
L Resz=zo(z -
Ac}-l[B+ B_)
[~~~;n
= rx}
ZoED'
n{r E 'R(m+n)xl : [P+(z) P_(z»)r(z) = o}.
(0.6)
Then the module form of the homogeneous interpolation problem is to find a rational (m + n) x (m - K
+ n) matrix function 9( z) such that
(0.7) More concretely, the condition (0.7) can be viewed as prescribing the zeros and poles of 9 on u (including partial multiplicities) from the local Smith form together with some additional directional information, as well as prescribing a left kernel polynomial for 9. H the norm constraint (0.4) is also part of the original (nonhomogeneous) interpolation problem, then 9 is required to satisfy
additional conditions
(0.8a)
9(z)*(Im ED -I.. )9(z)
= Im-K ED -I.. for z e {Ju
Ball and Rakowski
99
and
9(z)*(Im E9 -In)9(z) :5 Im-K E9 -In for z E 0'.
(0.8b)
The linear fractional parametrization of the set of all solutions takes the form
(0.9) where Ql E 'R(m-K)xn(O') and Q2 E 'Rnxn(O') are appropriate parameters, and where 9
= [:~~ :~~] with 9 11 E 'Rmx(m-K).
For more complete details we refer to [BR5]. The purpose ofthis paper is to consider the interpolation problem (0.1 ')-(0.3') and (0.5) with an additional right generic interpolation condition
(0.10) where Q_ and Q+ are given matrix polynomials of respective sizes n x Land m x L. Here we obtain a canonical extension of all the results in [BR5] to handle the additional interpolation condition (0.10). In this more general setting the relevant analogue of Sin (0.6) is the 'R(O')-module S C 'R(m+n)xl given by
(0.11) where S is given by (0.6). The associated homogeneous interpolation problem is to find a rational (m + n) x (m - K
(0.12)
+ n) matrix function 9
such that
_ _ [1l(m-K+n-L)Xl(O')] S - 9 1lLx1 .
If the norm constraint (0.4) is included in the original interpolation problem, then 9 is also required to satisfy
= Im-K E9 -In for z E 80'
(O.13a)
9(z)*(Im E9 -In)9(z)
(O.13b)
9(z)*(Im E9 -In)9(z) :5 Im-K E9 -In-L E9 0 for z
e CT.
100
Ball and Rakowski
and the linear fractional parametrization has the degenerate form
W
= [0 n Q1 + 0 12Q2 0 13 ][021Q1 + 0 22 Q2 0 23 t 1
where Q1 E 'R(m-K)x(n-L)(O') and Q2 E 'R(n-L)x(n-L)(O') are appropriate parameters and where
9 = [00 n21
0 12 0 13 ] with 0 11 E 'Rmx(m-K) and 0 12 E 'Rmx(n-L). 0 22 0 23 In addition we show here how the standard problem of BOO control theory (see [Fr]) fits
into this framework; this also extends the work in [BRS] to incorporate the extra condition (0.10). Specifically, given a rational matrix function P =
[~~: ~~~]
representing the plant for an BOO
problem, we show that the set of interpolation conditions (0.1 ')-(0.3'), (0.5), (0.10) are satisfied by the closed loop transfer function Pn
+ P12K(I -
P22K)-lP21 if and only if the closed loop
system with compensator K is internally stable. The characterization is in terms of null-pole data of a related matrix function
P (a partial inversion
or chain formalism transform of P). For the
case considered here the more general chain formalism transform introduced in [BHV] is required. We also solve an inverse problem of describing which plants are associated with a prescribed set of interpolation conditions, and thereby establish an equivalence between interpolation and feedback stabilization. It turns out that the set of interpolation conditions (0.1 ')-(0.3') corresponds to the 1block case, the set (0.1 ')-(0.3'), (0.5) corresponds to the 2-block case, and the general interpolation problem (0.1 ')-(0.3'), (0.5), (0.10) corresponds to the general 4-block case in the BOO theory. A significant limitation of the interpolation approach in the early development of the BOO theory was the lack of an interpolation theory incorporating generic interpolation conditions (0.5) and (0.10) in addition of (0.1 ')-(0.3') (but see [Hu]). Part of the motivation of [BR5] and this paper is to
address this situation. The paper is organized as follows. Section 1 recalls preliminaries concerning null-pole structure from [BGR4] and [BR1]-[BR3] which will be needed in the sequel. Section 2 formulates and solves the homogeneous interpolation problem ofthe type (0.12). Section 3 sorts out admissibility conditions on an interpolation data set (C+, C_, A".,A(, B+, B_, r, P+(z), P_(z), Q+(z),Q_(z» to guarantee consistency and minimize redundancy. In Section 4 we obtain the linear fractional parametrization for the set of all solutions and Section 5 delineates the connection with the BOO_ control theory. 1. preliminaries.
In this paper, we will use the concepts of the null-pole structure of a rational matrix
function W over a fixed subset
0'
of the complex plane 0::. They have been developed for a regular
rational matrix function (that is, a rational matrix function which is square and whose determinant does not vanish identically) in [BGRl]-[BGR3]; for a comprehensive treatment see [BGR4]. These concepts have been generalized to an arbitrary rational matrix function in [BRl]-[BR3] (see also [BR4]). We recall now the basic definitions and facts which will be used later.
101
Ball and Rakowski
Let 'R denote the field of scalar rational functions, and let 'R(O') be the subring of'R formed by functions analytic on 0'. Let 'Rmx ,. denote the space of m x n rational matrix functions, and let 'Rmxn(O') be the subspace of'Rmxn formed by functions analytic on An observable pair of matrices (C"., A".) of sizes m to be a ri,ht pole pajr for W over
(i) O'(A".) C
0'
X n".
and n..
0'.
X n".,
respectively, is said
if
0',
(ti) for every x E o:nwxl there exists
C".(z - A".)-lx - W(z)
(1.1)
(iii) for every
= D+C(z-A)-l B for W(z)j this is discussed
in [BR5]. For a more complete discussion, see [BGK] or [BGR4]. To discuss null or zero structure in the nonregular case, we need to introduce a definition. We define a real non-archimedean valuation
Irlz=.\
1•
={
Iz=.\ of'R by putting 0, e,-'I
if r = 0 if r '" 0
where 1/ is such that r(z) = (z-A)'If(z) with f(z) analytic and nonzero at A. If x 'Rn, where 'Rn can be identified with 'Rnx1 or 'R1X ,., let
= (Xl. X2,··· , xn) E
('Rn, II . IIz=.\) is a non-Archimedean nQrmed vector space over the real valued field ('R,I . Iz='\). Subspaces A and
n of ('Rn, 1I·llz=.\) are said to be orthogonal (see [M]) if
(1.2) for all x E A and y
= n.
We say that subspaces A and
holds for all x E A, yEn, A E 0'.
if (2.2) n We say that an element x of'R is orthogonal to a subspace of n
if'Rx is orthogonal to n (resp. to 'Ry) on 0'. of subspaces n and A of'Rn has a straightforward cHaracterization
of ~n (resp. an element y E 'Rn) on The orthogonality on
0'
n of 'Rn are orthogonal on 0' C ct
0'
in terms of linear algebra. Let n(A) (resp. A(A)) denote the subspace of ctn formed by the values at A of those functions in orthogonal on
0'
n which are analytic at A.
By Proposition 2.3 in [BR2],
if and only if n(A) n A(A)
= (0)
n and A are
102
Ban and Rakowski
for each A E (J. Let WE
n mxn , and let wo l
denote the left kernel of W, that is
w ol = {ip E nIxm : ipW = O}. A controllable pair of matrices (A" Be) of sizes
n, x n, n, x and
m, respectively, is said to be a
left null pair for W over (J (see [BR2]) if
(i) (J(Ae) C (J, (ii) for each x E (£IXnc the function x(z - Ae)-I B, is orthogonal to
wol on (J(Ae),
(iii) the function (z-Ae)-I B(W(z)h(z) is analytic on (J whenever hE nnXI((J) and W(z)h(z) is analytic on (J, (iv) the size of A, is maximal subject to the above conditions. A left null pair can be related to a canonical set of left null chains or left null functions for W(z) over (J (see [BR2] , [BR3] for the nonregular case, [BGK], [BGR4] for the regular case) and to a piece of a realization WX(z) = Dt - DtC(z - A + BDtC)-1 BDt for a generalized inverse WX(z) for W(z) (see [BCRR], [R] for the nonregular case and [BGK], [BGR4] for the regular case). Complete information regarding left null-pole structure of WE nmxn over (J is given by the null-pole subspace
An indication of this statement is that the null-pole subspace is a complete invariant for right equivalence over W; more precisely, two rational m x n matrix functions (assumed for simplicity to have trivial right annhilators) WI and W 2 are related by WI = W 2 Q where Q is analytic with nonsingular values on (J if and only if Su(Wt)
= Su(W2 ).
Let (C"., A".) be a right pole pair and let (A(, Be) be a left null pair for a function W E nffixn. Then there exists a unique matrix
(1.3) S .. (W)
= (WnnXI) n {C".(z -
r
(see [BR3]) such that
A".)-IX + h(z): x E (£n.xt,h E nmXI((J) and
L Resz=zo(z -
Ae)-I B(h(z) = rx}
zoEO'
The matrix
r
is called the coup1ing matrix associated with the right pole pair (C"., A".) and a left
null pair (A" Be) for W over (J. The triple
(1.4) is called a left D1!1I-pole triple for W over (J or a left a-spectral triple of W. More detailed motivation for these concepts and connections with more established notions in systems theory can be found in [BGR1] and [BGR4] for the regular case and [BRS] for the nonregular case.
103
Ball and Rakowski
Let W E 'R,.mxn. Any matrix polynomial P,. whose rows form a minimal polynomial basis for
wol
(see [F]) is said to be a left kernel polynomial for W. The following proposition
characterizes matrix polynomials P,. and data sets w arising as a left kernel polynomial and a left u-spectral triple for some rational matrix function. PROPOSITION
1.1. (cf. Proposition 4.1 in [BR2] and Theorem 3.1 in [BR3]) Let W E 'R,.mxn be a
function with a left kernel polynomial P,. and left u-spectral triple w as in (1.4). Then wand P,. satisfy the following conditions: (NPDSi) the pair (C"., A".) is observable and u(A".) C u,
Cd is controllable and u(Ad C u, A,r = B,c".,
(NPDSii) the pair (A"
(NPDSiii) rA". (NPDSiv) P,. has no zeros in CC and the leading coefficients of the rows of P,. are HnearIy independent, (NPDSv) the function P,.(z)C".(z - A".)-l is analytic on ct, (NPDSvi) if u(Ac)
= {AI! .x 2 , · · · ,.xr }, where the points .x}, .x 2 , · · · ,.xr are distinct, A, (
.xlI
.x2I
then the pair
1 [p,.(i
l) ) , P,.(.x2)
...
..
.xrI
P,.(.xr)
is controllable. Conversely, if {C.", A.", A" B" r} is a collection of matrices and P" is a matrix polynomial such that (NPDSi)-(NPDSvi) hold, then there exists a rational matrix function W with a left uspectral triple w as in (1.4) and with a left kernel polynomial equal to P". The construction of such a function W is indicated in [BR2] (see also Section 6 in [BRa]). Given a matrix polynomial P" and a triple w
r), where C.", A"., A" B"
r
= « c.", A.,,), (A"
B,), are matrices of appropriate sizes, we may associate with wand P,. a
linear space
(1.5) StreW, P,,)
= {h E 'R,.mXI : P"h = O} n {C,,(z -
A.,,)-lx + h(z}: x E ctn.xt, hE 'R,.mXI(u) and
E Resz=zo(z - Ad- B,h(z) = rx}. l
ZoEtr
It follows from formulas (1.3) and (1.5) that if w is a left u-spectral triple and P" is a left kernel polynomial for a function W E 'R,.mxn, then StreW, P,,} = StreW}. We will use the notation StreW, p .. ) and StreW} interchangeably. We shall refer to the collection (w, P,.) = (C.", A", A" B" a complete (left) nun-pole data set for W over u.
r, P,,(z}) as
104
Ball and Rakowski
2. A homogeneous interpolation problem. In the previous section we saw that a complete null-pole data set (w, P,.) over
q
for
a rational matrix function W is a useful set of invariants for describing the null-pole subspace S... (W)
= W1lnXl(q) associated with W.
However, for the 4-block interpolation problem, a more
general submodule of 1lm arises in a natural way. Specifically, assume that W in 1lmxn has a block row decomposition W 1l(q)-submodule of 1lmx1
= [WI
W 2 ] with WI E '7l mx (n-lc) and W 2 E '7lmxlc, and consider the
(2.1) We refer to S... (Wh W2 ) as the extended null-pole sub§Pace associated with the block row matrix function [WI W 2 ] over q. For our applications [WI W 2] has trivial right annhilator in 1lnxl, i.e., the columns of [WI W2] are linearly independent over 1l. Hence we make the assumption on W
= [WI
W 2] that the decomposition in (2.1) is direct. Note that we can recover W 21l1cx1 from
S...(W1, W2) as W21llcX1
=
nrS...
(Wh W2)
rE'R
The submodule W 11l(n-lc)xl(q) is not as uniquely deterlnined by S.. (Wh W 2); all one can say is that it is a direct sum complement to
n rS..(Wh W2) inside the 1l(q)- submodule S.. (Wh W 2).
rE'R
In any case the direct sum decomposition of S.. (W1 , W2 ) can be viewed as an affine version of the Wold decomposition for an isometric operator on a Hilbert space (see [NFl). From another point of view, note that S.. (Wf, W~)
= S.. (Wh W 2) if and only if [Wf
W~] = [WI W2] [ ~ ~] = [WIF + W 2 G
W2H]
where F and F-l are in '7l(n-lc)x(n-Ic)(q), G E '7l Icx (n-lc) and H and H-l are in '7l1cxlc . Indeed, to see this, note that both
map 1l(n-lc)xl(q) E91l1cx1 onto itself, and conversely, any multiplier in 1l"xn with this property necessarily must be ofthe form
[~ ~]
with p±l E '7l(n-lc) x(n-Ic)( q), G E '7l Icx (n-Ic), H±l E '7l1cxlc .
In particular we may always choose H so that the columns of W~ basis for their span, namely,
= W2H form a lninima.l polynolnia.l
n rS..(WI, W2). Note that the zeros and poles of Wf = W1F + W. 2 G re'R
can be quite different from those of WI; the invariant is the left zero-pole structure in a subspace
Ball and Rakowski
105
complementary to the 1l-span of the columns of W2 • We may always choose G E 1lA:x(n-/c) so that the span of the columns of W{ = WI + W 2G is orthogonal over the set of zeros and poles of W{ to the span of the columns of W2 (or, equivalently, of W~). Let us call any u-spectral triple
w = «C"., A".), (A" Bd,r) for W{ obtained from the pair (WI ,W2 ) in this way a W2-normalized left u-spectral triple for WI. The 1l-span of S,,(WI. W 2), U rS,,(WI. W 2 ) = [WI W 2 ]1lnxI , can rE'R
be specified via a left kernel polynomial P,. for the function [WI W 2 ]. Given a block row matrix function W
= [WI
W 2 ], we have now introduced (1) a W2-normalized left u-spectral triple w for WI. (2) a left kernel polynomial P,. for [WI W 2] and (3) a polynomial matrix Q E 1lmxL whose columns form a minimal polynomial basis for the 1l-span of the columns of W2 • Let us call the whole collection (w, P,., Q) a complete extended null-pole data set for W
= [ WI W2 ].
The analysis
above shows that two block row matrix functions [WI W 2] and [W{ W~] for which the associated extended null-pole subspaces are the same (Su(W{,
W~)
= Su(WI. W 2)) share the same complete
extended null-pole data sets. Moreover, we can recover the extended null-pole subspace Su(WI. W2) from the data set via the formula
({f E 1lmxI : P,.! = O}n {C".(z - A".)-I x + h(z): x E o:n.xI and h E 1lmXI(u) such that
E Resz=zo(z- Ac)-IB,h(z) = rx}) + Q1lA:xI
(2.2)
zoE"
For our application to interpolation problems in Section 4, we need to understand the inverse problem, namely: which data sets (w, P,., Q) arise as the extended complete null-pole data set over
u of a block row W
= [WI
W2] E 1lmxn. We view this problem as a homogeneous interpolation
problem. The answer is given by the following result.
THEOREM
= «C"., A".), (A"Bc), r» is the extended complete W = [WI W 2] E 1lmxn (where WI E 1lmx(n-/c) and
2.1. Suppose (w,P,.,Q) (where w
null-pole data set for a block row function
W 2 E 1lmx/c). Then the data set (w, P,., Q) satisfies the following conditions: (NPDSi) the pair (C".,A".) is observable and u(A".) C u, (NPDSii) (NPDSiii) (NPDSiv) (NPDSv)
the pair (4" Bd is controllable and u(Ad C u, rA". - A,~= B,C".,
P,. has no zeros in 0: and the leading coefficients of the rows of P,. are linearly independent, the function P,.(z)C".(z - A ... )-l is analytic on 0:,
(NPDSvi) if u(Ad
= {Ah ~2"
•• , ~r}'
where the points ~h ~2' ••• ~r are distinct, then the pair
106
Ball and Rakowski
is controllable. (NPDSvii) Q has no zeros in 0: and the leading coefIicients of the columns ofQ are linearly independent
(NPDSviii) the function (z - Ad- l B,Q(z) is analytic on 0: (NPDSix) if u(A,..)
= {wt, W2,··· , w
(Ie.
6 },
then the pair
Q(w,) Q(",,) ... Q(w.)l.
[A.
is observable;
J)
=
(NPDSx) P,.Q o. Conversely, if {C,.., A,.., A"B" r} is a collection of matrices and P,. and Q are matrix polynomials such that conditions (NPDSi) - (NPDSx) hold, then there is a block row matrix function W
= [WI W2] E 'Rmxn such that (w, P,., Q) is an extended complete null-pole data set for
W overu. REMARK.
Note that there is some redundancy in the conditions (NPDSi) - (NPDSx). In particular
(NPDSvi) implies the first part of (NPDSii) and (NPDSix) implies the first part of (NPDSi). Nevertheless, we list them in this form to make the connections with the I-block case (NPDSi) (NPDSiii) and the 2-block case (NPDSi) - (NPDSvi) clear. PROOF:
To prove the first statement, we note that condition (NPDSvii) follows from Proposition
3.18 in [BR2], and condition (NPDSix) follows from the fact that Q is analytic on 0: and the column spans of WI and Q are orthogonal on u. We give now the constructive proof of the second statement. The construction is a modification of the construction in [BR2] (see also Section 6 in
[BRa]). Let {C,.., A ... , A" B" r} be a collection of matrices and let P,. and Q be matrix polynomials such that conditions (NPDSi) - (NPDSx) hold. Step 1 Using the results from [GK], find a regular rational matrix function H with the u-spectral
«C. .
=
= ,A,..),(A"Bc),r). Find a Smith-McMillan factorization EDF of H and set WI ED. Step 2 Let v be the largest geometric multiplicity of a pole of H in u, let p. be the largest geometric multiplicity of a zero of H in u, and let '7 be the largest sum of the geometric multiplicity of a pole
triple w
107
Ball and Rakowski
and the geometric multiplicty of a zero of H at any single point of 0'. Let di denote the ith diagonal entry of D. For i = 7] - P. + 1,7] - P. + 2, ... , v, let P; be the minimal degree monic polynomial such that if dm-'I+i has a zero point
~
E
of order k then Pidi has a zero at
0'
~
of order k. Define an
m X 7] matrix polynomial Q = [%1 by
I, ifi=j$7]-p. { Pi, if7]-p.
m-p. 0, otherwise, and put
Step 3 For i = 1, 2, ... , p., let
a point
~
E
0'
4>; be the (m -
functions for H
at~.
i - I )th row of E-l, so that if H has a zero at
{4>1, 4>2, ... ,4>,.} is a canonical set of left null Note that the left null pair constructed from the functions 4>t. ... ,4>/J is
of the geometric multiplicity
then
K.
left-similar to the pair (A" Be). We may, in fact, assume that both pairs are equal. Modify the functions
4>10 4>2, ... ,4>/J as follows. Suppose that O'(A,..) U O'(Ad = {At. ~2,··· , ~.} and the largest
multiplicity of a zero of H in
0'
multiplicity of a zero of H at
~;
is p., and consider the point be
K..
~i
(i = 1, 2, ... , s). Let the geometric
By condition (NPDSvi), the matrix
Ai
=
[~~~:~l 4>/J(~i)
P"(~i)
has full row rank. By conditions (NPDSviii) and (NPDSx), geometric multiplicity of a zero of H in
0',
there is a point
~
AiQ(~;)
=
o.
Since p. is the largest
such that the matrix
A= 4>/J(~) P,.(~)
has full row rank and AQ( ~) = O. Hence we can add to
4>; (j = K. + 1, K. + 2, ... , p.) a function
p(z)c,
where c is a vector and p(z) is a scalar polynomial vanishing at ~t. ~2' .•• ,~. to the order p., so that the modified 4>K+l, 4>,,+2, ••• ,4>/J (which are again called 4>,,+1, ••• ,4>/J) are such that the matrix
Ball and Rakowski
108
Hi=
4>"(.~i)
P,,(Ai)
has full row rank and HiQ( Ai)
= O.
In this manner we obtain functions 4>1,4>2,· .• ,4>,. whose span
is orthogonal to the row span of P" on q( A".) U q( A,) and such that the function
+(z)
=
[~1;ll
Q(z)
4>,.(z) vanishes on q(A".) U q(Ad. Now it follows from the construction and condition (NPDSvili) that if
4>i is a left null function for H at AI. A2,··· ,A. of orders h, 12, ... ,I., then 4>i(Z)Q(Z) vanishes at Ai to the order at least kj where kj
~
max{l,li}. Suppose ki
4>i(Z)Q(Z)
= (.Ii (z 3=1
< 00. By condition (NPDSvii),
Ai)k;)Vi(Z)Q(Z)
= ~i(Z)Q(Z). where Vi is analytic, and does not vanish, at AI, A2, ... ,A•.
Let,pi
= 4>i -
~i (i
= 1,2,··· ,1-').
Then the set {,p1o,p2,··· ,,p,.} contains a canonical set ofleft
null functions for H at each zero of H in span of P" on q(A".) U q(Ad, and ,piQ
q,
the span of {,pI, ,p2, ... ,,p,.} is orthogonal to the row
= 0 (i = 1,2,··· ,1-').
Extend the span of {,p1o ,p2, ... ,,p,.} to an orthogonal complement B of the row span of
P" in (Qol, q(A".) U q(A,», and project each column of W 2 onto an orthogonal complement of the row span of Q in
(P~T,
q( A".) U q( A,» along BOT
+ {column span of Q}
to get W3 •
Step 4 Multiply W3 on the right by a regular rational matrix function without poles or zeros in
q(A".) U q(Ad, so that the resulting function W4 has no zeros nor poles in q \ (q(A".) U q(Ad). Step 5 Find a minimal polynomial basis column span of [W4 Q] in
(P~T,
{UIo U2, .••
,uT } for an orthogonal complement of the
q(A".) U q(Ad). Set
The extended null-pole subspace S,,(w, p .. , Q) given in (2.2) has a special relationship with the null-pole subspace Sew, p .. ) studied in [BRa] as the following result shows.
109
Ball and Rakowski
2.2 .. Suppose (w,PIC(z),Q(z))
= (C".,A".,A"BC,r,PIC(z),Q(z»
is a a-admissible extended null-pole data set and let StreW, PIC) given by (1.5) and StreW, PIC' Q) given by (2.2) be the associated "R( 0' )-modules. Then THEOREM
PROOF:
The containment C is trivial from the definition. Conversely, suppose that j E StreW, PIC' Q)
is analytic on
0'.
By (2,2)
j(z)
(2.3) where x E
rx.
ctnw,h E "RmXl(a), r
E
= c".(z -
A". )-l x + h(z) + Q(z)r(z)
"Rkxl are such that PICj = 0 and
In general, if 9 E "Rmx1 has partial fraction decomposition 9
(elements of "Rmx1 with all poles inside ~c(9)
= 9_. Since C".(z -
0'
E
Resz=z.(z-Ad-1B,h(z) =
z.E"
= 9_ + 9+ where 9_ E "RO'Xl(a c )
and vanishing at infinity) and 9+ E "RmXl(a), we define
A".)-l x E "RO'Xl(aC) and h E "RmXl(a) in (2.2), we have
(2.4) But a consequence of (NPDSix) is that (2.4) can happen only if
From (NPDSi) and Lemma 12.2.2 in [BGR4), we conclude that x
= o.
Hence (2.3) becomes
j(z) = h(z) + Q(z)r(z) where PICj
= 0 and E Res..=z. (z -
A". )-1 BCh(z)
= O.
Since Qr is analytic on
(J'
and by (NPDSvii)
zaEr
Q has no zeros on 0', we must have that r is analytic on 0'. Furthermore, from (NPDSviii) we see that
E Resz=z.(z-Ad-1 BcQ(z)r(z) = o. Then j = h+Qr in fact is an element of StreW, PIC)n"RmXI(a) z.E"
as asserted. 3. Interpolation Problem.
Let
0'
be
&. subset
of the complex plane
ct. We look for a rational matrix function W
which is analytic on/O" and satisfies the following five interpolation conditions. Let
Z1,Z2,··· ,ZM
be given (not necessarily distinct) points in
scribed 1 X m and 1 x n vector functions analytic at zi (j be positive integers. We require that
0'.
Let
Xi
and
Yi
be pre-
= 1,2,··· ,M), and let k 1 , k 2 ,··· , kM
Ball and Rakowski
110
(3.1) for i
= 1,2,··· , kj and j
= 1,2,··· , M.
Let WI, W2, ..• , WN be given (not necessarily distinct) points on
0'.
Let Uj and Vj be
prescribed n x 1 and m x 1 vector functions analytic at Wj (j = 1,2,··· , N) and let It, l2,··· , IN be positive integers. The second condition is that
(3.2) for i
= 1,2,··· ,Ij
and j = 1,2,··· ,N.
For each pair of points Zi and Wj such that Zi
Wj,
we are given numbers /fg(1
1,2,··· , ki and 9 = 1,2,··· , Ij) so that df +1- 1
(3.3)
(J)
-:-(1-=-+-g------:1)-:"! -:"dz--:f:-:-+-g--:-1 (xi
(g)
( z) W ( Z )uj
I
( z)) Z=Zi
= / f g,
where M'1)(z) is a polynomial obtained by discarding all but the first 1/ coefficients in the Taylor expansion of a function h at Zi; that is, if h(z) = L:~1 h{i}(z - Zi)j-l in a neighborhood of Zi, M'1)(z) =
L:']=1 h{i}(z -
Zi)j-l.
The fourth interpolation condition is as follows. We are given 1 x m and 1 x n rational vector functions Pj+ and pj_ (j = 1,2,··· , K) analytic on
0'
and require that
(3.4) for all positive integers i and for at least one (and hence for all) A EO'. Finally, we are given n x 1 and m analytic on
0'
X
1 rational vector functions qj_ and qj+ (j = 1,2,··· , L)
and demand that i 1
dd i-I (W(z)qj_(Z))
(3.5)
Z
I
= ddZ i-I qj+(Z) I Z=A Z=A i 1
for all positive integers i and for at least one (and hence all) points A E 0'. Below, we reformulate the conditions (3.1) - (3.5) and show when they are consistent. The combination (3.1) - (3.4) was considered in detail in [BR5]; we summarize this case (the so-called 2-block case) first. We note that the problem of finding a rational matrix function which is analytic on
0'
and satisfies conditions (3.1) - (3.3) is called the two-sided Lagra.nge-Sylyester interpolation
problem. Its complete solution is presented in Chapter 16 of [BGR4J. The problem of finding a rational matrix function which is analytic on in [BRS].
0'
and satisfies conditions (3.1) - (3.4) has been solved
Ball and Rakowski
111
3.1 2-block Interpolation Problem.
In [BR5] the following general interpolation problem was considered. We are given a subset u of the complex plane a; and an interpolation data set
(3.6) consisting of matrices C+ E a;mxn·,C_ E a;nxn., A". E a;n.xn·,A( E a;n(xn(,B+ E a;n(xm,
B_ E a;n( xn,
r
E a;n( xn. and matrix polynomials P+(z) E nKxm and P_(z) E nKxn which
satisfy the admissibility requirements (IDSi) the pair (C _, A".) is observable and u( A".) C Uj (IDSii) the pair (A(, B+) is controllable and u(Ad C Uj (IDSiii)
r A". - A(r = B+C+ + B_C_
(IDSiv) p_CRnXl) C p+(nmXl), P+(z) has no zeros in
U
and the rows of [P+(z) P_(z)] form a
minimal polynomial basisj (IDSv) the function
is analytic on a;. (IDSvi) if 0"( A".) = {At. A2, ... , Ar }, the pair
j[
P+(Al) B+ ) P+(A2)
ArI
'
P+~Ar)
is controllable. A collection of data w in (3.1.1) satisfying (IDSi) - (IDSvi) is said to be a uadmissible interpolation data set. The problem then is to describe all rational matrix functions with W(z) analytic on u which satisfy the interpolation conditions
(3.1') zoEO'
(3.2') zoEa'
(3.3')
L zoECI
and
(3.4')
Resz=zo(z -
Ad- 1 B+W(z)C_(z - A".)-l
=
r
112
Ball and Rakowski
We mention that the problem (3.1') - (3.4') is simply a more compact way of writing conditions (3.1) - (3.4). Indeed (3.1') is equivalent to (3.1) if we let, for each j
(3.7)
A(j
['
= {
1
Zj
,8;+ =
1
= 1,2, .. · ,M, {l}
[:!:){,) 1
Yj
{2}
,8;_ =-
z{l.j}
Zj
yJI.i}
J
where f{i} denotes the
ith
Yj
coefficient in the Taylor expansion of a function fat
Zj,
and set
(3.8)
Conversely, if matrices A(, B+, B_ of appropriate sizes are given, there exists a nonsingular matrix
S such that SA,S-l is a block diagonal matrix with the diagonal blocks in lower Jordan form. After replacing A( by SA,S-I, B+ by SB+ and B_ by SB_, we can convert the interpolation condition (3.1) to the equivalent condition (3.1'). Similarly, if for each j
= 1,2,··· , N
we let
(3.9)
Wj
A"'j =
[
1 Wj
and then set
A".
= [ A""
A"..
1
. A".N
then (3.2') collapses to (3.2). Conversely, if the matrices C+, C_, A". are given, we can find a nonsingular matrix S such that S-lA".S is in Jordan form. After replacing A ... by S-lA".S, C_ by
C_S, and C+ by C+S, we can reformulate the interpolation condition {3.2'} in the more detailed form {3.2}.
Ball and Rakowski
113
A similar analysis gives an equivalence between (3.4) and (3.4'). Suppose first that and let rii and
Wj
If Zi
f=
Z;
= wi
= hlg] where 'Y!i! = 1,2, .. ·ki and 9 = 1,2,,,, ,Ii) are numbers associated with Zi
as in (3.3). Then the interpolation conditions (3.3) hold if and only if
Wj
let rij be the unique solution of the Sylvester equation in X
where A".j and A" are as in (3.7) and (3.8) (see [BGR4], Appendix A.l) and set r = [fij] with 1 ::::; i ::::; M and 1 ::::; j ::::; N. Then the set of interpolation conditions (3.3) is equivalent to the single
block interpolation condition (3.3'). We also mention that validity of the Sylvester equation
is a necessary and sufficient condition for the consistency of (3.1') - (3.3') (see [BGR4] or [BR5]). Conditions (3.3) can be recovered from (3.3') by multiplying both sides of the equality by nonsingular matrices Sand T such that SA,S-l and T-l A,T are in lower and upper Jordan forms, respectively, and reading the numbers "(Ig from the appropriate blocks ofthe matrix SrT. Finally, if P+ and P_ are rational matrix functions whose jt" rows (j
= 1""
, K) are
equal to Pj+ and -Pj_ respectively, then it is easy to see that conditions (3.4) are equivalent to (3.4'). Demanding that P+ and P_ are polynomials is with no loss of generality. The admissibility conditions (IDSi) - (IDSvi) guarantee consistency and minimize redundancies in the interpolation conditions. For complete details we refer to [BR5]. 3.2 The general 4-block case.
Let Q_ and Q+ be rational matrix functions whose
P"
columns (j
= 1,2"" , L) are
equal to qj_ and qj+, respectively. Conditions (3.5) are equivalent to
(3.5') Similarly as with P+ and P_, we will assume first Q_ and Q+ are matrix polynomials and the columns of
(3.10) form a minimal basis.
Ball and Rakowski
114
We consider now the consistency of condition (3.5'). It follows immediately from (3.5') that
Also, since W is analytic on u, Q_ has no zeros in u. Indeed, if Q_ had a zero in u, then Q+ = W Q_ would have a zero in u, and so the rank of the matrix polynomial (3.10) would drop at some point of u, contradicting the fact that the columns of (3.10) form a minimal polynomial basis. Condition (3.1) says that the first kj Taylor coefficients at Zj of Xj(z)W(z) coincide with the first kj Taylor coefficients at Zj of Yj(z). Therefore, by (3.5'), the first kj Taylor coefficients at
zi of Xj(z)Q+(z) coincide with the first kj Taylor coefficients at Zj of y;(z)Q_(z). Consequently, the function
(z - AC;)-l[Bj+ Bj-l
[3~~~~n
is analytic on CJ: where AC;' Bj+ and Bj_ are as in (3.7). Hence the function
is analytic on CJ:. Suppose that a vector Uj(Wj) is in the column span of Q_(Wj), where functions in (3.2). Then Uj(Wj)
Uj
is one of the
= Q_{Wj)Uo, and it follows from (3.2) and (3.5') that
So in this case conditions (3.2) and (3.5) are either redundant or contradictory. To exclude such situations we require that the matrix
[Ui,(Wj,) uj,(wj,) .. . ui. (wi.) Q-{Wi'>] have full column rank whenever Wj,
= wi. = ... = Wj..
In terms of the data A"., C+, C_, this
assumption is equivalent to the controllability of the pair
(3.11)
where {wi"wi.,··· ,Wi.} is the set of distinct points among {WtoW2,··· ,WN}. We will call this assumption the consistency of right generic and right lumped interpolation conditions. Finally, in view of (3.4') and (3.5'),
Ball and Rakowski
115
P+Q+ = P+WQ_ = -P-Q-. So conditions (3.4') and (3.5') are consistent if
We summarize various consistency and minimality properties our interpolation data must have in the following definition. We will call the data
(3.12) a q-admissible interpolation JiiWl.ill if C+ E a: mxn • , C_ E a: nxn ., A". E a:n• xn., A( E a:ne xne, B+ E
a:nexm,B_ E a:nexn,r E a:nexn·,p+(z) E nKxm, P_(z) E nKxn,Q_ E nmxL,and Q+ E nnxL are such that (IDSi) the pair (C_,A".) is observable and O'(A".) C 0'; (IDSii) the pair (A(, B+) is controllable and O'(A".) C 0'; (IDSiii) r A". - A,r = B+C+ (IDSiv) P_ nnxI
c
+ B_C_;
p+nmxI, P+(z) has no zeros in 0' and the rows of [P+(z) P_(z)] form a
minimal polynomial basis; (IDSv) the function
is analytic on a:. (IDSvi) if 0'( A".)
= {AI, A2, ... , AT}, the pair P+(At) B+ ) P+(A2)
P+(AT) is controllable; (IDSvii) n1xmQ+(z)
c nlxnQ_(z), Q_(z) has
form a minimal polynomial basis;
no zeros in 0', and the columns of
Ball and Rakowski
116
(IDSviii) the function
is analytic on 0:. (IDSix) if u(A".)
= {w}, W2,··· , w.}, then the pair
J)
is observable. (IDSx) [P+ P_]
[~~] = o.
Given a u-admissible interpolation data set, the interpolation problem is to find which m x n rational matrix functions W analytic on u satisfy conditions (3.1') - (3.5'). 4. Parametrization of solutions.
Theorems 4.1 and 4.2 below present our results on parameterization of solutions of the interpolation problem (3.1') - (3.5') (respectively with or without an additional norm constraint). We first need the following observation. Ifw
= (C+, C_, A"., A"
B+, B_, r, P+(z), P_(z), Q_(z),Q+(z»
is a u-admissible interpolation data set, then the collection of matrices
(4.1) together with the matrix polynomials PI<
= [P+
P_] and Q
= [~~]
satisfy conditions (NPDSi)
- (NPDSx) in Theorem 2.1. Therefore there exists a rational block row matrix function 9
8 = [8
: 9 1S ] in n,(m+n)x(m-K+n) (where 9 1 E n,(m+n)x(m-K+n-L), 9 2 E : 92S n,(m+n)xL and 9 1 = [9 11 8 12 ] with 9 11 E n,mx(m-K) 9 s = [9 1S ] with 8 1s E n,mXL) which 9 21 922 ' 9 2S [91
s]
11
=
8 21
has
9 12 9 22
(w, [P+(z) P"':(z)], [~~~~~]) as an extended complete null-pole data set over u. The 2-block
version of the following appears as Theorem 4.1 in [BR5]. THEOREM
4.1. Let u E 0: and let was in (3.12) be a u-admissible interpolation data set. Then there
exist functions W E n,mxn(u) which satisfy the interpolation conditions (3.1') - (3.5'). Moreover, if
117
Ball and Rakowski
is a block row rational matrix function with extended complete nun-pole data set over 0' equal to
(w, [P+(z) P_(z)], [g~~~~]), then a function WE 1lmxn is analytic on 0' and satisfies interpola-
tion conditions (3.1') - (3.5') if and only if W
= [011Q1 + 0 12 Q2 0 13] [021 Ql + 022Q2 0 23r 1
where Ql E 1l(m-K)x(n-L)(0') and Q2 E 1l(n-L)x(n-L) are such that
[021Ql
+ 0 22 Q2 0 23] (1l(n-L)Xl(0') EB 1lLXl)
= [021022023] (1l(m-K+n-L)X1(0')EB1l LX1 ).
(4.2)
We note that condition (4.2) holds for a generic pair (Q1, Q2) of rational matrix functions
lr IT::::::::~: ~::~ri::'':::ho:',::':~:M~;: :-:::~u:::,: function [0 21 0 22 0 23 ], an 1l-subspace inside 1l(m-K+n)xl of dimension m - K. For the Hoo-control problem, one takes 0' to be either the right half plane n+
Re z > O} or the unit disk V
= {z : Izl <
= {z
:
I} and asks that W, in addition to meeting a set
of interpolation conditions on 0', satisfy IIWlloo := rms1LPzEuIlW(z)1I
<
'Y for some prescribed
tolerance level 'Y. Without loss of generality we assume that 'Y has been normalized to 'Y = 1. The following refinement of Theorem 4.1 gives the solution ofthis generalized Nevanlinna Pick problem (Le. interpolation problem with norm constraint). The 2-block version of the following result is Theorem 4.2 in [BRS]. THEOREM 4.2.
Let 0' be either the right half plane n+ or the unit disk V and let w as in (3.12) be
a O'-admissible interpolation data set. Suppose that there exists a rational (m + n) x (m - K
+ n)
block row matrix function 0(z) = [0 11 (Z) 0 21 (Z)
0 12 (z) 0 22 (Z)
(with 0 11 E 1lmx (m-K), 0 12 E 1lmx (n-L») such that
: 0 13 (Z)] : 0 23 (Z)
(a) ([ g~] ,A", A(, [B+ B_], r, [p+(z) P_(z)],
[g~~~~])
is an extended complete
nuJI-pole data set for 0 over 0' and
/
(b) e is analytic on 80' (including at infinity if 0' = n+) and satisfies 0(z)* J0(z) j EB -h,z E 80' where J Then the fonowing are equivalent.
= 1m EB -In,j = Im-K EB -In-L.
=
118
Ball and Rakowski
(i) There exist functions W E
'Rmxn(O')
(3.5') and in addition satisfy
which satisfy the interpolation conditions (3.1') -
IIWlloo < 1.
(ii) 9 satisfies 9(z)* J9(z) $ j Ell O(n-L)x(n-L) at all points z of analyticity in Moreover, if (i) and (ii) hold, function W E 'Rmxn is analytic on lation conditions (3.1') - (3.5') and has
W= [9
(4.3)
11 H
satisfies the interpo-
IIWlloo < 1 if and only if
+ 9 12 9 13]
for an H E 'R(m-K)x(n-L)(O') with
0',
0'.
[9
21 H
+ 9 22
9 23 ] -1 =: ge[H)
IIHlloo < 1.
In fact the existence of a matrix function 9 satisfying conditions (a), (b) in Theorem 4.2
REMARK.
is also necessary for interpolants
W with IIWlloo < 1 to exist, but we do not prove this here.
To make Theorem 4.2 useful we need a systematic way of computing the rational matrix function
e
appearing in Theorem 4.2. For practical purposes we need only compute a rational
matrix function 9 of the form
9=e[Jl
J2
~J
where 11,12, and 13 are any rational matrix functions (of the appropriate sizes) with 13 invertible and
e is as in Theorem 4.2, since in such a case 9
map ge
= ge
and
e induce the same linear fractional
(see [BHV)). One can obtain such a matrix function 9 from a preliminary
constructed to meet the specifications in Theorem 4.1 as follows. IT by W'j(z) = 0li(Z)*01'(Z) 1<'J<3 Partition W as a block 2 X 2-matrix function by
define W(z)
= [W.j(Z)]
W= where Wo
O2.(z)*02j(z).
[~! ~:]
= [W'jh~'.j~2 and set V equal to the Schur complement
Finally find a square outer matrix function Ro(z) such that V(z)
= Ro(z)*jRo(z).
Then
_= 9-9
[R00 0] I 1
e=
[011 021
012 022
e
013] 023 '
Ball and Rakowski
119
is the desired matrix function such that the associated linear fractional map
ge parametrizes
interpolants with norm less than 1 as in Theorem 4.2. Hence, once one has constructed a Theorem 4.1, one arrives at an appropriate
e as in
e via one j-spectral factorization V = R*jR. For more
complete details we refer to Theorem 4.3 in [BHV]. Alternatively, once one has a matrix function
e meeting the specifications in Theorem 4.1,
one could transform to a plant P such that the transform P of P to the generalized chain formalism is equal to
e (see Section 5). Then the interpolation problem with norm constraint IIWlloo < 1 is
equivalent to the Boo-problem for the plant P (with tolerance level 1); one can then use any of the known solutions of the Boo-problem (e.g. [DGKF], [G], [PAJ]) to produce the parameterizer
e of
contractive (or "bounded real" in engineering parlance) interpolants. Of course, it would be desirable to have the criterion for existence of interpolants W with IIWlloo < 1 and the construction of the linear fractional map
ge expressed more directly in terms
of the interpolation data w, as has been done for the I-block case in [BGR4]i this together with a more explicit realization formula for in this area. As was remarked above, pole data set whenever w
e in terms of the data set u, is the remaining open problem
(w, [P+(z) P_(z)], [~~~;~]) is a u-admissible extended null-
= ( C+,C_, A"., A"
B+, B_, r, P+(z), P_(z), Q_(z), Q+(z») is au-admis-
sible interpolation data set. The converse statement is not true in general; the following theorem, which will be used in our characterization of stabilizable linear feedback systems in the next section, characterizes which u-admissible extended null-pole data sets
(w, [P+(z) P_(z)], [~~~;~]) arise
from u-admissible interpolation data sets in terms of the associated extended null-pole subspace S(w,[p+ P_],
[~~]); see Theorem 4.3 [BR5] for the 2-block case and Theorem 13.2.3 in [BGR4]
for the I-block case. THEOREM
4.3. Let
(w, P, Q) be a u-admissible extended null-pole data set of the form
and set w
= (c+, C_, A"., A"
B+,B_,r, P+(z), P_(z),Q_(z),Q+(z»).
Then the following are equivalent. (i) w is a u-admissible interpolation data set. (ii) The extended null-pole subspace S
= S,,(w, P, Q) c
following properties: (a) S n [n.mxl ED 0] c n.mXl(u) Ell 0,
n.(m-K+n)xl (see (2.2)) has the
120
Ball and Rakowski
(b) POE9R ftX1(Snn.<m+n)Xl(O'») =
oEll n.nXl(O') WherePOE9R
ft . . ( [ : ] )
[~].
=
PROOF: Suppose first that w is a O'-admissible interpolation data set. By definition, any function
f
E S has the form
= [h(Z)] = [C+] (z _ A".)-lz + [h+(Z)] + [Q+(z)] r(z) f-(z) C_ L(z) Q_(z)
f(z)
where z E o:n., h+ E n.mXl(O'), h_ E n.nXl(O'), r E n.LXl. Suppose that f-(z)
h_(z)
+ Q_(z)r(z)
= O. Let P~c denote the projection map P~c : k
partial fraction decomposition k = k_
+ k+
where k_ has all poles in
=0
(i.e. k_ E n.~Xl(O'C» and k+ E n.nXl(O'). Then from fC_(z - A".)-lz E n.~Xl(O'c) and h_ E n.nXl(O'), we see that
0'
->
= C_(z -
A". )-lZ +
k_ if k E n.nxl has
and vanishes at infinity
we get that P~c(f-)
= OJ
since
(4.4) But now by condition (IDSix), (4.4) forces
(4.5) By Lemma 12.2.2 in [BGR41, the first condition in (4.5) forces z = O. Also, since by (IDSvii) Q_ has no zeros in
0',
the second condition in (4.5) forces r to be analytic on
h(z) = h+(z) + Q+(z)r(z) is analytic on
0'.
[}~]
But then
Thus S satisfies conditions (ii-a) in Theorem 4.3.
To verify (ii-b) we must show that for any given so that
0'.
f-
E n.mXl(O') we can find hE n.mXl(O')
E S. But by Theorem 2.2, S.,.(w,p)nn.<m+n)xl(O') = S.,.(w,p,Q)nn.<m+n)xl(O').
Hence this result follows in the same way as for the 2-block case (see Theorem 4.3 in [BR5]). Conversely, suppose which S
= S.,.(w,[p+
P-l,
(w, [P+ P-l, [8~]) is a O'-admissible extended null-pole data set for
[8~])
satisfies (ii-a) and (ii-b). Thus (w,[p+ P-l,
[8~])
satisfies
(NPDSi)-(NPDSx) and we must verify that w satisfies (IDSi) - (IDSx). First note that (IDSiii), (IDSv), (IDSviii) and (IDSx) follow from their counterparts (NPDSiii), (NPDSv), (NPDSviii) and (NPDSx) respectively without use of any assumptions on S.,.
(w, [P+ P-l, [8~]). Next, one can
use Theorem 2.3, assumption (ii-b) and the same arguments as those for the 2-block case (see Theorem 4.3 in [BR5]) to deduce (IDSii), (IDSiv) and (IDSvi) from their counterparts (NPDSii), (NPDSiv) and (NPDSvi). It remains now only to verify (IDSi), (IDSvii) and (IDSix). Suppose now that (C_, A ... ) is not observable. Then by Lemma 12.2.2. in [BGR4l there is an z
e 0:".
not zero with C_(z - A... )-lz
we can solve for h+
e n.mXl(O') so that
= 0 identically in z.
From Theorem 4.5 (i) in [BR3I,
121
Ball and Rakowski
is in S,,(W, P) C S,,(w, P, Q) (here we use that (IDSvi) has already been verified). Furthermore, since ([ g~]
,A,,)
is observable by (NPDSi), and since C_(z -
A" )-lx = 0, by
Lemma 12.2.2. in [BGR4j again necessarily C+(z - A" )-l x is not identically zero. Then fin (4.6) is an element of S,,(w,P,Q) in violation of (ii-a). Hence we must have (C_,A".) observable, i.e. (IDSi) holds. Next suppose (IDSvii) is not true. Then we can find r E 1lLX1 such that Q+r ~ 1lmXl(0') but Q_r E 1lnXl(0"). Again by an argument based on Theorem 4.5 (i) in [BR3j, we can then produce an element h+ E 1lmXl(0") so that
[~~r]
E S,,(w, P)
c S,,(w, P, Q). The n
is an element of S,,(W, P, Q) in violation of (ii-a). Hence (IDSvii) must hold. Finally, suppose (IDSix) is violated. Then we can find x =F 0 in o;n. and r =F 0 in 1lLX1 so that L(z)
= C_(z -
A,,)-lx
+ Q_(z)r(z)
can produce h+ E 1lmXl(0') so that
[~~]
E
E
1lnXl(0'). From Theorem 4.5 (iii) in [BR3j we
S,,(w,P) C S,,(w,P,Q) where h_ = (I -
Also by Theorem 4.5 (i) from [BR3j there is 9 E 1lnx1 (0') so that
[g~] (z -
P~c)(Q_r).
A" )-1 X +
[g~)]
E
S,,(w, P) C S,,(w, P, Q) (here we use that (IDSvi) has already been verified). But then
+ Q_(z)r(z) is analytic on 0' and (NPDSix) is in force, we + Q+(z)r(z) is not analytic on 0". Hence f is an element of
However, since x =F 0, C_(z - A,,)-l x are guaranteed that C+(z - A,,)-I X
S,,(w, P, Q) in violation of (ii - a). Thus, (IDSix) must hold and Theorem 4.3 follows. The proof of Theorem 4.1 requires the following lemma, an adaptation of one of the main ideas in [Be]. LEMMA 4.4. Let 0' C 0;, let w as in (3.12) be a a-admissible interpolation data set, and let
122
Ball and Rakowski
be a block row rational matrix function with extended complete null-pole data set over u equal to
(w, [P+ P-1, [~~])
where
wis as in (4.1). Then a function W E nmxn is analytic on u and
satisfies the interpolation conditions (3.1 ')-(3.5') if and only if
[Wjz)] [021 02 2 0 231(n(m-K+n-L)X1(u) EB n LX1 )
C 0 ( n(m-K+n-L)x1(u) EB nLX1).
(4.7) PROOF:
As in the proof of Theorem 4.3, one can show that
[0 21 0 22 0 231( n(m-K+n-L)x1(u) EB n LX1 )
={C_(z -
A"y 1x: x E C n.} + nmX1(u) + Q_nLX1
S,,( (C_,A,.),(0,0),0),0,Q_).
=
Suppose W is analytic on u and satisfies the interpolation conditons (3.1 ')-(3.5'). By Lemma 4.4 in [BR51,
[lj] ({C_(Z-A,,)-1X:XEG:n.}+nmX1(u»)
C
S,,(w, P) C S,,(w, P, Q)
=
0(
n(m-K+n-L)x1(u) EB nLX1).
But by condition (3.5'),
and hence the inclusion (4.7) follows. Conversely, suppose that the inclusion (4.7) holds. Then
[lj] Q_nLX1
C
nr0(n(m-K+n-L)Xl(u)EBnLXl) ~ER
= 0(0 EB n LX1 ) = [8~] n LX1 and hence W satisfies (3.5'). Moreover, by an argument in the proof of Theorem 4.3 we know that
123
Ball and Rakowski
Using also that Q_r = 0 implies that Q+r = 0 (a consequence of (IDSvii», we see that the inclusion (4.7) implies that
[lj] c
S"
({C_(Z-A1r)-lx:x E o:n.}+1lnXl
(u»)
(w, [P+ p-1) = fm(m-K+n)xl(u).
Now Lemma 4.4 from [BR51 implies that W is analytic on u and satisfies the remaining interpolation conditions (3.1 ') - (3.4'). PROOF OF THEOREM
4.1. By Lemma 4.4 it suffices to show that W E 1lmxn satisfies
[lj]
[9 21 9 22 9 231( 1l(m-K+n-L)Xl(u)EIl1lLXl )
C 9 ( 1l(m-K+n-L)xl (u) EIl1lLXl)
(4.8)
if and only if W has a representation of the form
(4.9) where
Ql
E 1l(m-K)x(n-L)(u), Q2 E 1l(n-L)x(n-L)(u) are such that
[9 2l Ql
(4.10)
+ 9 22 Q2 9 231( 1l(n-L)xl(u) EIl1lLXl)
= [9 21 9 22 9 231(1l(m-K+n-L)Xl(u) Ell 1lLXl).
Suppose first the (4.9) and (4.10) hold. Rewrite (4.9) in the form
[lj]
[9 2l Ql
+ 9 22Q2
9 2319
[~~ ~].
Apply both sides to 1l(n-L)xl(u) EIl1l LXl and use (4.10) to get
[If] [9
21
9 22 9 231(1l(m-K+n-L)Xl(U) Ell 1lLXl)
= 9 [~~ ~]
(1l(n-L)Xl(U) EIl1lLXl).
Ball and Rakowski
124
Since Ql and Q2 are analytic on u, we have
and (4.8) follows. Conversely, suppose (4.8) holds. Note that r~r 'RLXl)
=
[lj]
9 23] ( 'R(m-K+n-L) Xl (u)E9
823'RLxl is a 'R-subspace of 'Rnxl of dimension L which (by (4.8)) is contained
n
r9('R(m-K+n-L)Xl(u) E9 'RLXl) == rER dimension count,
in
[lj] [821 822
[lj]
[~13] 'R LXl , also an 'R-subspace of dimension 8 23
823'RLXl ==
L. By
[~~:] 'RLXl.
Next note that the quotient module
[lj] [821 8 22 8 23]
('R(m-K+n-L)Xl(U) E9 'RLXl) /
[lj]
823'RLxl
is a free 'R(u)-submodule of
[qn-L,+ ] ql,+ ] with n - L generators; we may choose n - L generators of the form 8 [ qti- , .. ·8 qn-oL,- and
then set
Q+ == [ql,+ ... qn-L,+] E'R(m-K)x(n-L)(u), Q_ == [ql,- .. . qn-L,-] E'R(n-L)x(n-L)(u).
Then the left side of (4.8) has the representation
[lj] [92l 9 22 923] == 8
[~~ ~]
== [8 UQ1 9 21 Ql
('R(m-K+n-L)Xl(u) E9 'RLXl)
('R(n-L)Xl(U)E9'R LX1 )
l2 Q2 813] + + 9922Q2 9 23
('R(n-L)Xl(U) E9 'RLXl)
From equality of the bottom components in (4.11) we deduce that the pair (QhQ2) satisfies (4.10) and then (4.11) can be rewritten as
Ball and Rakowski
125
[lj] [921Ql + 9 22 Q2
923] ( n.(n-L)xl( u) Ell n. LX1 )
= [99 2111Q1 + 9 12 Q2 9 13 ] Ql + 8 22Q2 9 23
(4.12)
(n.(n-L)Xl(U) Ell n.LX1 )
Also from (4.10) we see that the square matrix function [9 21 Ql +9 22 Q2 9 23 ] cannot have determinant vanishing indenticaIly, and hence [9 21 Ql +9 22 Q2 9 23 ]-1 exists. Now (4.12) leads immediately to the representation (4.9) for W. The proof of Theorem 4.2 requires the following lemma. LEMMA 4.5. Suppose u,w and 9 =
[~11 ~12 ~13] 021 022 023
are as in the hypothesis of Theorem 4.2.
Then 9 satisfies
9(z)* J9(z) :5 i Ell 0, z E u (where J
= 1m Ell -In
and
i = Im-K Ell In-L)
if and only if [In-L 0][922 923r1921 has analytic
continuation to all of u. PROOF:
By assumption 9(z)*J9(z)
= i Ell -h for z E ou. In particular
[~t~] [912 9 13]- [~~~] [922 923] = -In' Hence
[9* ][922 9 23] 9~~
=
hn +
Z
E OU.
[9* ][912 9 13] for z E ou. As [922 9 23] is square, we conclude 9i~
that [922(Z) 9 23 (Z)] is invertible for Z E
ou.
Then for each fixed z we can rewrite the system of
equations
(4.13) (for z E ou) in the equivalent form
(4.14) where
= [912 9 13][922 9 23r1 U12 = 9 11 - [912 9 13][922 923r1921 g:~] = [822 823r1 U11
[
[g:] = -[822 823]-1821 .
126
Ball and Rakowski
Note that 0(z)* J0(z)
= j Ell -h on au is equivalent to
or equivalently, to
whenever z E au and (u,y,yO,v,w) satisfies (4.13). Since (4.13) and (4.14) are equivalent, we see that 0(z)* J0(z)
=j
EIl-h on
U12] au is equivalent to U(z) = [UU U2I U22 (z) being isometric on au.
Similarly, the validity of 0(z)* J0(z)
:s; j
hI
U32
Ell 0 on u is equivalent to
or otherwise stated, to
whenever z E u and (u,y,yO,v,w) satisfy (4.13). Since (4.13) and (4.14) are equivalent, we read off that this in turn is equivalent to [Im+n-L O]U(z) being contractive on u. In particular
must be contractive at all points of analyticity of u, and hence has analytic continuation to all of the set u. Conversely, to show that 0(z)* J0(z)
:s; jEllO on u is equivalent to showing that [Im+n-L 0]
U(z) has contractive values at all points of analyticity in u, or, equivalently by the maximum modulus theorem, that
have analytic continuation to all of u. By assumption we know only that
has such an analytic continuation. The fact that this forces Un, U12, and Un to have such an analytic continuation as well relies on the special structure of the extended null-pole subspace
e(1l(m-K+n-L)Xl(U) Ell 1lLXl) = s. . (w,[p+,P_J, [8~]) given by Theorem 4.3. Details for the I-block case (the case where K
= 0 and L = 0) are given in Theorem 13.2.3 in [BGR4Ji we leave
it to the reader to check that the general case here can be verified by analogous arguments.
Ball and Rakowski
PROOF OF THEOREM
127 4.2. Let a,w and 8 be as in the statement of Theorem 4.2. Suppose first
that 8(z)* J8(z) ::::: JED O(n-L)x(n-L) at all points z E a where 8(z) is analytic and that H E 1l(m-K)x(n-L)(a) with
IIHlloo < 1.
Then
(4.15) By Lemma 4.5 we know that [In-L 0][8 22 8 23 ]-18 21 is analytic on a and, from the proof of Lemma 4.5, that 11[8 21 823J-1821(z)1I invertible for all
Z
< 1 for z E Ba. Hence t[In-L 0][8 22 8 23 ]-18 21 H + In-L is
E Ba and for all t with 0 ::::: t ::::: 1. Hence wno det([In_L 0][8 22 823r1821H
+
In-L) = wno det In-L = 0, where wno X is the change of the argument of X(z) along Ba.
As we observed above that [In-L 0][8 22 823r1821H det([In_L 0][822 823r1821H
+ In-L)
+ In-L
is analytic on a, we conclude that
has no zero in a. From this we see that
From (4.15) we conclude that
[8 21 H
+ 8 22 8 23] (1l(n-L)Xl(a) ED1lL)
= [8 22 8 23 ] ( 1l(n-L)xl( a) ED1lL ).
(4.16) On the other hand,
[8 21 8 22 8 23 ] ( 1l(m-K+n-L)X1(a) ED1lL) ( 4.17)
= [8 22 8 23 ][[8 22 823J-1821 In] (1l(m-K+n-L)X1(a)ED1l L ).
But by Lemma 4.5 [In-L 0][8 22 823]-1821 is analytic on a, so
[[822823]-1821 In] ( 1l(m-K+n-L)x1 (a) ED1lLX1) (4.18)
= 1l(n-L)Xl(a) ED1lLX1.
Combining (4.17) and (4.18), we obtain
Ball and Rakowski
128
[9 21 9 22 9 231 ( R(m-K+n-L)xl(U) E9 RLX1) = [9 22 9 231 ( R(n-L)xl(U) E9 RLX1).
(4.19)
Combine (4.19) and (4.16) to see that the pair (H,I) is an admissible parameter pair in the sense of Lemma 4.4. Hence, by Lemma 4.4 we know that W = [9 11 H + 9 12 9 13 )[9 21 H + 9 22 923r 1 is analytic on u and satisfies the interpolation conditions (3.1') - (3.5'). Moreover, for z E 8u,
where 'I/J
= [9 21 H + 9 22
923r 1. Hence IIW(z)1I
< 1 for z E
8u. By the maximum modulus
principle, IIW(z)1I < 1 for z E u. Conversely, suppose that there exists a function W E Rmxn which is analytic on u, satisfies the interpolation conditions (3.1') - (3.5') and has IIWlloo < 1. Then by Theorem 4.1 we know that there are Ql E R(m-K)x(n-L)(u) and Q2 E R(n-L)x(n-L)(u) such that
[9 21 Ql (4.20)
+ 9 22 Q2
9 231( R(n-L)xl(u) E9 RLX1)
= [9 21 9 22 9 231(R(m-K+n-L)Xl(u) E9 RLX1),
from which we recover W as
(4.21) An alternative way to write (4.21) is
= [9 21 Ql + 9 22 Q2
9 231. Since IIWlloo < 1 and on 8u by assumption, we have, for z E u, where 'I/J
e satisfies condition (b) in Theorem 4.2
129
Ball and Rakowski
( 4.22) Thus Q2(Z) cannot have any null space for z E
0',
and hence, as it is square, Q2(Z)-1 exists for
z E au. Also (4.22) then implies that H(z) = Ql(Z)Q2(Z)-1 iswell defined and satisfies IIH(z)1I < 1 for z E
au. Next note from (4.20) the inclusion
[0 22 0 23 ]( 'R("-L)Xl(u)ED'R LX1 )
c [0 21 Ql + 0 22 Q2 023] ( 'R(,,-L)Xl(u) ED 'RLXl).
(4.23)
We also know from the proof of Lemma 4.5 that [0 22 0 23 ] is invertible on
au.
Then (4.23) can be
written in the form
'R(n-L)Xl(U) ED'RLX1 (4.24)
C ([0 22 023r1021[Ql 0]+
[~2 ~])('R(n-L)Xl(u)ED'RLXl).
A
= [1,,-L
0][022 023r1021Ql + Q2 has size (n -
has size L X (n - L). In this notation (4.24) assumes the form 'R(n-L)Xl(U) ED 'R LX1 C This in turn requires
(4.25) Note that
JJ
[~2 ~] has the form [~ where L) X (n - L) and B = [01£][022 023r1021Ql
Note that the nxn matrix function [022 023r 1021[Ql 0]+
[~ ~]
('R(n-L)Xl(u) ED 'RLXl).
130
Ball and Rakowski
A = ([In-L 0][0 22 023r 10 21 H proof of Lemma 4.5) and where IIH(z)1I
+ I)Q2
where 11[0 22 0 23r 1 0 21 11 < Ion au (from the
< 1 and Q2(Z) is invertible on au from observations made
above. Hence A(z) is invertible on az and wno det A(z) is well defined. The inclusion (4.25) gives us that
On the other hand,
(4.27) As was observed above, II[In-L 0][0 22 023r1021HII
argument wno det ([In-L 0][0 22 023r1021H
+ I)
<
1 on au. Then by a standard homotopy
= 0, so
wno det A = wno det Q2.
(4.28)
Since Q2 is analytic on 0', by the argument principle we deduce
wno det Q2
(4.29)
~
o.
Combining (4.26), (4.28) and (4.29) leads to
(4.30)
wno det A
= 0 = wno det Q2.
Condition (4.30) has several consequences. First of all, det Q2 has no zeros on 0' so Q;1 and
H := QIQ;1 are analytic on u. Secondly, we deduce that equality must hold in (4.24) and hence in (4.23). This has a consequence that
[0 22 9 23 ] (1l(n-L)Xl(U)
or equivalently
EIl1lLX1)
= [021
0 22 0 23] ( 1l(m-K+n-L) xl (0') Ell 1lLX1) ,
131
Ball and Rakowski
This condition in turn is equivalent to
By Lemma 4.5 this last condition is equivalent to 0(z)* J0(z) :::; j ffi 0 for z E u. Thus we have verified that condition (ii) in Theorem 4.2 is necessary for interpolants W with
IIWlloo < 1 to exist.
It remains only to verify that W has the form (4.3) for an H E n(m-K)x(n-L)(u) with
IIWlloo < 1.
We have already verified that H := Q1Q;1 is analytic on
<
the maximum modulus theorem it follows that supIIH(z)1I
0'
with norm < 1 on Bu. By
1. Moreover, from (4.21) we deduce
zED"
that
= ([0 n H + 0 12 0 13] [~2 ~] )([0 21 H + 0 22 0 13] [~2 =[0 n H + 012 0 13 ][0 21 H + 0 22 023r1
W
as needed. 5. Interpolation and internally stable feedback systems.
In this section we establish the connections between the interpolation theory presented in the previous sections and the problem of designing a compensator to stabilize a given plant in a standard feedback configuration which has been studied in the control literature (see [Fr], [DGKFl). We emphasize that the connection between internal stability and interpolation has been a recurring theme in the systems theory literature (see e. g. [YBL], [V], [Kil). The matrix version of the result is usually derived via a coprime factorization of the plant and the Youla parametrization of stabilizing compensators (see [YJB]). Our contribution here is to relate the interpolation conditions directly to the original plant P; the connection is given in terms of the extended complete null-pole data set of a related block row rational matrix function
P.
We also solve the inverse problem of
describing which plants P go with a prescribed set of interpolation conditions
5.1 Preliminaries on feedback systems. Suppose we are given a rational block matrix function P
= [~~~ ~~:] , where Pn, P12,
P 21 , P22 have respective sizes n z x n w , n z x n u , nil
X n w , ny
complex plane 0: 00 • (For discrete time systems
is usually taken to be closed unit disk while for
0'
x n", and
0'
is a subset of the extended
continuous time systems 0' is usually taken to be the closed right half plane including infinity.) The problem is to design a rational n,. x nil matrix function K (the compensator) so that the closed loop system depicted in Figure 5.1 is internally au.bk, a notion which we shall make precise in a moment. (Here we assume that all input-output maps are causal, linear, time invariant and finite dimensional, and that the Laplace transform has already been implemented so all input-output maps are represented as multiplication by rational matrix functions.)
Ball and Rakowski
132
w
~
u
z
f
,~
--"'-
Y
K
'" .....
'
Figure 5.1 In Figure 5.1,
w,z,'U,y
are functions with values in CC,,·xt,ccn.xt,ccn.xt and CC n• xt , re-
spectively, which are analytic in some right half plane (for the continuous time case) or in some disk centered at the origin (for the discrete time case); in our discussion here we also assume that all the functions are rational, although this assumption is not necessary. The configuration depicted
in Figure 5.1 is equivalent to the system of algebraic equations
PllW
+ P t 2'U =
P2tW
+ P 22'U = Y Ky =
(5.1) In the control theory context, the function
aipal, z is the mm: ~ and y is the
K which computes the control signal system E(P,K):
W
~
W
z
'U.
is the disturbance or
measurement~.
'U
reference~, 'U
is the J:mltml
The idea is to design a compensator
based on the measurement y so as to make the overall
z perform better. The standard BOO-control problem is to design K which
minimizes the largest error z (in the sense of L2- norm) over all disturbances w of L2- norm at most 1, subject to the additional constraint that K stabilizes the system: (5.2)
K
min 6tr>bilizing
max IIz1l2. IIwll.$1
Here the L2- norm is over the imaginary line for continuous time systems and over the unit circle for discrete time systems. In this section we put aside the norm constraint (5.2) and analyze only the connection
between the stability of the system in Fig. 5.1 and interpolation theory. To define precisely internal stability and the related notion of well-posedness for the system in Figure 5.1, following [Fr] we introduce auxiliary signals tit E 1l".xt and 112 E 1l".xt as in Figure 5.2.
Ball and Rakowski
133
w u
,.....
v,
z
..... ~
fP
...
Y,
K
.;
.....
..... ,.
_
' I....
./
I'
u,
Y
....
vi
Figure 5.2 The diagram in Figure 5.2 is equivalent to the system of equations
+ 'P12U = 'P21W + 'P22U = 'Pn w
(5.3)
Z
Y - V2
KY=U-Vl.
Well-posed ness means that the system (5.3) can be solved for (z, u, y) in terms of (w, Vb V2) and that the resulting map
[~]
-+ [ ; ]
is given by multiplication by a proper rational matrix function 1t
(for the continuous time case) or by a rational matrix function 1t analytic at zero (for the discrete time case). Internal stabi1ity means that in addition this function 1t is analytic on all of u. Thus internal stability amounts to the assertion that the output signal z and the internal signals
U
and
yare uniquely determined and stable for any choice of stable disturbance signals w, Vb v2; for a more complete discussion we refer to [Fr] and [V]. By elementary algebra one can show that His given by the explicit formula
(5.4) where
~
= 1- 'P22K.
In particular the closed-loop transfer function Tzw from disturbance (and/or
reference) signal w to error z is given by
Tzw = 'Pn + 'P12K(I - 'P22K)-1'P21 (5.5)
=: Fp[K].
134
Ball and Rakowski
A standard assumption in the literature is that P 1 2 is injective (as a multiplication operator from 'Rn• x1 into 'Rn.x1) and that P21 is surjective (as a multiplication operator from 'Rnw x1 into 'Rn• x1 )j in particular, n" ~ n z and nil ~ nw. An equivalent assumption is that the linear fractional map K
--+
Fp[K] defined by (5.5) is injective.
IT P21 in fact is square and invertible, one can solve the system of equations
Puw + P12U = Z P21 w + P 22U = Y for (z, w) in terms of (u, y)j the result is
=z 1'21u + 1'22Y = w
1'uu + 1'12Y
where
l' = [P12 - Pu P;,?P22 PuP;,? ] -P;,?P22
In the language of circuit theory the transform P
--+
P;,?
l' amounts to the transform from the scattering
to the chain formalism (see [B]), and was the basis for the analysis in [BRS]. To remove the assumption that P21 be invertible, we use here the generalized transform to the chain formalism introduced in [BHV]. Since P 21 by assumption is surjective, we may add extra rows P~1 to P21 so that the augmented matrix function
[~~~]
is square and invertible. Define
P~2 of a compatible size arbitrarily
and set
£= [
~ :'~2l
:'1.1 ... ..
P21
: P22
P~1 : P~2 Here yO is to be considered as a physically meaningless fictitious signal created for mathematical convenience. Since
[~~~]
is invertible, we may solve the system of equations
Puw + P12U = Z P21 W + P22 U = Y P~lW + P~2U
= yO.
135
Ball and Rakowski
for (z,w) in terms of (u,y,yO). The result is
(5.6)
where
P=
[rn 'P21
r
P12
13 ]
P22
'P23
is given by
(5.6a) (5.6b) (5.6c) and
(5.6d) The system of equations (5.1) associated with the feedback configuration in Figure 5.1 can be expressed in terms of P as
(5.7)
0 [ -J
o
0 0 J
o ] [ VI W] + o
-K
-V2
[-J 0 0
In particular the closed-loop transfer function T zw from w to z works out to be
(5.8)
Tzw = [Pn K + P12, P13] [P21K + P22,P23]-1
We also remark that the assumptions on 'P imply that
P is
[P22 P23]
is square and invertible and that
injective as a multiplication operator from n.(n.+n w )xl into n.(n.+nv)xl, and that one can
always backsolve for 'P from
P. For more complete details we refer to [BHV].
Below, in this section we shall say that a square rational matrix function W is hjprOller if W is analytic and invertible at infinity and we are in the continuous time case, or if W is analytic
and invertible at zero and we are in the discrete time case. In addition we say that the square rational matrix function R is u-outer if both R and R-l are analytic on u (where u is the closed right half plane in the continuous time case and the closed unit disk in the discrete time case).
136
Ball and Rakowski
5.2 Stability of feedback systems and interpolation In this section we delineate the connections between internal stability of a feedback system
in Figure 5.1 and the theory of null-pole structure and interpolation developed in the previous sections. We assume that we are given a rational matrix function P
5.1 with P2I surjective and P I2 injective, and then define P
= [~~~ ~~~]
= [~ll ~12 P2I
P22
as in (5.6). We consider P as a block row matrix function (With PI
[~~:])
as in Section
: ~13] : P23
= [~~~ ~~~]
and P2
=
and apply the notions of extended null-pole structure for block row matrix functions
explained in Section 2. Define integers m, n, K, L by m = n.. ,n = nw,K = n .. - n .. ,L = nw - ny,
so that P has size (m + n)
X
(m - K
+ n) with Pll
of size m
X
(m - K), P12 of size m
X
(n - L),
etc. Let u be the closed right half plane (continuous time case) or the closed unit disk (discrete time case), and let (w,P,Q) = (C",A",A"B"r,p,Q) be an extended complete null-pole data set over u for the block row matrix function
P in
the sense explained in Section 2. Then in fact
(w, P, Q) has the finer block structure (w, P, Q) = ([
g~] ,A,., A"
[B+ B-1, r, [P+ P-1,
[~~])
where C+, C_, A", A" B+, B_, r are matrices of respective sizes mxn", nxn,., n". xn"., n,xn" n,x
m,n, xn, and n, xn,., and where P+, P_,Q+, Q_ are matrix polynOlnials of respective sizes K X m, K X n, m X L, n X L. The following is the main result of this section. THEOREM
5.1. Let P
= [~~~ ~~~]
with PI2 injective and P2I surjective be a rational matrix
function describing the plant in Figure 5.1, and define the rational block row matrix function P
= [~ll ~12
P2I equivalent:
P 22
: ~13] :
of size (m
+ n)
P23
(i) Pis stabilizable
X(m -
K
+ n)
as in (5.6). Then the following are
p(1l(m-K+n-L)xI(u) E91lLXI ) ofP satisfies: 0) 1lmXI(u) 0
(ii) The extended null-pole subspace S :=
(a) S n (1lmXI E9
C
E9
and
(b) PIlE91la .. (sn1l(m+n)XI(u») =OE91lnXl(u) wherePOED1la .. ([:]) = (iii) If (w, P, Q)
= ([ g~] ,A,., A"
[B+ B-1, r, [P+ P-1,
[g~])
is
&D. extended
of null-pole data over u for the bloclc row matrix functioll P, thell
[~].
complete set
Ball and Rakowski
137
w = (C+,C_,A",A"B+,B_,r,p+,p_,Q+,Q_) is a O'-admissible interpolation data set (see (3.12)). Moreover, ifP is stabilizable, the following holds true:
(1) A rational matrix function K stabilizes P if and only if K has a O'-coprime factorization K=NKDi/ with NK E 'R(m-K)x(n-L)(O') and with DK E 'R(n-L)x(n-L)(O') O'-biproper such that
(2) An m
X
n rational matrix function W is the closed loop transfer function T zw associated
with a stabilizing compensator K for P if and only if W is analytic on
0'
and satisfies the
interpolation conditions (3.1') - (3.5') associated with the O'-admissible interpolation data set w, and [0 In-L 01P-L
[lj] 111