This content was uploaded by our users and we assume good faith they have the permission to share this book. If you own the copyright to this book and it is wrongfully on our website, we offer a simple DMCA procedure to remove your content from our site. Start by pressing the button below!
(~) ~ c(IP(OI +I gradP(OI + 1) 0 and Vc > 0 we have
(19)
holds.
Since the definition of a polynomial of N -principal type involves only the various principal quasi-homogeneous parts Pq(O, inequality (19) remains valid if P is replaced by P + Q, N(Q) C 8(P) (of course, the constant c in (19) should be replaced by c(Q)). Hence, the proposition implies (i)==?(ii).
Remarks. 1) If N(P) is determined by an equation (a,q 0 ) ~ m, the above t heorem goes into Theorem 4.1.3. 2) Inequality (16) implies (16') However, inequality (16') may hold not only for polynomials of N -principal type. 3) We note that condition (A) is not used in the proof of the proposition. 4) When proving the proposition we shall incidentally obtain a new proof of Theorem 5.1.2 in application to the case of polynomials P having reguhir Newton's polyhedra.
§2. Estimates for polynomials of N-principal type in regions of special form When proving Proposition 1.5 in Chapter 4 for the case of two variables we first separated out special regions associated with the sides and vertices of Newton's
187
Operators of Principal Type Associated with Newton's Polyhedron
polygon, proved estimates of the type (1.19) in these regions, and then established that the exterior of a circle of a sufficiently large radius can be covered by a finite number of regions where the estimate was proved. Following the same plan we shall prove inequality (1.19) for the multidimensional case as well. However, since for n > 2 a polyhedron in IRn has not only faces of zero dimension and dimension n -1 but also faces of intermediate dimensions k, 0 < k < n- 1, all the constructions are substantially complicated. In this section we shall define axiomatically those regions where estimates of the type (1.19) will be proved. In §3 we shall prove that t hese regions cover the complement to a ball in IRn. In this way, along with Proposition 1.5, Theorem 1.5 will also be proved completely.
2.1. w-cones and •-cylinders. We associate with q E IRn the one-parameter transformation group
Let
1r
be a subspace of IR~. A set W C IRn \ {0} is called a rr-cone if
Tq(p)W
c
W
Vp > 0,
Vq E 1r.
We shall say that a subset V C W generates a rr-cone W if ry E V, q E rr, and p E IR+ such that = pq ry.
e
ve E W
there are
Definition. A rr-cone W C::: IR(e) \ {0} is said to be regular if it is generated by a compact set V not intersecting the coordinate planes, that is, more concisely, V c (IR \ {.O})n. Remark. In contrast to the generating set, the rr-cone itself may intersect coordinate planes. For instance, if e 1 = (1, 0, ... , 0) E 1r, then -e 1 E 1r, and W contains the curve e(p) = (ryJ/ p, T/z, •.. , Tin), ry E W, which intersects the plane {e 1 = 0} as p---+
+oo.
A function A( e) is said to be rr-homogeneous if
(1) The number d( q) is called the q-order of the function. If N(P) is Newton's polyhedron of a polynomial P, r
1r,
Chapter 6
188
Remark. If n = 3 and dim 1r = 1, we obtain an ordinary cylinder with compact base. If dim 1r = 2, then we have a region in IR3 bounded by two planes parallel to 7r.
We introduce the notation log~+= (log 1~11,
... , log l~nl),
(2)
and consider the mappings Log:
R(e) \ {0}
Exp:
IR(q)
---t
---t
IR(eH
1Rq
(~~log~+),
( q ~ ( eqt' ... 'eqn)).
(3) (3')
These mapping establish a one-to-one correspondence between regular 1r-cones in IR?e) and 1r-cylinders in IR(q)" More precisely, we have the following Lemma. (i) If W C IR(€) is a regular 1r-cone, tben w = Log W is a 1r-cylinder. (ii) If w C IR(q) is a 1r-cylinder, then W = exp( w) is a regular 1r-cone.
P·roof. (i) According to the definition of a 1r-cone, if~ E W then Tq(p)~ E W, whence log~++ qlogp E w Vq E 1r, Vp E IR+. Hence, it remains to show that the section of w by a plane >. transversal to 1r is a compact set. If the 1r-cone W is regular, then it is generated by a compact set V not intersecting the coordinate planes. Therefore v = Log V is a compact set in IR(q), and the projection of v on >. (coinciding with the section of w by the plane >.) is also a compact set. (ii) Denote by v the section of w by a plane>. transversal to 1r. It is obvious that W = exp(w) is a 1r-cone generated by V = exp(v). If vis a compact set in IR(q)' then V is a compact set in (IR \ {0} )n . 2.2. 1r-cones relating to Newton's polyhedron. If f(k) is a face of N(P) and l/(k) is its normal cone, then by 1r(f(k)) and 1r(V(k)) will be meant, respectively, the k-climensional and ( n ~ k )-dimensional hyperplanes containing r< k) and V( k). Lemma 2.1 allows us to establish the following assertions that will play an important role in what follows. Lemma. Let f(k) be a face of N(P) and let W be a regular 1r(l/(k))-cone. Tben for every compact set A C 1r(f{k)) there is R = R(A) > 0 sucb that
(4) Proof. In view of (2) , we have to select R such that (a~ (3, q)
< logR,
Vq E w = LogW,
Va, (3 EA.
(4')
Operato?'S of Principal Type Associated with Newton's Polyhedron
189
By the definition of a normal cone, we have (a- (3, q) = 0 if a, (3 E 1r(r(k)) and q E 1r(V(k))· Therefore it suffices to select R such that ( 4') is fulfilled for q belonging to the section of w by a plane A transversal to 1r(V(k))· According to the above lemma, this section is compact. Since a- (3 also runs over a compact set, R can always be selected in this way. The definition of a regular 1r-cone implies the "local" form of the condition that P is a polynomial of N -principal type. Proposition. Let r
(6) is called the polyhedral angle of r
IR(e)
is said to possess the property G(r(k), c:) (more
(a) U is contained in a regular 1r(V(k))-cone W; (b) Va E T+(r(k)) n 1r(r(k)) and any integral (3 E T+(r(k)) \ 1r(r(k)) the inequality
(7) holds. The main result in this section is the following l) If
the face rCk) is inessential, then according to Definition 1.5, condition (i) holds for it. angle (6) is formed by the intersection of those supporting half-spaces to N(P) which pass through the faces of maximum dimension on whose boundary rCk) lies. 2 )The
Chapter 6
190
Proposition. Let r
such that
(8) P:roof. 1. According to the above definition, U belongs to a regular n(V(k) )-cone W. By Proposition 2.2, there is a covering UW.A ::J W consisting of n(V(k))-cones W.A such that in each of them either (5) or (5') holds. Replacing U by U n W,x. we can assume, without loss of generality, that in U (or in the n(V(k))-cone W containing U) one of the conditions of Proposition 2.2 holds. 2. We first assume that
PrckJ
f.
0 ve E V C W
(9)
We shall prove that in this case the inequality (10)
c:
is fulfilled provided that is sufficiently small. We first of all note that 3c0 > 0 such that ve E W we have
(11) In view of the n(V(k))-homogeneity, it suffices to find c0 such that (11) holds on the generating set V of the cone W. By virtue of the compactness and condition (9), it is always possible to select such c0 • Combining (4), (7), and (11) we conclude that
We shall show that for a sufficiently small
c: we have (12)
whence ( 10) will follow. Fixing a E n(r(k)) n T+(r(k)) and applying Lemma 2.2 we find that IP(e)- PrckJ(OI
~
L
laplle"l
~ c:(L: lapi)IC~I
PEN(P)\f(kJ
~ c:co ( L provided that c:co~lapj
lap!) IPrckJ(e)l <
~ IPrckJ(OI
(12')
< 1/2. Inequality (12) is a trivial consequence of (12').
Operators of Principal Type Associated with Newton's Polyhedron
191
3. Let (5') hold in U and let J 1, l = 1, ... , s, be the sets of indices of the essential variables of the face f(k). By the hypothesis, in every set there is an index, say 1 such that for ~EVcW. (13) We put p(l) = 8P/86, and let N(P
It follows that ( cf. the derivation of (ll)) (14) Denote by T~) (1( k)) the intersection of the polyhedral angle of the face N(P(l)) with IR(a)+. It follows from (7) that
l~p I < cl~al
v~ E
u,
1( k)
of
\Ia E T~l) ( '(k}) n 7r( '(k})
\1{3 E (T~')(I(k)) \ 1r(1(k))) n
zn.
(15)
Similarly, ( 4) implies that 3R > 0 such that (16)
It follows from (15) and (16) ( cf. the derivation of (10)) that for a sufficiently small c;
we have
3y~l(r(kl)(e)::::; cl ~~(e) I V~ E U.
(17)
Performing the summation of inequalities (17) over l = 1, ... , s we find
(18) where
s
v(f(k))
is the convex hull of
UT~)(
(19)
l(k)).
1=1 1 lThe
extension of the normal cone can appear only in the case when nate hyperplane which does not intersect the face f(k) .
-y(k)
intersects a coordi-
Chapter 6
192
We now show that
(20) where rCk) is an arbitrary essential face of N(P). Inclusion (20) and inequality (18) imply that (21) 36(?)(0 ~ const Igrad P(OI v~ E u. 4. We proceed to the proof of inclusion (20). The definition of the polyhedrons implies that
T~1\·yC k))
where J = J(l) U · · · U J(s). We begin with the case when the face f(k) do_!s not lie in the coordinate planes. Here, according to Lemma 1.3, we have Vk = Vk and rp.inqj = m~n qj. Using the definition of the function dp(q) we see that in this case 1EJ
1~1~77
we have v(f(k)) = {a E IR(a)+, (a, q) = dp( q), Vq E
It is clear that the polyhedron
V(k) }.
"6( P) determined by the inequalities
is contained in (22'). The case of faces lying in coordinate planes reduces to the above. Indeed, let a face r
Since the face f(k') lies in none of the coordinate hyperplanes, what has been proved implies that
8(P)
C v(f(k')),
where v(f(k')) i~ the polyhedron (19) corresponding to the face :r
v(f(k))
and v(f(k'))
Operators of Principal Type Associated with Newton's Polyhedron
193
Lemma. Let a face r
let
r
= r
E
I}.
(24)
Let ~ 1 , l E I be an essential variable of the face r(k). Then~~ is an essential variable of r
IR+ n l/(k)
such
l~j~n
It follows from (24) that l/(k)
= {q =
q'
+ q", q' = (q~, ... , q~) E l/(k')'
q" =
L biei, bi ~ 0 }· iEI
If q1 = min qi and l E I, then q~ = qt = min q~. Since r(k') does not lie in the coordinate planes, we have V{k') = V(k')· Once again using the definition of essential variables we conclude that ~~ is an essential variable of the face r
I(R)
= {~
E !Rn, l~il ~ R,j
= 1, ... , n},
Hence, the desired estimate (1.19) is implied by the following Proposition. Vc > 0 there is R = R(c) sucl1 that !Rn \ I(R) can be covered by a finite set of regions U>.. each of which possesses the property G(r\k),c) for some senior face r\k) c N(P). The next §3 is devoted to the proof of the proposition.
§3. The covering of Rn. by special regions associated with Newton's polyhedron In the foregoing section we associated with each face r(k) of Newton's polyhedron N(P) of a polynomial P a class of regions possessing the property G(r(k), c). For a sufficiently small c we established for polynomials of N -principal type an estimate of the form of
(1) in the regions
nc
G(r
(i) indicate an effective method for constructing regions possessing the property G(r(k), c); (ii) show that by means of a finite set of such regions we can cover the complement of any compact set in !Rn, for instance, of the cube
I(R)
=
{~ E !Rn, l~il
where R depends on c.
< R,j
= 1, ... , n},
194
Chapter 6
Then for an adequately chosen constant c we obtain the inequality
i.e. Proposition 1.5 together with Theorem 1.5 will be proved. We shall in fact introduce a class of polyhedral regions in IR(q) possessing a property g(f(k), c) and going into regions possessing the property G(f(k), c) under the exponential mapping (2.3 1 ). We shall show that by means of a finite number of such regions it is possible to cover the complement to the translated negative coordinate n- hedron
i_(r)
= {q
E !Rn,qi ~ r,j
= 1, ... ,n}.
(2)
3.1. The property g(r
regions, i.e. regions that are intersections of afinite number of (closed) half-spaces; in what follows, when speaking of regions in R(qJ we shall mean polyhedral regions. Let 1r be a subspace of R(q), dim 7r = n - k. As was noted in the foregoing section, a region C C R(q) is called a 1r-cylinder if (a) Cis invariant relative to translations along 1r, i.e. coincides with its cylindrical hull C = ( (__,ry) 1T' def = { q = qI
+q
II
,qI E
c ,q
II
E 1r } ;
(3)
(b) the section of C by any k-dimensional hyperplane transversal to 1r is a compact set (i.e. a bounded polyhedron). Let f(k) be a face of N(P) and let V(k) be the polyhedral angle of normals to f(k). We shall say that a region u C R(q) possesses the property g(f(k), c) if (i) there is a 7r(V(k))-cylinder C such that u C C; (ii) Va E T+(f(k))n7r(f(k)) and any integral f3 E T+(f(k))\7r(f(k)) the following inequality holds:
(a- (3,q) > log(l/c) Vq E u.
(4)
3.2. Semi-cylinders. Let 7r be a subspace in IR(q) and let 1r + and 1r _ be the complementary half-spaces of 1r. A region Vis called a 1r+ semi-cylinder if (a) D = (V)1T'+ def {q = q1 + q",q1 E V,q 11 E 1r+}; (b) (V)1T' (see notation (3)) is a 7r-cylinder (i.e. the section of (V)1T' by a plane transversal to 7r is compact). (c) for any half-space 7?+ C R(q) transversal to 1r and containing 1r+ there is a translation S1r+ of the half-space such that D C S1r+.
Operators of Principal Type Associated with Newton's Polyhedron
195
Remark. Let 11"+ and 7r_ be the complementary half-spaces of 1r and let 81r+ be the boundary of 11"+ (and 7r_). If V± are 11"± semi-cylinders and (V-)7T = (V+)1T, then v + n v- is a 811"+-cylinder. ·'VIie indicate a natural method for constructing a semi-cylinder from a 1r-cylinder C. Let 11"+ be a half-subspace of 1r and let R be an arbitrary half-space of R(q) containing 1r + and transversal to 1r. Then the intersection of C with the translated half-space ·R is a 1r+ semi-cylinder. This operation can be repeated several times. The intersection and union of 1r-cylinders and 1r+ semi-cylindered (having the same name) do not fall outside these classes of sets. The above definitions trivially imply the following Lemma. Let 1r be a subspace of R(q) and let 1r 0 be a subspace of 1r of codimen-
sion 1; let 11+ be a subspace of 1r transversal to 1r 0 , let C be a 1r 0 -cylinder, and let M be a J.l+ semi-cylinder. Then the intersection C n M is a 7r~ semi-cylinder where 1r~ is a half-space of 1r 0 lying in 11+.
Let V(l) be a polyhedral angle in R(q)' dim V(l) = n -1, and let V{}+I)' ... , V{{+I) be its faces of dimension n - l - 1. Denote by 1r~, ... , 1r:J_ the half-subspaces of 7r(V(o) corresponding to the faees V(~+l)' ete. Then
v;
1
= 1r+
n · · · n 1r+J .
(5)
Definition. _A region V is call~d a V(l) semi-eylinder if V V 1 n · · · n VJ, where Vi are 11"~ semi-cylinders (1r~ are those in (5)), all the cylinders (Vi)1T(\t(l)) coineiding. In the further presentation the following assertion plays an important role.
Proposition. Let r
1 Vq E V, c Va E T+(r
(a -
f3, q) > log -
(6)
\1(3 E (T+(r
r}'+
1), j = 1, ... , J, be those faces of N(P) of dimension l + 1 on Proof. Let whose boundary r
normals lying on the boundary of V( 1), and let 1r~ be the half-subspaces of 1r(V(l)) corresponding to V{{+ 1) so that (5) holds. l)If
l
= n- 1, then J = 1 and rj1+1 ) = N(P) .
Chapter 6
196
In each plane 7r(rjl+ 1 )) n T(fU)) we take a set tions are fulfilled: 1) /j (j = 1, ... , J) do not intersect 1r(r(l)); 2) the convex hull of /l U · · · U /J contains
/j
such that the following condi-
To prove the proposition it suffices to construct Vj a 1r~ semi-cylinder Dj C C such that 1 (6') (a - f3, q} > log for f3 E 1 j, q E 1J j. £
Then 1J = n1Ji is the desired V( 1) semi-cylinder. To construct Dj we take an arbitrary element qo E 7r~ \ 81r~. According to the definition of the half-space 1r~, we have
We note that (a- /3, q0 } does not depend on a (since (a, q0 } = const for a E 1r(f(l)), q0 E 1r~ C 7r(V(l))· By virtue of the compactness of /j, 3b > 0 such that (a-
/3, qo) > b
Va E 1r(f(l)),
V/3 E 'Yi.
Let Cj C C be an arbitrary 1r~ semi-cylinder and let Dj = Cj + Lq 0 • If L = L(c:) is sufficiently large, then inequality (6') holds for q E 1Jj. The proposition is proved. 3.3. Some additional remarks. 1) Let V( l) be determined by ( 5) and let 7?~ be the extension of the half-subspace
1r~ to a half-space of IR" transversal to 7r(V(l))· Let R+ be a translation of 7?~ . ......
The region 1J = 1J n R+ is called the truncation of the V(t) semi-cylinder 1J in the direction of 7r~. As can easily be seen, f> is a V{t) semi-cylinder. When proving Proposition 3.2 we have in fact established that by means of the operation of truncation in the directions of 1r~ it is possible to obtain from an arbitrary V(l) semi-cylinder V 0 C C (where C is a 7r(V(l))-cylinder) a V( 1) semicylinder 1J possessing the property g(f(l), £ ). 2) Let r
197
Operators of Principal Type Associated with Newton's Polyhedron
to r<.l). We note that on every such hyperplane Qj there lies a face of maximum J .
dimension of the polyhedral angle V(~) corresponding to r}o).
3) Thus, if r
~~
= {q E ~n,qj
~
O,j
= 1, ... ,n}.
(7)
Proof. By virtue of the regularity of N(P), the origin {0} = r~o) is the only minor vertex of N(P). Since t he coordinate hyperplanes {aj = 0}, j = 1, .. . ,n, are the only faces of maximum dimension passing through r~O)' we have Vo(O) = ~~. It remains to note that all minor faces of N(P) lie in coordinate planes of various dimensions and pass through the origin. 3.4. Constructing covering by regions possessing the property g(r
Theorem. For any t: > 0 there is r = r(t:) such that the region ~n \ i_(r) 1 ) admits of a covering by a finite set of regions V>.. each of which satisfies the condition g(f~k),t:) for a certain senior facef~k) C N(P). The theorem will be proved by induction. We shall proceed from the covering of ~n \ i_ (O) by the polyhedral an!~les of normals V({) corresponding to the vertices of
N(P). At thelthstepweshallobtainacoveringof~n by "final" V({) semi-cylinders, k ~ l - 1 (they do not change in the further rearrangements) and "preliminary"
V({)
semi-cylinders appearing at the foregoing step.
truncation in the directions corresponding to the faces we cut out of the "preliminary"
V({)
V({)
of maximum dimension
semi-cylinders the "final" V{t) semi-cylinders
possessing the property g(r)1), c). 1 )For
Applying the operation of
the definition of the region i_(r) see (2).
198
Chapter 6
We now show (and this is the geometrical basis for the induction) that the part of a V(z) semi-cylinder that remains after a certain truncation of that semi-cylinder is removed is covered by the V({+l) semi-cylinders corresponding to the (l +I)dimensional faces on whose boundary
r
lies.
Le1nma. Let V(l) be a polyhedral region (5) , dim V(z) = n - l, and let
j
=
V({+l)'
1, ... , J, be the faces of V( I) of maximum dimension corresponding to the half-
spaces 1r~. Let V = nVi be a V(l) semi-cylinder and let V be its truncation in the direction of a half-space R+ which is a translation of the half-space passing through 1ri and transversal to 1r(Vz). Then there is a V(7+I) semi-cylinder V such that
?ri
,..... vcvuv.
(8)
Proof. Let V(~~l)' ... , V(~+l) be those faces of V(l) of maximum dimension for which the dimension of their intersections with V(~+l) are maximum: s = l, ... , m.
Denote by R_ the complementary half-space toR+· We set
Then inclusion (8) is obvious, and it remains to show that
iJ is a
V(~+l) serm-
cylinder. To this end we denote by .Ai, ... , .A~m the half-subspaces of 81ri bounded by the intersections 81r~- n V(~+l)' s = 1, ... , m. Then TT k V ( l+ 1)
We shall show that Indeed, we have
=
\itn
A+
• • •
n\im
A+ •
iJ is representable as an intersection of
.A~ semi-cylinders.
(9) According to Remark 3.2, :, R- n Vk is a 81ri -cylinder, and, by the conditi()n of the lemma, Vi$ is a 1r~ semi-cylinder. Applying now Lemma 3.2 to 1r = 7r(V(o), 1r0 = 81ri, 1r~ = .A~, f.-l~ = 1ri., C = R_ n Vk, and M = Vi• we find that R_ n Vk n Vi· is a .A~ semi-cylinder. Therefore region (9) is a V(7+l) semi-cylinder. The lemma is proved. The proof of the theorem. The general induction scheme has already been outlined, and it only remains to show that one can confine oneself to semi-cylinders
199
Operators of Principal Type Associated with Newton's Polyhedron
satisfying the condition g(f(k), £) where f(k) runs over the set of the senior faces of N(P). ~ So, let r~O)' ,\ = 0, ... 'Ao, be the vertices of N(P), the vertex r~O) = {0} being minor and the other vertices being senior. It is clear that Ao
!R(q) =
uV(~)
A=O
(V{o) are closed polyhedral angles). As has already been mentioned, whence
V(~)
=
lR~,
uV{~)· Ao
Rn \ JR~ C
A=l
Based on Proposition 3.2, we cut out of each of the polyhedral angles V(~) (which are
V(~) semi-cylinders) polyhedral regions 1J~A)
C
g(f~O), £) (by means of truncation in
the directions corresponding to the faces of V{~) of maximum dimension). According to the lemma, the set
is covered by a union of V(~) semi-cylinders, /-ll
=
1, ... , M 1 • According to Corol-
lary 3.3, the V(';) semi-cylinders corresponding to the minor faces r~l) (they lie on coordinate axes) are contained in translations of the n-hedron (7). Hence, after the first step there remains a finite set of V(';) semi-cylinders corresponding to the senior one-dimensional faces of N(P). Continuing this process and using Corollary 3.3 at each step we arrive at the nth step at which there appears a {0} semi-cylinder, i.e. a bounded polyhedron. Since the latter is always contained in region (2) (provided that r is sufficiently large), the theorem is proved completely. Remarks. 1) Let r
01ri
V(,)
=
1ri
n
7ri.
jEJ
The geometrical meaning of the transition from V{l) to
V(l)
consists in discarding
the faces of V(z) corresponding to the minor faces r~l+l) on whose boundary r
Chapter 6
200
In this case no semi-cylinders corresponding to mmor faces appear (and, accordingly, Corollary 3.3 is no longer needed). 2) In the theorem we have constructed a covering of IRn by closed polyhedral regicns 'D>., . Examining the proof of the theorem one can readily see that the covering can be constructed so that the open parts of 'D>., cover IRn . 3) The regions D>.. constructed in the theorem are polyhedral, I.e. they are determined by a finite systems of inequalities of the form of
V{t)·
j = 1, ... 'J>.,,
(10)
where the vectors z(>..,j) and the numbers R>..j are determined up to within a normalizing factor, and R>..j = R>...i(c:). In view of the remarks in Section 3.3, as the vectors zC>..,j) c IR(a) one can take only the direction vectors of the various one-dimensional faces (both senior and minor) of N(P). If 'D>.. corresponds to a facer~) of dimension l > 0, then among inequalities (10) there must be such that differ in sign. In other words, V>.. C g(f~) , £)is determined by a system of inequalities i = 1, ... , I>..,
(11)
j = 1, . . . 'J>.,.
(11')
The vectors zC>..,i) correspond to the one-dimensional faces belonging to f~), and zC>..,i) correspond to the one-dimensional faces adjoining r~). 4) Since N(P) is Newton's polyhedron of a polynomial, it has only integral vertices. Therefore as the direction vectors of one-dimensional faces of N ( P) one can also take vectors with integral and, which is more, even components. Here, we can assume, without loss of generality, that the vectors z(>. ,j ) in (10) (or in (11)) h ave only even components.
§4. Differential operators of N-principal type with variable coefficients In this section we consider differential operators with coefficients belonging to
c=: P(x,D) = Laa(x)Da,
(1)
whose symbols P(:x; 0 are polynomials of N -principal type at every fixed point x E IRn . Under the additional assumption that the coefficients in senior monomials of the polynomial P( x ; 0 are real we shall prove a multidimensional analog of L 2 estimate ( 4.3.3) . A simple modification of the argument in §4.4 makes it possible to extend the estimate to the scales of HI-L and to prove an analog of estimate (4.4.3) and a local solvability theorem generalizing Theorem 4.4.1. We shall not dwell on these questions and leave the proof of the indicated theorems to the reader as an exerc1se.
Operators of Principal Type Associated. with Newton's Polyhedron
201
4.1. The statement of the basic result. As in §4.3, with a symbol P(x; 0 we associate the polyhedra N(P(x)), 5(P(x)), and 8(P(x)) at each point x E Rn and denote by N(P), 5(P), and 8(P) the convex hulls of the unions of the indicated polyhedra over x E Rn. Definition 4.3.1 is extended trivially to the case n > 2, i.e. operator (1) is called an operator of N -principal type if (i) N(P(x )) = N(P) Vx ERn; (ii) P(x 0 ;0 is a polynomial of .N-principal type Vx 0 ERn. Recall that condition (i) means, in particular, that if c/i)(x), j = 1, ... , J, are the senior vertices of N(P), then a 0 ci)(x) i=- 0, x ERn. Condition (ii) means, in particular, that the polyhedron N(P(x 0 )) is regul~r. By virtue of (i), the polyhedron N( P) also possesses this property. As in Chapter 4, we impose on the symbol P(x; 0 an additional condition, namely Condition (R). If an integral point a E N(P) is not minorl), then aa( x) is a real function. Theorem. Let (1) be an operator of N -principal type and let the additional condition (R) be fulfilled. Then Vc > 0 3w(c) such that in a region n of a sufficiently small diameter, diamn::::; w(c:), the inequality (cf. (4.3.3))
lluii6(P) ~ c:llP(x, D)ull Vu E V(f!) holds, where
lluliF
(2)
j 3F(P)(01u(01 d~. 2
This theorem automatically implies the multidimensional generalizations of Corollaries 1 and 2 in Section 4.3.1, i.e. for any differential operator Q(x; D) such that N(Q(x;~)) C E(P), the inequality
llu ii6(P) ~ cii(P + Q)(x, D)uii
VuE V(f!), diam f2 < w(c:, Q)
is fulfilled. Since, by virtue of condition (R), the symbols of the operators P and P* differ in minor terms, inequality (2) implies an analogous inequality for the adjoint operator P* and, consequently, for the transposed operator tp.
Remark. In the course of the proof we have incidentally established an estimate for N quasi-elliptic operators:
c
L
IIDaull ~
IIP(x, D)uli
VuE V(f!).
aEN(P)
l)That is integrally minor in the terminology of Chapter 4.
202
Chapter 6
4.2. Microlocalization of estimate {2). With account of (i), the results of §§2 and 3 can be unified to state the following Proposition 1. Under the conditions of the theorem there exists a finite covering {U1}, j = 1, ... ,J, ofthe complement ofthe cube l_(R): J
JR(€) \ l_(R)' c
U Uj, j=l
such that in each of the regions Uj one of the following two conditions holds: V~ E Uj,
P(x,O > co3N(P)(0,
lgradP(x , OI > Ct38(P)(0,
lxl < bo,
v~ E Uj,
(3)
lxl < bo.
(4)
In the Appendix to the present chapter we prove Proposition 2. There exists a generalized partition of unity {1/; j ( 0}, 0 ~ j ~ J, subordinate to the covering in Proposition 1 ( cf. Section 4.3.2), i.e. satisfying the following conditions: (i) V; 1( 0 E c=; (ii) 'l/Ji(O;::: o, supp'l/Ji c U1, Uo = I_(R); (iii) there is K > 0 such that J
J{-l
~ L1/Ji(0 ~ K;
(5)
j=O
(iv) there is p, 0
~
p
~
1, such that 0< p
(v) for any
a> 0 and j3
~
1;
(6)
E N(P) we have
(7) Theorem. Let the conditions of Theorem 4.1 be fulfilled. Let the covering {Uj} and the generalized partition of unity {'l/Jj} satisfy the conditions of Propositions 1 and 2. Then,.\/,c > 0 3w(c) such that Vj = 1, ... , J the inequality
(8) holds in a region n, diamn
< w(c), where t > n/2.
Remark. As in the remarks in Section 4.3.3, we assume that the coefficients of the operator p belong to c= and are uniformly bounded on ]Rn together with all their derivatives.
203
Operators of Principal Type Associated with Newton's Polyhedron
The reduction of Theorem 4 . 1 to the above theorem is carried out by means of an almost literal repetition of the argument in Section 4.3.3, and we do not dwell on this here. The proof of estimate ( 8) under condition ( 3) encounters no serious difficulties and is a simple modification of the argument in Section 4.3.4. Thus, the proof of the main Theorem 4.1 reduces to proving inequality (8) on condition that the symbol P( x, 0 satisfies inequality (4) in the region Uj. 4.3. The proof of estimate (8) under condition (4). To contract the notation we shall write '1/J instead of '1/Ji and also v = '1/J(D)u. The general scheme for the derivation of the estimate is in many respects analogous to the case of real operators of principal type (see Hormander (2] or Egorov [2]) and is based on an identity that will be derived below. Lemma 1. We have the identity n
'E IIP(j)(x,
n
D)vll 2
j=l
=
L Im[xjP(x, D)v, p(i)(x, D)v] j=l n
n
j=l
j=l
- L ImJxip(j)*(x, D)v, P*(x, D)v] + L Re[P(i)*(j)v, P*v] n
+ Llm[xjv,[PU),P*]v],
(9)
j=l
where pU) is the operator with symbol 8P(x; 0/Bej, p(i)* is the adjoint operator of pU), and the symbol p(i)*(j) is obtained by differentiating the symbol pU)* with respect to ei; [, ] designates the Hermitean scalar product in L 2 . Proof. For any differential operator we have P(x, D)(xjv) = XjP(x, D)v- iP(j)(x, D)v. Multiplying scalarly by p(j)(x; D)v and taking the imaginary part we obtain
IIP(i)(x, D)vjj 2
= Im[xjP(x, D)v, pU)(x, D)v] - Im[P(x,D)(xjv),P(i)(x,D)v].
(10) ~·
!,-·
Integrating by parts we transform the second term on the right-hand side in the following way:
- Im[P(xjv ), pU>v] = - lm[xjv, P* pU>v]
== -
+ Im(x jV, (P(j), P*]v] Im[x jpU>*v, P*v] + Re[P(i)*U>v, P*v] + Im[x jV, [P(j) , P*]v]. Im(P(j)*(x jV ), P*v]
204
Chapter 6
Substituting into (10) and performing the summation over j we arrive at identity
(9). We now estimate separately the various terms in identity (9). The most difficult problem is to estimate the last term on the right-hand side of (9). We begin with estimating the left-hand side. Lemma 2. Let v = '1/;(D)u, u E 'D(O), and let inequality(~) be fulfilled on the support of the function '1/J(O. Then \It > n/2 \/w, I<1, and I
L
IIP(j)(x,D)vll 2 > K1llvii~(P)- I
(11)
j=l
provided that n is a sufficiently small region, i.e. diam n
~
w.
P·roof. Assume that the origin belongs to the region n (if otherwise, Xi in ( 9) should be replaced by Xj ·- x~, j = 1, ... 'n, where x0 = {x~, ... 'x~) En). Set ting
P(D)
= P(O, D)
and using inequality (4) obtain n
llvii~(P) ~ c;.- 2
L IIP(j)(D)vll
2
j=l n
~
2c;.- 2
L
n
IIP(j)(x, D)vll 2
+
2c;.- 2
j=l
L II(P(j)(x, D)- pU)(D))vll
2.
(12)
j=l
Consider a truncating function x(x) E 'D equal to 1 for lxl ~ w 0 and to zero for lxl > 2wo. Then the last term on the right-hand side does not exceed n
4c1
2
L llx(P(j)(x, D)-
n
pU)(D))vll 2
+4c1
j=l
2
L 11(1- x)(P(i)(x, D)- p(i)(D))vll
2.
j=l
(13) We note that
x(P(j)(x, D)- p(i)(D)) =
L
cf3(x )Df3,
max lcf3(x )I
= O(wo).
{3E6(P)
Taking~ sufficiently small w 0 we estimate the first term in (13) from .above by means of llvii~(P/2. Further, if Wo > w > diamn, then the symbol (1- x(x))(P(i)(x; 0pU) ( 0 )~( 0 is equal to zero on the support of the function u E 'D( n). Using the
property of pseudo-locality of the corresponding operator (based on property (6) of the function '1/; = '1/;j) we estimate the second term in (13) from above by means of const llull(-t), t > n/2. Substituting these estimates into (12) we arrive at (11).
205
Operotors of Principal Type Associated with Newton's Polyhedron
Lemma 3. Let the conditions of Theorem 4.2 bold. Then Vc
> 0 3w(c) such
that in a region n, diamn::::; w(c), the right-hand side of identity (9) is estimated from above by means of
ciiP(x, D)vll 2 + Ccllvii}(P) + c(c)llull~-t)'
(14)
where t > n/2, v = 1/J(D)u, and the function 1/J satisfies conditions of the type (6) and (7). Comparing Lemmas 1, 2 and 3 and assuming that constant in (11)) we arrive at (8).
Cc < KI/2 (where
K 1 is the
The proof of the Lemma 3. 1) Estimation of the first term on the right-hand side of (9). As in the proof of Lemma 1' we take the truncating function x( X). We have
Im[xjP(x,D)v,P(j)(x,D)v] ( llpU>vllllxjPvll
( c3llvii6(P) llxxiPvll + c3llvllg(P) 11(1- x)xjP~(D)vii·
(15)
Take 280 , the diameter of the support of X, so that lx j XI ( c. Then the first term on the right-hand side of inequality (15) does not exceed (15') By virtue of the pseudo-locality of the operator Xj(1- x)Pl/J(D), the last term on the right-hand side of (15) does not exceed (15") Substituting (15') and (15") into (15) we estimate the left-hand side of (15) by means of expression ( 14). 2) Estimation of the second term on the right-hand side of (9). Repeating literally the above estimation we show that
If condition (R) 1 ) is fulfilled, then
P*(x, 0
= P(x, 0 + L P~:~(x, 0/a! = P(x, 0 + Q(x, e),
(17)
a>O
where Q is a polynomial symbol in Therefore
e, and we have N(Q(x; 0) c
IIP*vll ( IIPvll + const llvii6(P)" l)Note that up to now we have not used this condition.
8(P) for all
X.
(17')
Chapter 6
206
Substituting (17') into (16) we estimate the left-hand side of (16) by means of expr;o;ssion ( 14). 3) The estimation of the third term on the right-hand side of (9). By Schwarz' inequality, we have (18) The symbol of the operator pU)*(j) is a linear combination of the monomials corresponding to the minor points of the polyhedron N(PU>*) = N(PU>) C E{P). It follows that IIP(j)*(j)vll ~ c4 IID 11 vll. (19) fjE6(PCi))
L
By virtue of the regularity of the polyhedron b(P), Vc and V/3 E 8(P(j)) there is a constant c;1( c) such that
It follows that
Substituting these inequalities into (19) we see that (19') Substituting (19') into (18) and estimating IIP*vll by means of (17' ) we obtain
Re[P(j)*(j)v, P*v] ~ cscllvii6(P) I!Pvll
+ C7cjjvii}(P) + c6(c )IIPvllllull(-t) + cs( c)jlvii6(P) llull( -t) ~ ciiPvll 2 + c(c7 + c~/2 + 1)jjvii}(P) + (c - 1 c~(c) + c- 1 c~(c ))llu11(-t) ' which proves the desired estimate. . 4) Thus, to complete the proof of the lemma we have to establish the inequality
4.4. The proof of estimate {20). To begin with, we consider in detail the structure of the commutator of the operators p(i) and P*.
207
Operators of Principal Type Associated with Newton's Polyhedron
Lemma 1. The symbol Hj(x; 0 of the commutator [P(j), P*] can be represented as (21) Hj(x, 0 = Q(x, 0 + R(x, ~),
where the symbol Q can be written in the form
Q(x,O =
L
qap(x)~a+P.
(22)
aEli(P) f3Eli(P)
The symbol R is written
(23) where f3 E N(P) and the (integral) multiindices a have the form a=a I - aII - aIll ,
a I E N(P) . ,
a II ,aIll
> 0.
(23')
Proof. We first of all note that if the condition (R) is fulfilled, then
P*(x; D)= P(x; D)+ Q(x; D), where Q is a linear combination of the operators Da, a E [P(i), P*] = [pU), P]
~(P).
Therefore we have
+ [pU), Q].
The symbol of the commutator [pU), Q] has the form
I)p(j)('y)Q<-y)- P<~jQ('y));,, -y>O
and is obviously representable as (22). The symbol of the commutator [P(i), P] has the form p(i)(-y) P('Y)/1!p(~jph) ;,!
'I:
L
-y>O
-y>O
Here the second sum is of the form of (22), and the first sum has the form (23), where in (23') we have a' E N(P), a" = ej, and a 111 =I· By virtue of the above lemma, the proof of inequality (20) is implied by the following lemmas.
Chapter 6
208
Lemma 2. Vc inequality
> 0 there is w(c.) such that in a region n, diamf! < w(c.), the
[xjq(x)v, Da+.Bv] ~ C}cllvii~(P)
+ Cz(c)llull(-t)'
a, (3 E 8(P),
v
= 'lj;(D)u,
u E D(D),
(24)
holds.
na
Proof. If the operation of differentiation is transferred to X jqV by means of integration by parts, then the left-hand side of (24) takes the form
As has already been done many times, we take a truncating function x( x) such that it is equal to 1 on the support of u(x) and the inequality jxjq(x)x(x)! < c:/2 holds. Then we have
[xjqDav, Dfiv] ~ IID.Bvll(llxjxqDavll + llxj(1- x)qDavll)
~ ~llvii~(P) + c(t)jjD.Bvllllull<-t) ~ cllvii~(P) + c(c:)llull(-t) · As to the terms in the sum corresponding to 1 argument as in the proof of estimate (19').
> 0, we can use in the case the same
Lemma 3. Under the conditiolJS of Theorem 4.2 Vc: > 0 3w( c) such that in a region n, diam n < w( c), we lwve
(25) where the multiindices a and (3 are of the form of (23').
Proof. If the vector a+ {J can be represented as a sum a' +{3', a', {3' E 8( P), then the desired assertion reduces to the foregoing lemma. Therefore we shall consider the case when no such representation is possible and the ordinary integration by parts does not help. 1) Put
(26) It is clear that
h(0 ~ const36(P)(~)
V~ ERn.
(27)
On the other hand, according to ( 4), we have h( ~)
> const 36(P) ( 0
for
~ E supp 'lj;.
(27')
Operators of Principal Type Associated with Newton's Polyhedron
Let us show that there is p, 0 < p ~ 1, such that V'Y
209
> 0 we have (28)
To prove (28) we note that the regularity of the polyhedron 28(P) implies that there always exists p > 0 such that
With account of inequality (27'), we conclude that
It follows that the function h( 0 = .jh2{Jj satisfies the inequality ( cf. the proof of Lemma 2 in the Appendix to §1.4)
By virtue of (27), we obtain (28). 2) Take a function <.p( 0 possessing the following properties: (i) <.p(O 1 forE E supp1/J, (ii) h(O > const3b(P)(0, E E supp<.p, (iii) l8"~<.p(E)I < c"~(1 + IEI)-Pbl. The construction of this function is carried out by means of the same procedure as in the case of the function 1/J = 1/Ji using the original partition of unity (see the Appendix to the present section). 3) We come back to the proof of inequality (25). Setting h 1 (0 = <.p(0h(0 we have
=
[x jrv, no+f3v] = [x jrv, <.p(D)h(D)h - l (D)Da+f3v]
= [h 1 (D)(xjrv), h- 1 (D)Da+Pv]
~ llhi(D)(xjrv)llllh- 1 (D)Da+Pvll·
(29)
4) Let us estimate the second factor on the right-hand side of (29). We note that if (23') holds. then a+(3E28(P) (30) ~
_.,
Indeed, if q E IR+ and min qi = 1, then
(q, a+ (3) = (q, a') + (q, (3) - (q, a") - (q, a"') ~ 2dp( q) - 2 = 2dp( q). Recalling the definition of S(P) we obtain (30). This inclusion implies that
Chapter 6
210
With account of (27), we obtain
Thus, if v = 'If;( D)u, then
(31) 5) V•/e now pass to the estimation of the first factor in (29). We have
(32) using the smallness of diam n and the truncating function X' x( X) = 1' X E estimate the first term on the right-hand side:
n, we (33)
Using the commutation formula we write N-1
[h1(D),xjr]v =
L
D'Y(xjr)h~-r\D)v/'Y! + RNv.
-y>O
Comparing (28) and property (iii) of the function
This inequality implies that
(34) Comparing again (28) and property (iii) of the function
holds. Therefore, according to Hormander [4], we have
(35) provided that the chosen number N is sufficiently large. Comparing (31)-(35) we arrive at (25). The lemma is proved.
211
Operators of Principal Type Associated with Newton's Polyhedron
Appendix Here we present the proof of Proposition 2 in Section 4.2 and construct a system of functions {1fj(~)} satisfying conditions (4.5), (4.6), and (4.7). We shall use the construction that was presented in Section 4.3.3 and in the Appendix to §4.3 for the two-dimensional case. As in the two-dimensional case, the central point of the whole construction relates to the regions corresponding to the zero-dimensional faces (vertices). The case of the faces r
(1) where the vectors [ilt =
(li 1\
1{1j(0 =
•• • ,
ltf) have even compone~ts. As in ( 4.3.10), we set
ece- R II B(exp([iiL,log~+)- RjJL),
(2)
2)
j
where B(t) E c=, B(t) ~ 0, B(t) = 0 fort< 0, and B(t) = 1 functions (2) is supplemented with the function
fort~
X.
The set of
(2') As was noted in Section 4.3.3, a special analysis is required for the verification of the fulfilment of the smoothness condition on the coordinate hyperplanes and the verification of conditions ( 4.6) and ( 4. 7). In what follows we shall assume that 1~1 > R, and therefore the first factor in (2) will be dropped. 2. As in Item 1 in Appendix to §4.3, we first verify inequality ( 4. 7) for (3 = 1 i.e. the inequality
(3) Its derivation is a literal repetition of the derivation of inequality (1) in the indicated Appendix. It follows from (3) that if there are w > 0 and p, 0 < p ~ 1, such that
(4) then (3) implies (4.6). 3. Consider a region Uj corresponding to a vertex r~o) not lying on the coordinate axe~. The normal cone of this vertex consists of positive vectors q E IR+, i.e. there is p such that
Since we have supp 1fi E Uj and the image of Uj under the logarithmic mapping ~ ~ (log 1~11, ... , log l~nl) is contained in the translation of V(~)' we have log ~~kl
> plog l~d -logwo
V~ E supp1{1j,
k, l = 1, ... , n.
(4')
Chapter 6
212
Inequalities (4') imply ( 4) and hence condition ( 4.6) for the functions 'lj;j. We now verify condition ( 4. 7). According to the hypothesis, we have. supp 'lj;i E Uj, where the region Uj possesses the property G(f~0 ),c:), which means (see Sec-
tion 2.3) that if a(A) is a coordinate of the vertex f~O), then
Hence, it suffices to verify ( 4. 7) for a = a(A). Since r~O) does not lie on the coordinate hyperplanes, all the coordinates ( a(A)l, ... , a(A)n) are positive, and consequently are no less than 1. Using inequality (3) for {3 = ({3 1 , ... , f3n), f31 ~ 1, we obtain By virtue of condition (4 }, the expression in the parenthesis does not exceed a constant. Multiplying both side of the inequality by le}:p..J I we obtain
4. We now consider the case when r~o) lies in a coordinate hyperplane of codimension n- m. Expand lR(o) as a direct sum: a= ({3, 1), {3 E IR(.B)' 1 E IR(1)m, and assume, to simplify the notation, that if a= (a1, ... , an), then {3 =(all ... , am) and 1 = ( am+l, ... , an)· Accordingly, the variables are divided into two groups:
e
e= (ry,(), "7 E Rm, ( E Rn-m.
Thus, let the vertex r~O) belong to the plane {am+l = ... = an = 0} and not belong to a coordinate plane of a higher dimension. Let us divide the onedimensional faces passing through f~O) into two groups, namely
r~l)' f1 = 1, ... '/11' belonging to {am+l = .. . =an = 0};
(5)
r~l)' f1 = /11 + 1, ... '/12, transversal to {am+l = ... =an= 0}.
(5')
In accordance with this division of one-dimensional faces we write: J.l.l
'1/Jjco =
'I/J]l)co'I/J)2 )co
=
II c1ejl' 1- RilL) II c1eil' 1- RilL).
(6)
iL=l
We note that the function 'lj;Y) depends only on the variables 1J (and does noi depend on the variables(). Denote by Nm the section of N(P) by the coordinate plane {am+l = · · · = an = 0}. Obviously, Nm is a regular polyhedron in Rm and r~o) is a senior vertex of that polyhedron not lying in the coordinate planes. Therefore the argument in Item 3 implies that
ITJd > w1l"lk IP 1 ,
1]
E supp 'lj;J 1),
l, k
= 1, ... , m,
0
<
Pl :::;; 1.
(7)
Operators of Principal Type Associated with Newton's Polyhedron
We now consider the function
'1/J?).
213
Let (!3(>. ), 0) be the coordinates of the vertex
r~o) and let (0, 'Y(J.t)), J1 = Jll + 1, ... ~ Jll, be the coordinates of the intersections of the straight lines passing through the one-dimensional faces (5') with the subspace {a1 =···=am= 0}. Denote by Nn-m the convex hull of 'Y(J.t)' J1 = J.11 + 1, ... , J.12, and the origin. The polyhedron Nn-m is the section of the regular polyhedron T+(f~)) (see (2.6)) by the plane {a1 =···=am= 0}. It is clear that Nn-m is a regular polyhedron in Rn-m. For an appropriate normalization of the direction vectors [J.t of the one-dimensional faces (5') we have J1 = Jll
+ 1, ... ,f.12·
Consequently, the function ~J2 )(0 in (6) has the form
~?\ry,() =
ll2
IT
8(ry2Pp..)(-21(1')- RJ.tj)·
(8)
J.t=J.tl+l
It follows from the definition of the function for
( TJ,
Among the vertices 'Y(J.t) there are vertices coordinate axes. Hence, (9) implies
(J
that (2)
( ) E supp'lj;j , 'Y(J.tt)
= 1"1e1, l
1= m
Jll
<
m
+ 1, . . . , n,
=
J1
<
J12·
(9) lying on
+ 1, ... ,n.
With account of (7), we have
l"lkl > w2l~tiPk,
k
= 1, ... ,m; l = 1, ... ,n,
~ E supp'I/Jj.
(10)
( E supp O~j/0~ 8 •
(11)
We now show that
l(sl > w3I6IPa,
8
= m + 1, ... , n; l = 1, . . . , n,
For definiteness, we shall assume that 8 = n. Differentiating (8) with respect to ~k and using the property that 8' (t) is identically,: equal to zero for t < 0 and t > x, we see that for every point ~ E supp {)~ j / {)~ n there is v, Jll + 1 ::::; v ::::; J1 2 , such that
Comparing this inequality with (9) we conclude that
l(')<.,l I > const l( 1<~>l I
VJ.1 = Jll
+ 1, ... , f.12·
Chapter 6
214
Since
I(JL)
are the vertices of the polyhedron Nn-m, we have
Since all the coordinates of the vertex l(v) are positive, we have l(v)n > 0. We select a point 1 = ( lm+l, ... , In) so that In < l(v)n and for some s the condition Is > l(v)s holds. Then we see that m
+ 1 ~ s ~ n.
(12)
Hence, we have proved inequality ( 4.6). We now proceed to the verification of inequality (4.7). Withol}t loss of generality, we can assume that a= (,Bp,) , O) (this follows from (9)). If among the components of ,Bin (4.7) there is .Bz ~ 1, 1 ~ l ~ m, then the desired estimate is proved using the argument in Item 3. Therefore we shall assume that ,B = (0, ... , 0, .Bm+l, ... , .Bn)· It suffices to consider the case I.BI = 1, say .Bn =en. Then we have
I~~:I (
t
const IO'(ry2P('lC2'<'l - Rv
)ll~nl-1'
v=Jtl+l
whence
The factor in square brackets is bounded and the other factor is estimated by means of S8(P)(0. 5. We now consider the case of the region corresponding to the face r
'1/Y?) .. . tf;JM)
where each of the factors is a function considered in Sections 1 to 4 and, consequently, sat isfies conditions of the type of ( 4.6) and ( 4. 7). It remains to note that the functions satisfying these con,ditions form a ring relative to multiplication. .
CHAPTER VII
THE METHOD OF ENERGY ESTIMATES IN CAUCHY'S PROBLEM §1. Introduction. The functional scheme of the proof of the solvability of Cauchy's problem 1.1. The present chapter is devoted to sufficient conditions for correctness of Cauchy's problem for differential operators with variable coefficients. In Chapter 2 (see Theorem 2.5.5) a general result on the solvability of Cauchy's problem was established. Under the assumption that the symbol satisfied the conditions of constant strength and exponential correctness we obtained a priori estimates in the H[~f norms for the original operator P and its formal adjoint operator P* (see (2.5.31) and (2.5.32) ):
:L IIP(a)(y; D)ull(s),-y ~ C:s(r)IIP(y; D)ull(s),')'l
'~ ro(s),
(1)
p ~ Po(s),
(1')
a>O
where y = (x,t), x ERn, t E R, and cs('Y), c::(p) ~ 0 as r ~ -oo, p ~ +oo. Although the existence and uniqueness theorems in §2.5 were proved by constructing the parametrix for the operator P, they can be in fact deduced directly from inequalities (1) and (1'). The condition of constant strength of the symbol used in the derivation of the above estimates is very stringent and is not fulfilled for strictly hyperbolic and, the more so, dominantly correct differential operators with variable coefficients. In this chapter we present a scheme for studying Cauchy's problem which does not use the condition of constant strength of the symbol and makes it possible to prove the correctness of Cauchy's problem for dominantly correct differential operators with variable coefficients. The approach in this chapter is based on a rather simple observation that to prove the correctness of Cauchy's problem in the spaces H[~f+ it suffices to have weaker estimates (as compared to (1) and (1')). For a natural[ we set p(l)(y;e,r)
def
p(o, ... ,o,l)(y;e,r) = 81P(v;e,r)/8rl.
By the solution to homogeneous Cauchy's problem
P(y,D)u = f
(2)
will be meant a distribution u with support in the half-space t ~ 0 satisfying (2) in the sense of distributions:
(u, tPv) = (J,v) Vv ED We have 215
(2')
Chapter 7
216
Theorem A. Let a differential operator P(y; D) and its formal adjoint operator P*(y; D) satisfy the a priori estimates m
C8
L("Yo -1') IIP(/)(y; D)ull(s), 1
1
~ IIP(y; D)ull(s), 1 ,
(3)
VuE HGJ),
1=1 m
c; L("Yo -"Y)IIP*(I)(y; D)vll< -s),-1 ~ IIP*(y; D)vll< -s),-1 , 1=1
(oo) Vu E H [-,] ' -~ ~ -"Yo,
(3')
where lsi ~ M and "Yo = "Yo(M). Then VM > 0 there is 1(M) such that Vf E H[~~+' lsi~ M , and 1 < 1(M) the homogeneous Cauchy problem (2) has a unique solution u E Hi~~+· Moreover, we have p(l)(y; D)u E H[~f+' l = 1, ... , m, and the solution satisfi~s inequality (3). Before presenting the proof of the theorem we .discuss the general scheme for derivation of estimates (3) and (3').
1.2. Estimates (3) and (3') are a consequence of more exact inequalities obtained by Leray's method of "separating operator" [1]. The method is based on the following elementary Proposition. Let P(~,T) be a polynomial in the solved with respect to the highest power ofT: P(~,T)
= Tm +
L
variables~ E
IR.n, T E C 1
aaj~o:Tm-i,
(4)
j~1,a
and let T
=a+ i1.
(5)
Then the conditions below are equivalent.
(I) Petrovski1's correctness condition is fulfilled, i.e. there is "Yo such that (6) (II) There is c, depending only on n and m (where m is the degree of P with respect to T), and a constant "Yo such that m
c
I) "Yo -1) 21 - 1 IP(l)(~,a + i1)l 2 ~ Hp(e,a,/'),
I ~ "Yo·
(7)
1=1
(III) There is lo such that
H p(~, a, 1) > 0 '
for
1 ~ /'o,
(C a) E JR.n+l.
(8)
217
The Method of Energy Estimates in Cauchy's Problem
Proof. (II)==;.(III)==;.(I). The first implication follows from the fact that p(m)(e, 7) m!, and the second implication is based on the property that Hp = 0 when P = 0.
=
(I)==;.(II) For any fixed
ewe factorize polynomial (4): P(e, 7) =IT (7- 7j(e)). m
(9)
j=l Differentiating (9) with respect to 7 we obtain m
p(l)(e, 7)
=LIT (7- 7j(e)). k=l
(10)
j:j:.k
Substituting (9) and (10) into (5) we find m
Hp(e,a,,) = L::c-,+lm7k(0) ITia+i,-r"j(01 2-
(11)
j:j:.k
k=l
If (6) is fulfilled, then Im7k(0 ~ /o, whence m
llo- '"p(l)(e,a + i/)12 ~ m(lo- 1)
LIT Ia +if- 7j(012 ~ mHp(e,a,,). k=l j#k
Differentiating consecutively (10) with respect to 7 we readily prove inequality (7) to full extent. Corollary. If polynomial (4) satisfies Petrovski1's correctness condition, then there are /o and x > 0 such that
where 1
~
/o - c, c > 0.
Proof. Differentiating ( 4) consecutively we obtain the triangular system
P{l)(e, 7) = m(m- 1) ... (m - l + 1)7m-l
+ 2,~)m- j) ... (m- j -1 + 1)aajea7m-j-I,
= 1, ... , m,
= 0, ... , m- 1, in terms ofp(l), l = 1, ... , m:
making it possible to express 7j, j 7j =
l
L ajk(OP(j+k)(e, 7), k
where ajk(O are polynomials in e. Taking the maximum degree of these polynomials as x and using (7) we derive inequality (12).
Chapter 7
218
1.3. If P(Dx, Dt) is a differential operator with constant coefficients, then passing to the Fourier transform we find
- Im[exp( 1t)P(D)u, exp( 1t)P(I)(D)u] =
jj Hp(~, cr, !)lu(~, cr + i1)l d~ dcr. 2
By virtue of Proposition 1.2, the right-hand side can be estimated from below by means of m
const L)lo- !? 1- 1 llP(l)(D)ull;. l=l
According to Schwarz' inequality, the left-hand side can be estimated from above by means of
Comparing these estimates we obtain inequality (3) with s = 0 for the operator P(D). Replacing u by Xj(D)u = (iDt + !o + + lDxl 2 ) 8 u in this inequality we obtain (3) with an arbitrary s E R . If the operator P(Dx, Dt) is correct in Petrovskil''s sense, then the operator P(Dx, -Dt) possesses the same property. Writing down an inequality of the type (3) for this operator and making change of variable t-+ -t we obtain (3'). The aim of the present chapter is to develop the indicated approach in application to operators with variable coefficients. We consider the quadratic form
Jl
- Im(exp( 1t)>.~(D)P(y; D)u, exp( 1t)>.~(D)P( 1 )(y; D)u]. Under some (rather cumbersome) conditions on the symbol P(y; ~' T) presented in §2 the form can be estimated from above and below by means of
where H p ( ~, cr, 1) denotes the value of the symbol
H p(y; ~' cr, !) = - Im(P(y; ~' T)P(I)(y; ~' T))
(13)
at a fixed point y = y 0 , whence inequality (3) is obtained comparatively simply. Inequality (3') is deduced in like manner. An analysis of sufficient conditions for t he validity of inequalities (3) and (3') leads to the following assertion.
219
The Method of Energy Estimates in Cauchy's Problem
Theorem B. Let a symbol P(y; ~' T), solved with respect to the highest power ofT: P(y;~,T) = Tm + LPj(y;~)Tm-j, j~l
satisfy the following conditions: (I) Vy 0 E JRn+l the polynomial P(y 0 ; ~' T) is correct in Petrovski1's sense; (II) symbol (13) satisfies the condition of constant strength, i.e. there are /o and A > 0 such that A- 1 ~ Hp(y';~,u,!)/Hp(y 11 ;~,u,/):::; A,
Vy',y 11 E JRn+I,
V1:::; /oi
(14)
(III) Vy', y 11 E JRn+l and Vy E JRn+l we have lp(.B)I(y';~,T):::; c:,a(ImT)IP(y 11 ;~,T)I,
{3
IP(a)(Yi ~' T )I :::; ca(Im T )IP(y; ~' T )1(1
+ lei),
> 0,
(15) a
> 0,
(16)
where c ,a(Im T ), ca(Im T) ----+ 0 as Im T ----+ -oo. Then the differential operator P(y; D) satisfies a priori estimates (3) and (3'), and, consequently, homogeneous Cauchy's problem is uniquely solvable. The theorem will be proved in §3. In the case of constant coefficients conditions (I), (II), and (III) go into a single condition, namely the operator P(~, r) should be exponentially correct. Conditions (15) and (16) are fulfilled automatically for exponentially correct symbols of constant strength. Later (see §3) we shall show that the condition of constant strength for P implies an analogous condition for H p, i.e. Theorems A and B imply the correctness theorem for Cauchy's problem for exponentially correct operators of constant strength. In §§3 and 4 we shall present meaningful examples of (pluriparabolic and dominantly correct) differential operators with variable coefficients for which the condition of constant strength does not hold but all conditions of Theorem B are fulfilled. 1.4. The proof of Theorem A. 1) The uniqueness of the solution to problem (2) is the simpler assertion in the theorem. This property and the stronger assertion
(17) follow from the inequality
In view of the continuity, this inequality is extended to the space s E IR and N ~ deg P:
HGtN) for any (18)
Chapter 7
220
Further, let u E H[\joo) and let Pu = 0. The definition of H[~loo) implies that u E H[~{) for some s 1 . Therefore, if a sequence
Uj
E H[~J)
converges to u in Hr~{),
then the sequence Puj converges to Pu = 0 in Hr~t), where Applying (18) we conclude that u = 0, i.e. (17) holds. 2) In view of the duality relation
s2
~
s1 -
deg P.
( H(s))'- H(-s)
hl
-
(--y]'
it follows from the inequality (18') that for any given right-hand side f E Hr~f there exists a solution u E H[~f to Equation (2). Indeed ( cf. Hormander [3, §8. 7]), consider the linear functional L(,P) = (f,r.p) on the linear manifold {,P,'Ij; = P*r.p,r.p E Hr~~}. By virtue of (18'), we have IL( 'ljJ) I ~ IIJII(s),-y II 'PI!( -s) ,--y ~ Cs IIJII (s),-y liP* 'P II (-s},c---ySince P*r.p = '1/J, the norm of the functional does not exceed C 8 IIJII(s),T Therefore, by the Hahn-Banach theorem, there exists an element u E H[~f, llull(s),-y ~ Cs llfll<s)m such that (u,,P)=L(,P), thatis (u,P*r.p)=(f,r.p). Thus, the proof of the theorem has reduced to the proof of the fact that u belongs to H[~f+ for f E Hr~f+. It is this property for whose proof the stronger estimate (3') (as compared to (18')) is applied. For this proof we need some estimates in the more general spaces H[~!,-r"] l) whose special cases are the spaces H[~f and H[~f+ and their conjugate spaces. 3) We define the norm in H[~f by means of the PDO with symbol (19) where /O is selected so that symbol (19) does not vanish for the values of Im T in question. So, we set (20) Let Hf~!,-r"] with 1' ~ 1" denote the set of those u belonging 1" for which the norm
llull(s)d d'
=
sup -y' ~ 'Y ~ -y"
llull(s),-y
Hr~f with 1' ~ 1 ~ (21)
l)For a detailed presentation of the theory of these spaces see Volevich and Gindikin [1, 7].
221
The Method of Energy Estimates in Cauchy's Problem
is finite. If 1' and 1" are finite numbers, then H[(s} "] coincides with the intersection "{,"{
H[~}] n H[~}, 1 and the norm (21) is equivalent to the natural norm in the intersection of spaces:
(21') In case 1' = -oo, we obtain the subspace H[(s) 'Yl ,"{2 1. 4) We now show that the proof of the existence of a solution u E H[~f+ reduces to the proof of the existence of a solution belonging to H[(s} l for arbitrary {1 < {2, 'Yl '"12 where -12 is sufficiently large. Then f E H[~]) for all p < {· If inequalities (3) and (3') Indeed, let f E are fulfilled, then estimates (18) and (18') are sure to hold, and consequently for every p:::;; 1 there exists a unique solution Up E H[~l to Equation (2), and we have
HGf+·
(22) where the constant c 8 does not depend on p. If we prove for at least sufficiently large p that the function Up does not in fact depend on p, i.e. up= u, p < p 0 , then, taking the supremum of the left-hand side of (22) over all p :::;; p 0 , we obtain (for Po < 1) the inequality It follows (see Volevich and Gindikin [1, §2.5]) that u = 0 for t < 0. Let {1 < 12 :::;; po and let -po be sufficiently large. Then, by the hypothesis,
for any right-hand side H[(s) 'Yl ,"{2 l to Equation u'Yl = u'Yl "12 = u'Y2 •
f
E
H[~;,'Y2 ]
C
H[~f+ there exists a unique solution
u'Y1 "12 E
(2). However, the uniqueness in the spaces H[(sl) implies that p
5) We now deduce the existence of a solution in H[(s) l with 'Yl ,"{2
{I
< 1 2 < p0 from
8 ) an a priori estimate in the conjugate spaces ( H[('Yl l )'. We state the necessary ,"{2 definitions. We set
H( -s)
-
(-'Yl,-"12]-
(H(s)
hl,'Y2]
)'
(23)
and endow the left-hand space with the natural norm of the Banach conjugate space of H[~!,'Y2 ]. It is proved that this space coincides with the linear hull of
(-s) H (-'Yd
( -s) + H[_'Y 2]' and as the norm in the space (23)
the expression
(24) can be taken, where x(t) E C 00 (R 1 ), x(t) = 1 fort;::: 0, x(t) = 0 fort:::;; -1. The central point of the proof of Theorem A is the following
222
Chapter 7
Lemma. Let 12 > {l, let 12 - {l ~ 5, and let tbe conditions of tbe theorem bold. Then 'VM > 0 and \18 > 0 there is lo(M, 5) such that for lsi ~ M and { l < 12 < 1o(M,5) tbe inequalities llull(s),"Y2,"Yl ~ Ksi1Pull(s),"Y2 "Yl'
(25)
1
II vii( -s),-"Yl ,-"Y2
~
K; II Pull< -s),-"Yl ,-"Y2
(25')
bold. In view of the duality, inequality (25') implies the existence of a solution belonging to H[(s) "Yl, "Y2] . Therefore the assertion of the theorem follows from what has been said 1n 4). 6) The proof of the lemma. To simplify the notation, we confine ourselves to the proof of (25) (inequality (25') is proved in a similar way). By definition, for 12 > 1 1 we have By Leibniz's formula, m
xPu = P(xu)-
L Xlp(l)u,
Xl =
D!x/a!
l=l
On writing down an analogous relation for (1- x)Pu we obtain
m
1=1 m
~I: [(,o- ll) 1IIP(l)(xu)ll<s)m + (l'o -1'2)'11p(l)(l- x)ull<s),"'f2 1=1
(26) We have
Using ,the fact that Xt(t), l ~ 1, is a function of compact, suppo~t we show that IIXlp(l)(l- x)ull(s),"Yl
Comparing (27) and (28) we find
~ c(s,/'2- ldiiP(l)(l- x )ull(s),"Y2'
(28)
223
The Method of Energy Estimates in Cauchy's Problem
It is shown in a similar way that llxzp(l)ull(s),"Y2 is also estimated by means of the right-hand side of (29). Substituting these inequalities into (27) and taking a sufficiently large -"(2 < -"(I we estimate the right-hand side of (26) from below by means of m
~I: [('Yo- 'YI) 1IIP(l)(xu)ll<s) ,"Yl
+('Yo- 'Y2) 1IIP(l)(l- x)ull(s) ,"Y2]
l=I
~
ml m! -ic 'Yo- 'Y2)m [llxull<s),"Yl + 11c1- x)ull<s),"Y2J = 2 c 'Yo- 'Y2)mllull<s),"Y2,"Yl,
i.e. we arrive at inequality (25).
7) Thus, to complete the proof of the theorem we have to establish (28). We write
llxtp(l)(l - x)ull(s),"Yl
def
II exp( 'YI t)As(Dx, Dt)Xlp(l) (1 - x)ull
= ll.\s(Dx, Dt + i"(I) exp( "(It)xzP(l)(1- x)ull
As(Dx, Dt
+ i'YI)
= II As(Dx, Dt +
( . )[ ( ) ) i'Y20 As Dx, Dt + Z"f2 exp 'YI t- 'Y2t XI
(30)
x exp( "(2t)P(l)(l- x)ull· By virtue of the elementary inequality l.\s(e,a + i'YI).\;I(e,a + i'Y2)I :s;; (1 + b2- 'YIIY,
the expression A8 (Dx, Dt + i"(I)A_ 8 (Dx, Dt + i'Y2) is a bounded operator in L2, and therefore the right-hand side of (30) is estimated from above by means of c('Y2- 'YI)II.\s(Dx,Dt + i"(2)[exp('Y2t- 'Y!t)xz]exp("f2t)P(l)(l- x)ull·
(31)
The expression in square brackets is a function of compact support, and its derivatives are estimated by means of constants depending on the difference "(2 - "(1 solely. It can be shown that (31) is estimated by means of
c' ('Y2- 'YI )liAs( Dx, Dt + iJ2) exp( 'Y2t)P(l) (1- x)ull
def
c' ({2 -{I )llp(l) (1- x)ull (s),"Y2
(this inequality is proved particularly simply in the case of integral values of s
~
0 ).
§2. Sufficient conditions for the existence of energy estimates In this section we present a set of rather cumbersome conditions making it possible to estimate from above and below the forms
- Im[Q(y; D)u, Q( 1 )(y; D)u](s) ,"Y'
Q = P, P*,
(1)
by means of analogous for.m s corresponding to an operator Q with constant coefficients (frozen at a point y = y 0 ). From the estimate for forms ( 1) we derive inequalities (1.3) and (1.3') and thus establish the solvability of Cauchy's problem. As consequences of the conditions in the present section, we shall obtain in §3 some easily verifiable conditions guaranteeing the solvability of Cauchy's problem. The results in this section are taken from the paper by Volevich [1].
Chapter 7
224
2.1. Formulation of the main results. We shall deal with differential operators P(y; D), y = (t, x) E JRn+I, solved with respect to the highest derivative with respect tot, i.e. the symbol P(y; ~' 7) has the form
P(y;~,7)
= 7m + LP;(Y;07m-j.
(2)
j>O
As in Chapters 2 and 3, we shall assume, without a special stipulation, that the coefficients of the polynomial symbol (2) belong to c= and do not depend on y for large IYI· It will also be assumed that conditions (I) and (II) in the foregoing section are fulfilled. When estimating the forms ( 1) we shall use the norm
{u}(s),-y=
(jj Hp(yo;~,<7,!)(1+1~12+0"2+!2)slu(CO"+i!)l2d~dO")I/2'
(3)
where y 0 is a fixed point. By the condition of constant strength for symbol (2), the replacement of y0 by any other point results in an equivalent norm. If we set, as in §1,
_x;= := (±iDt + /o + V1 + !Dxl 2 ) 8 , ± [u, v ](s),-y = [exp( 1t)-\±(D)u, exp( 1t)-\;=(D)v],
(4) (5)
then, as was noted in §1, the norm (3) is equivalent to - Im(P(y0; D)u, p(I)(y 0; D)u](s),-y 1
I~ /o·
(3')
We introduce the following convenient notation. If Q(y; ~' 7) and R(y; ~' 7) are two polynomial functions in 7, we set
. _ 1 [8R . . . 8Q(y; ~' {Q,R}(y,CO",/)- 2i 87 (y,~,7)Q(y,~,7) -R(y,~ , 7) 87
7)] '
7
=
0" + i,.
This definition implies that
{Q, R} = {R,Q}. (6) Proposition 1. Let symbol (2) satisfy conditions (I) and (II) in §1 and, moreover, let there be /o such that Vy E !Rn and V1 < /o we have
IH}!\y;~,0",/)1 < c:p(!)Hp(y;~,O",/), f3 > 0, I{P,p(f3)}(p)(Y;~,O",/)I < cp(!)Hp(y;~,O",/), f3 > 0, I{P(a),p(f3)}(p)(Y;~,0" 1 /)I < Eap(!)Hp(y;~, 0",/)(1 + l~l)lal, l/31 ~ o, 'lal > 0,
(7) (8)
(9)
where cp(/), cap(!)~ 0 as 1 ~ -oo. Then VM > 0 3/o(M) such that Vs E R, lsi~ M, and 1 ~ !o(M) the two-sided estimate
c:;- 1{ u Hs),-y holds.
~ - Im +[P(y; D)u, p(l)(y; D)u](s),-y ~ c8 { u Hs) ,-y
Vu E
H[\J)
(10)
225
The Method of Energy Estimates in Cauchy's Problem
Proposition 2. Let conditions (I) and (II) in §1 be fulfilled, let condition (7) bold, and, besides, let
I{P,Pca)}(P)(y;C0",/)1 < cp(!)Hp(y;(,O",/), I{P,P(a+f3)}(f3)(y;~,0" 1 /)I
f3 > o,
(11)
< c 0 p(!)Hp(y;~,0", /) (1 + l ~l)lal, f3 ~ 0, a > 0.
Tben VM > 0 3/~(M) such that \Is E llt, estimate
lsi ~
M, and 1 ~ !~(M) the two-sided
c:-l {v }(-s),--y ~ Im -[P*(y; D)v, p*(l)(y; D)v]( -s),--y ~ c:{v }( -s),--y Vv E
(12)
1
H(oo)
[--y]
(13)
bolds. Remark. Formally, (9) and (12) are infinite sets of conditions. However, if
lal >
x + deg H p + 1, where xis the constant in Corollary 1.2, then inequalities (9) and (12) are fulfilled automatically.
2.2. Theorem. Let symbol (2) satisfy all conditions of Propositions 1 and 2 in the foregoing section. Then inequalities (1.3) and (1.3') take place. Proof. If conditions (I) and (II) hold, then, by virtue of Proposition 1.2 (II), Vy' E JRn+I we can write the inequality m
c: L)
/O -
!) 21 - 1 IIP(l)(y' i D)ullts),-y ~ {U }(s),-y 1
(14)
1=1
where the constant /o can be selected so that inequalities (14) are fulfilled for any y' E JRn+I and 'Y ~ lo· These inequalities readily imply an analogous inequality for the operator with variable coefficients: m
c~
L)/o -
!) 21 -lllp(l)(y; D)ull(s),-y ~ { u }(s),-y·
(15)
l=l
Indeed, since t4e degrees of all polynomials P(y ; ~' T) are uniformly bounded with respect to y E Jltn+I, they form a finite-dimensional space, and a~ong them there are a finite number of linearly independent elements. Therefore we can write J
P(y;e.,T) = "Lcj(y)P(yi;e,T), j=l
(16)
Chapter 7
226
where the functions Cj(Y) possess the same smoothness properties as the coefficients of the original polynomial (2). Differentiating (16) with respect to T we obtain J
p(l>(y; e, T) =
2: Cj(y)P<1>(yi; e, T).
(16')
j=1
Applying inequality (14) with y' = yi to each of the operators on the right-hand side of (16') we obtain (15). Comparing (15) and (10) we find ( cf. Section 1.3) m
c~ I:Cio- !)21 - 1 IIP( 1)ull(s),-y ~- Im +[!u, p( 1 )u)(s),-y ~ IIPullcs),-yiiP(l)ull(s) ,-y 1=1
~ ( lo -
m
!)- 112 11Pullcs),-y (
L(lo -
1/2
!)21 - 1 IIP( 1)ull(s),-y)
,
1=1
whence follows inequality (1.3). Similarly, to prove (1.3') it suffices to show that m
c~ * I:Cio- 1?1- 1 IIP*(l)v11(-s),--y ~ {v H-s),- -y·
(15')
l-1 According to (16), we have
1-"'
1
. -"'-(,B) . -(,B) i. P * (y,e,T)LtP(p)(y,e,T)/(3.Lt (3!D ,B c1.(y)P (y ,e,r).
Hence, to prove (15') it suffices to establish the inequalities m
const
L(!o -
1)21 -
L
~
{ v }(-s),--y,
(y';e,<J +i!) l ~ Hp(y';e,<J,!),
I::::; lo·
1
IIP(l)(,B) (yi; D)vll(-s),--y
,8~0
l=l
which are equivalent to the set of inequalities 21
1
,a·-( l)
const(!o- 1) - 18 P We put 17
= (e,
(J ).
(17)
For any polynomial Q( 17) we have the inequality c1Q(,B)(7J)I ~ sup IQ(1J + B)l,
(18)
181~1
where the constant c depends only on the degree of Q and the dimension of the space. In view of inequality (18) (applied to the polynomial Q(17) = pU>(y'; (J + i1)), we have
e,
c1(1o -!) 21 - 1IP( 1)(,B)(y';e,<J+if)l 2
::::;
sup Hp(y';1J+B,,). IBI~l
227
The Method of Energy Estimates in Cauchy's Problem
We now show that if -1 is sufficiently large, then
Indeed, exp anding the left-hand side by Taylor's formula we obtain
It now remains to apply condition (7). 2.3. The plan of the proof of the propositions in Section 2.1. We set w = exp( lt).A't(D)u. If u runs over H[\]J, then the function w runs over H~=). Setting D 1 = (Dx, Dt + i1) we can rewrite the middle term in (10) in the form
- Im[.A~(D 1 )P(y; D-r ).A~s(D, )w, .A~(D-r )P(l) (y; D, ).A~s(D, )w] =
(~.A: 8 (D- 1 ){ p(I)*(y; D_ 1 ).A~(D,).A;(D- 1 )P(y; D 1 )
(19)
- P*(y; D_-y).A~(D-y).A;(D_ 1 )P< 1 )(y; D 1 )} .A~s(D,)w, w). Here we used the fact that
If the coefficients of P were constant ( cf. Section 1.3), we would obtain the quadratic form (Hp(D,1)w,w). In the case of variable coefficients we separate out the Hermitian form corresponding to the differential operator H p(y; D, 1), i.e. rewrite ( 19) in the form Re(Hp(y;D,1)w,w) + (Q 81 w,w), (20)
where
Qs 1 = ~.A:s(D--r){ p(I)*(y; D_,)Xt(D, )X;(D- 1 )P(y; D 1 ) - P*(y; D_ 1 ).A~(D-y).A;(D--r)P< 1 )(y; D 1 ) }.A~ 8 (D 1 ) -
~Hp(y;D,1)- ~Hf,(y;D,1).
(21)
We shall prove the following inequalities:
c-; 1 (Hp(y 0 ;D,1)w,w ) ~ Re(Hp(y; D,1)w,w) ~ c1 (Hp(y 0 ,D)w,w) I(Qs 1 w,w)l ~ c(I)(Hp(y 0 ;D,I)w,w),
c(l)----+ 0,
I-+ -oo.
(22) (23)
Chapter 7
228
Noting that
we obtain the proof of Proposition 1 in Section 2.1. We note that (22) is an analog of Garding's inequality for inhomogeneous quadratic forms. As to Proposition 2 in Section 2.1, after the substitution of
z = exp( -!t)>..;(D)v the middle term in (13) can be rewritten as
Re(Hp(y;D,1)z,z) + (Rs'Yz,z),
(24)
where
Rs"( =
;i)...~s(D'Y){ p(l)(y; D'Y)>..~s(D'Y)>..;(D_'Y)P*(y; D_'Y) - P(y; D'Y )>..~s(D'Y )>..=s(D-"( )P( 1)* ( y; D_'Y)} >..; (D_'Y) -
~Hp(y; D, !) - ~Hp(y; D, 1).
(25)
Proposition 2 in Section 2.1 follows from (22) and the inequality
2.4. The proof of Inequality (23}. If Q1(y; D) and Q 2 (y; D) are two PDO's then for any natural N we set
This relation is usually called the commutation formula. Setting
we write
(28)
The Method of Energy Estimates in Cauchy's Problem
229
The expression under the summation sign in (28) is a PDO. To calculate its symbol we note that if Q 1 and Q 2 are two differential operators, then, in view of Leibnitz's formula, the symbol of Qi Q2 is equal to
Therefore the symbol of the PDO under the summation sign in (28) is equal to
App1ying the commutation formula once again we write operator (21) in the form
Q S"f
= Q s"{N + Ts"{N,
(29)
where Q s'YN is a PDO with symbol """""
1
~ od ,8! 8!
{P.
(a)'
p(f3)}
(f3+0)
~(a),\-(0),\+ (. 2s -s -s- Hp y, 1], I
)
-
a,{3,0
1""""" ({3) ( . 2 ~ H P(f3) y, 1], I
)
.
{3>0
(30) Noting that {P, P} = Hp we rewrite the symbol in the form
1 {P. ({3)} (a),\-(0)+ 1"' ({3) a! ,8! 8! (a)l p (f3+8)~2s -s ,\_s- 2 ~ H P(f3)•
""""" ~ la+f3+8I>O
(30')
{3>0
The operator Ts'YN is written
~,\=sCp(l) RN(~2s, P)- P* RN(~2s, p(l)Y~s)
+
1 R (,\- {P. p(f3)} )~(a),\-(0) + a! ,8! N -Sl (a)' (f3+0) 2s -s ,\_s•
"""""
~
(31)
!a+f3+0I>O
Lemma 1. The symbol of the operator Q s'YN is represented a; Qs'YN(Y;1J) = Lci(y)bj(1J,I), j=l
where
(32)
Chapter 7
230
Proof. We now show that, by virtue of Proposition 1 in Section 1.2, we have
1Qs 1 N(Y;TJ)I < e(!)Hp(y 0 ;TJ,/),
e(!)--+ 0,
1--+ -oo.
(34)
Writing the symbol P(y; ~' r) in the form of (16) we arrive at representation (32). The inequalities
IH~~)(y; 7], !)I < ep( !)Hp(y 0 ; TJ, !) follow from (7) and the condition of constant strength. We have to estimate the first sum in (30'). As can easily be seen, for 1 < /o we have
~~~~\TJ,/).A::::~8 )(TJ, !)X~s(TJ,!)I ~ I
+ ~~l)-la+BI+1
~ I<~e(l
+ 1~1)-la+BI.
With account of (8) and (9), we arrive at (34). To estimate the operator Qs 1 N we need Lemma 2. Let J-L(TJ) be a positive function and let
J-L(TJ')tL-1(ry") ~ I<(l + ITJ'- ry"l)t . Let a(y) =a+ a'(y), let a'(y) E V, and let
Ib( TJ) I ~ 8tL 2 ( TJ) . Then I( a(y )b(D)v, v)l ~ 8I<( a)IIJ-L(D)vll 2 • Proof. By Schwarz' inequality, we have
I( a(y )b(D)v, v) I ~ IIJ-L(D)vlllltL- 1(D)a(y )b(D)vll· Using the inequality (see Volevich and Paneyakh [1, (1.10)])
IIJ-L- 1(D)a(y)wll
~ K (Ia I+
j la(ry)l(l + ITJI) dry) IIJ-L- (D)wll 1
1
we prove the assertion of the lemma. To apply Lemma 2 to estimate the operator Qs 1 N we put
h(ry) = Htj\y 0 ; TJ,/). According to condition (7), we have
h(ry') = [1 +"" (ry'- ry")/3 Hj!)(yo; ry",/)J I/2 ~ t(l +I "- 'l)l h( "7 ") L.t (3' H ( o. " ) " cons TJ TJ ' f3>0 • P Y , 1J 'I where 21?:: degHp. Applying Lemma 2 to the forms (cj(y)bj(D,y)w,w) we prove the inequality
(23') We now proceed to the estimation of the form corresponding to the operator
Ts 1 N in (29).
231
The Method of Energy Estimates in Cauchy's Problem
Lemma 3. The operator Ts-yN (see (3.1)) is represented in the form Ts1N
where
Pjk
,,
= ~Pjk/
ink
t,
j+k
~2m-2,
(35)
are operators of the (2p - N)th order with respect to the variables x ,
1.e.
1,81
~
2N- 2p.
(35')
Here pis the maximum degree of the operators Pj in (2), and the constant in (35') does not depend on 1. Proof. By the linearity, we have
RN(~2s' P) =
L RN(b,.2s, aaj(Y))D~(Dt + i1)m-j j>O
(we have used the fact that the coefficient in the operator Df is identically equal to 1). The expression RN(~ 28 , aaj) is an operator of the (2s- N)th order with respect to x. It follows that the order of the operator >..=sp(l)* RN( ~2s, aaj )X2=s with respect to x is equal to 2p- N. The remaining terms in (31) are considered in like manner. V\te now proceed to the estimation of the quadratic form
corresponding to operator (35). Applying integration by parts with respect tot we can rewrite the form thus: J•/
+ k' ./: : : : m- 1, J., + k" ./: : : . m- 1.
The absolute value of the latter form does not exceed x=
N
2
-p.
If N is sufficiently large, then by virtue of Corollary 1.2, this expression can be estimated from above by means of
We have thus proved that (23") Comparing (23') and (23") we obtain (23).
Chapter 7
232
2.5. The proof of Inequality {26). The proof of (26) is carried out according to the same plan as the proof of (23). If Q1 and Q2 are two differential operators, then the symbol of Q 1 Qi is equal to
Using the commutation formula we can represent operator (25) as a sum a PDO with symbol
and operators representable in the form of (35). Applying the conditions of Proposition 2 in Section 2.1 and Lemma 2 we prove (26).
2.6. Garding's inequality for inhomogeneous quadratic forms (the proof of inequality (22) ). We shall prove the following Proposition. Let H(y; ry) be a positive polynomial symbol in TJ having smooth stabilized coefficients 1 ) and satisfying the following conditions:
(i)
H(y' j Tj )H- 1 (y" j Tj)
(ii)
IH(fi)(y; TJ)I
< Co Vy', y"
E JRn+l,
< c:H(y; TJ) \lyE JRn+l'
Vry E JRn+l,
Vry E JRn+l.
Assume that the constant c in (ii) is sufficiently small. Then the two-sided estimate c- 1 (H(D)w, w)
< Re(H(y; D)w, w) < c(H(D)w, w)
(36)
holds, where H(D) = H(y 0 ; D), y 0 E JRn+ 1. The proof is carried out according to the same scheme as the ordinary Garding inequality. 1) We first consider inequality (36) on the functions w with support in a ball of a sufficiently small radius 8 and center at y0 . Write the operator H(y; D) in the form J
H(y; D)
= H(y 0 ; D)+
L hi(Y )H(yi; D). j=l
:
We take a truncating function ,P(y) E D equal to 1.for IY- y 0 I ;::: 28. Then we have
H(y; D)w
IY - y0 I ~ 8 and to zero for
= H(D)w + L('l/Jhj)(y)H(yi; D)w.
l)This condition can be ch·opped (see Volevich [1, Section 3.4].
The Method of Energy Estimates in Cauchy's Problem
233
We now write J
IRe(H(y; D)w, w)- (H(D)w, w)i:;:;;;
L 1('1/JhiH(yi; D)w, w)l j=l
J
:;:;;; IIH
1 12
(D)wll
L IIH- 1 (D)'l/JhjH(yi; D)wll 1 2
j=l J
:;:;;; IIH 112 (D)wll
I: (11'1/JhiH- 1 (D)H(yi; D)wll
(37)
1 2
j=l
Since hj(y 0 ) therefore
= 0,
the maximum of the function ('1/Jhj)(y) does not exceed c8, and
J
L ll'l/JhjH- 1 (D)H(yi; D)wll:;:;;; c8c~ 12 IIH 1 1 2 (D)wll = Ct8IIH 1 wll. 1 2
1 2
j=l
The Fourier transform of the operator (H- 1 12 (D)'lj;hi- 'l/JhjH- 112 (D) )H(yi; D) is an integral operator with kernel (38) Condition (ii) implies that
Since the function ;fhj(1J) decreases faster than any power of function ( 38) does not exceed
I7JI,
the modulus of
cc(8)(1 + 177' -1]"1)-n-2 Hlf2(1J"). Therefore inequality (37) assumes the form
IRe(H(y; D)w, w)- (H(D)w, w)l < (c18 + c2(8)c:)(H(D)w, w). Taking 8 satisfying the condition c 1 8 < 1/4 and c satisfying the inequality c 1 (8)c < 1/4 we conclude that
1
3
2(H(D)w, w) ~ Re(H(y ; D)w, w) ~ 2,(H(D)w , w).
Chapter 7
234
2) Localization. Take a system of nonnegative functions {'Pi(Y)} possessing the following properties: (a)
=
(d) max !Da
J
!Da
< ca(8)
Va,j.
Then we have Re(H(y; D)w, w) = L
Re(
J
=L
Re(H(y; D)
L(DfJ
By what has been proved, we have
~ L(H(D)(
: : ; 2 L(H(D)(
(40)
To estimate the second term on the right-hand side of ( 39) we take the functions 'lj;i(Y) E V satisfying conditions (a), (b), and (c) and such that
=
L L ('PifJH(fJ)(y; D)('lj;jW ), 'lj;jW ), fJ>O j
Using Lemma 2 in the foregoing section we estimate this expression from above by means of
Let us show that
(41) To this end we note that 'lj;jW =
I: 'lj;j<pr w = I: 'lj;j
kEUj
where Uj is a finite set with the number of elements J 1 not depending on j. Therefore ( cf. Lemma 2 in Section 2.4) we have IIH 112 '1j;iwll 2
::::; J1
L !IH 112 ( 'lj;j
::::; J1 c2
L kEUj
IIH 11 2
( 42)
235
The Method of Energy Estimates in Cauchy's Problem
Performing the summation of inequalities ( 42) over j we obtain ( 41 ). Comparing (39) with ( 40) and ( 41) we conclude that if£ is sufficiently small, then the left-hand side of ( 39) is estimated from above and below by means of
~(H(D)(rpjw), (rpjw)). J
Further, repeating in fact the already performed calculations we find
:!
I~(H(D)(rpjw),cpjw)- (H(D)w,w)\ ~ L I(D,BtpjH(,B)w,cpjw)l ~ ~ IIH 1 (1/Yjw)ll ~ L IIH 1 (cpjw)ll· c3c
1 2
C4c
1 2
If £ is sufficiently small, then
1 3 -(H(D)w, w) ~ ~ IIH 1 12 (D)rpiwll 2 ~ -(H(D)w, w) 2 ~ 2 which proves the proposition.
§3. An analysis of conditions for the existence of energy estimates It was shown in §2 that the conditions of Propositions 1 and 2 in Section 2.1 guarantee the existence of estimates (1.3) and (1.3') under which Cauchy's problem is uniquely solvable. However, as was mentioned above, it is difficult to verify the fulfilment of these conditions for given classes of differential operators. In the present section we shall present cruder sufficient conditions for the existence of energy estimates and, in particular, prove Theorem B stated in §1. Examples of differential operators satisfying the conditions of this theorem will also be given. A more complicated example of dominantly correct operators will be considered in §4. The results in this section are taken from the papers by Volevich [1] and Gindikin [1] (see the Appendix in the latter paper). 3.1. Some immediate consequences of Theorem 2.1. As in §1, we shall consider a symbol P(y; ~' T) with smooth stabilized coefficients solved with respect to the highest power Tm, the coefficient in Tm being identically equal to 1. In what follows these conditions on the symbol will not be stipulated. Proposition 1. Let a symbol P(y; C T) satisfy the correctness conditions Vy E Rn+t.and let for the function Hp(y;~,a,1) the condition of constant strength be fulfilled. Let, additionally, the conditions below hold:
I{P(,B),P(o)}(y;e,a,,)l < Ea,B(r)Hp(e,a,,),
f3
> 0, a~ 0,
I{P,P(<:{}(y;~,a,,)l < Ea,B(r)Hp(~,a,[), f3 > 0, a~ 0, I{P,P(o)}(y;~,a,,)l < ca(r)Hp(e,a,,)(1 +lei), a> 0,
(1) (2) (3)
Chapter 7
236
where Eaf3(1), £ 01 (1) ~ 0 as 1 ~ -oo. Then the symbol P(y;~,r) satisfies all conditions of Propositions 1 and 2 in Section 1.2. Remark. In the case of constant coefficients all conditions of the proposition reduce to the condition
(1') This condition is equivalent to the exponential correctness of the polynomial P. The proof of Proposition 1. 1) We first verify the conditions
f3 > 0. For l/31
= 1 condition ( 4)
(4)
follows from (1) with a= 0 since in the case we have
We now show that condition (4) for 1/31 > 1 follows from the analogous condition for 1/31 = 1. We use the simple argument in the paper by Shilov [1]. By Lagrange's formula, we have
Ilog Hp(ry+B,I)I H ( ) = llogHp(TJ + 8,1) -logHp(TJ,I)I TJ,I p
= H-p 1 (TJ
+ 0*,1)1 L
where () E Rn+l, IBI ~ 1, and follows that
()*
()kfhH(ry
+ 0*,1)1 ~ c(l) ~ oo,
1
~
-oo,
is a point on the line segment joining 0 and B. It
where £1 ( 1) ~ 0, 1 ~ -oo. Since the monomials ()f3 are linerally independent as functions of 81, ... , Bn+I, the above inequality implies that (4) holds for any values of l/31. 2) Let us verify conditions (2.8). Since the space of polynomials is finitedimensional, we write
p(t)(f3>(y, TJ
=
+ i1)P(y; TJ + i1)- p
L dj(Y) [p(l)(f3)(yi; TJ + ii)P(yi; TJ + il) - p
+ h)P(l)(yi; TJ + il)]'
237
The Method of Energy Estimates in Cauchy's Problem
that is
(5)
n:
Applying the operator to both sides and using inequalities (1) for a = 0 we obtain (2.8). 3) The fulfilment of conditions (2.9) is verified in like manner with replacement of Pin (5) by P(a)· 4) We verify (2.11) and (2.12). Conditions (2.12) for (3 = 0 go into (3), and therefore they should be verified for (3 > 0. In this case (2.11) and (2.12) are special cases of the more general condition
(3 > 0.
(6)
The proof of (6) is analogous to the above verification of (4). For left-hand side of ( 6) is equal to
1!31
1 the
and the required estimate is a consequence of (1) and (2). If 1!31 > 1, then the vector (3 is representable as a sum of integral vectors: (3 = (3' + (3", if3' I = 1. Applying inequality (2.18) with (3 = (3" to the symbol Q = {P, P(a)}(.B') and using the fact that, by virtue of the already proved inequalities (4), we have
Hp('fJ
+ B,,)H-p 1 (ry,/)-+ 0
for 1-+ oo (uniformly with respect tory),
we arrive at (6). A direct consequence of Proposition 1 is
e,
Proposition 2. Let a symbol P(y; ry) satisfy Petrovski1's correctness condition Vy E JRn+l, the condition of constant strength for Hp, and condition (3), and, moreover, let for any pair of points y', y" E JRn+l the inequality
(3
> 0,
(7)
bold, where c:,a(l) -+ 0 for 1 -+ -oo. Then all conditions of Proposition 1 and, consequently, of Theorem 2.1 are fulfilled. Proof. Using the representation
we write We now apply the operator D~, and set y' = y" = y to obtain, by virtue of (7), relation (1 ). Applying the operator D~, and putting y = y' = y" we derive (2).
238
Chapter 7
3.2. The proof of Theorem B in Section 1.3. We shall need some auxiliary assertions. Let Q(17, 1) and R(17, 1) be some functions of the variables 1 E ( -oo, lo) and 17, where 17 runs over the same set for the two functions, say (for definiteness) over JRn+l. Lemma 1. Let
Then the following conditions are equivalent: (i) R(1J,I)Q- 1(1J,I)--+ 0 for 1--+ -oo uniformly with respect to 17; (ii) \Ia E C there is lo(a) such that
Q(17,1)
+ aR(17,1) =J. 0,
1 < lo(a),
17 E JRn+l,
where the function lo( a) can be chosen so that it is bounded from below on any compact set in C. Proof. (i)==?(ii) is obvious. (ii)==?(i). Assume that (i) does not hold. sequence (1Jj,lj), li--+ -oo, such that
Then for some c
> 0 there is a
IR(1Jj,lj)Q-1(1Jj,lj)l ~c. We set aj = R(1Jj,''lj)/Q(1Jj,lj)· Then !ail < c-I, and, by virtue of (ii), the sequence lo( aj) is bounded from below by a constant lo. Since lj --+ -oo, we have 1 i < 1o for sufficiently large j, and we hence
lj < IO· The resulting contradiction proves the lemma. Lemma 2. Let polynomials Pj(~, T ), j = 1, 2, satisfy Petrovskil's condition, that is ::!10 such that ·
_..,. lo, I rnT::::::::
.,t E
l!l>n, ~
(8)
Then
Proof. If T1k(0 and T2k(0 are the roots of the polynomials P1 and P 2 , then replacing P1 and P2 by their factorizations we derive
The Method of Energy Estimates in Cauchy's Problem
239
If Im7 ~ lo, then, according to (8), we have Pt(e,1)P2(e,1) =I 0. Further, since Im( 7- 7j k( e)) < 0, j = 1, 2, the two expressions in the square brackets have positive imaginary parts, and consequently ( 9) holds. If two functions Q( 1], 1) and R( 1], 1) are related by conditions of Lemma 1, we shall write R -< Q. The same notation will be retained for Q( 1) and R( 1) regarded as functions of the variables 1J = ( Re 7) and 1 = Im 7.
e,
e,
e,
Lemma 3. If P is a polynomial correct in Petrovski'l's sense and R( P(e, 1 ), then {R,P}(e,a,l)-< Hp(e,a,l)·
e, 7)
-<
. (10)
Proof. According to Lemma 1, if R-< P, then V7i E
(P
i.e. the polynomial P have {P
+ aR)(e, r) # 0,
Im 7
+ aR is also correct
+ aR, P} = {P, P} + a{R, P} =
< lo(a),
in Petrovskil''s sense. By Lemma 2, we
Hp
+ a{R, P} =j:; 0,
Im 1 ~ lo(a).
Applying Lemma 1 once again we obtain (10). We now can prove Theorem B. We have in fact to show that condition (1.15) of the theorem implies (7) and that (1.16) implies (3). Indeed, take arbitrary y', y" E Rn+l, f3 > 0. According to (1.15), we have R
def
p(f3)(y'; e, 7)-< P(y"; e, 7)
def
P.
Applying condition (10) of Lemma 3 to the polynomials P and R be obtain (7). We note that in the assertions of Lemmas 2 and 3 the polynomial dependence of the functions involved on T is essential while the polynomial dependence on is inessential. In view of this fact, Lemma 3 can be applied toR= P(a)(Y; 1) and P = P(y;e,1)(1 +lei). Therefore
e,
{P(a)(y), P(y)}(I
e
+leD -< Hp(y)(1 + lel) 2 ,
whence follows (3). Theorem B is proved completely. 3.3. Remarks on the condition of the constant strength for Hp. Condition (1.15) means that the symbol P(y; r) is exponentially correct for every fixed y E Rn+t. If tpe condition of constant strength is imposed on tge symbol P, that is 31o, A > 0 such that \fy', y" E JR.n+t the inequalities
e,
lm1::;; lo, hold, then conditions (1.15) and (1.16) are fulfilled automatically. Moreover, as will be shown, the exponential correctness and the condition of constant strength for P imply the condition of constant strength for H p, i.e. Theorems A and B imply a non-trivial generalization of Theorem 2.5.5.
Chapter 7
240
Proposition. Let P(y; ~, T) be a polynomial correct in Petrovski1's sense at every point and let the condition of constant strength be fulfilled for it. Then the function H p(y; ~, f7, 1) satisfies the condition of constant strength. To prove this assertion we first of all note that the lemma below is readily proved by repeating of the argument in Lemma 1 in the foregoing section. Lemma 1'. Let
Then the conditions below are equivalent: (i) R(ry,/)Q- 1 (TJ,/) < c for1 ~'Yo and some c; (ii) (Q + aR)(TJ,/)-=/:- 0 for lal < c and 1 < /O· If the conditions of Lemma 1' are fulfilled, we shall say that R is weakly subordinate to Q. The following lemma is a modification of Lemma 3 in the foregoing section.
Lemma 2. If P is a polynomial correct in Petrovskil's sense and R is weakly subordinate to P, then {R, R} is weakly subordinate to { P, P}. Applying Lemma 2 to the polynomials R = P(y';~,T) and P = P(y";~,T) we conclude that {P(y'), P(y')} is weakly subordinate to {P(y"), P(y")} for any y' and y", which exactly means that the assertion of the proposition is true. We outline the scheme of the proof of Lemma 2. We shall also need Lemma 3. If P1 and .P2 are polynomials correct in Petrovski1's sense and R is weakly subordinate to P1, then {R, Pz} is weakly subordinate to {P1 , P 2 }.
Proof. If lal is sufficiently small, then P1
+ aR is a polynomial correct in Petro-
vski1's sense, and, by Lemma 2 in the foregoing section, we have
The proof of Lemma 2. If a is sufficiently small, then the polynomial {P+aR, R} is weakly subordinate to {P + aR, P} = { P, P} + a{ R, P}. Since, according to Lemma 3, {R, P} is weakly subordinate to {P, P}, we see that {P, P} +a{ R, R} is weakly subordinate to {P, P}. We have thus proved that for sufficiently small lal
{P, R}
+ a{R, R}
is weakly subordinate to {P, P}.
With account of the fact that {P, R} is weakly subordinate to {P, P} , it follows that the assertion of the lemma holds. The condition of constant strength for H p is the main condition of Theorem B, and its verification is most difficult. However, there are classes of symbols for which
241
The Method of Energy Estimates in Cauchy's Problem
H p is estimated from below by means of the sums of the moduli of the monomials involved, and Newton's polyhedron of H p does for depend on y. In this case the condition of constant strength for H p is fulfilled automatically. Let a symbol P(y; ~' r) be given. We denote by N(P(y)) and 8°(P(y)) Newton's polyhedron of the polynomial P(y; ... ) and the polyhedron of the integrally minor terms of the polynomial, respectively. Regarding {P(y), P(y)} as a polynomial in n+2 variables (~,a,1) we denote by N(HP(y)) the corresponding Newton polyhedron. Finally, let N(P), 8°(P), and N(Hp) be the convex hulls of the unions of N(P(y)), etc. over ally E JRn+l. Theorem. Let tbe following conditions be fulfilled for tbe symbol P(y; ~' r):
(i) N(HP(y)) = N(Hp) \fy E JRn+\ (ii) tbe symbol Hp(y; ~'a, 1) is estimated from below in terms of tbe moduli of tbe monomials involved in it:
Hp(y; ~'a,!) > const (o:,{3,r)EN(Hp)
(iii) Vy E JRn+l and any polynomials Q1 and Q2, N(Ql) E N(P), N(Q2) C 8°(P), we bave
Tben tbe symbol P satisfies all conditions of Proposition 2 in Section 3.1. Proof. It is obvious that (i) and (ii) imply the condition of constant strength for Hp, and hence we have to verify conditions (3) and (7).
Applying condition (iii) to Q 2 (~,r) = p(f3)(y';~,r), f3 > 0, and Q 1 (~,r) =
P(y" ;Cr) we obtain (7). To prove (3) we write Pin the form n
P
= Tm + L
~jPj +Po,
N(Pj) C 8°(P),
j
= 0, ... , n.
j=l
Differentiating this relation with respect to y (it is this place where use is made of the fact that the coefficient in the highest power of r :is identically equal to a constant) we find
I{ P, P(o:)} I =
I_L ~i {P,
Pj(o:)}
+ {P, Po(o:)}
~ ca(!)Hp(y;~,a,!)(l
+
1~1),
I c(!) ~ 0,
'Y ~ -oo.
Chapter 7
242
3.4. Strictly pluriparabolic differential operators. Here we shall present a class of differential operators whose symbols satisfy the conditions of Theorem B. These operators include as special cases the strictly hyperbolic and q-parabolic operators. We first give the definition and description of these operators for the case of constant coefficients, i.e. for polynomials. R~present the space Rn+ 1 as a direct sum of the subspace Rk of the variables o- = ( o- 1, ... , O"k) and the subspace R 1 of the variables ( = ( (1 , . .. , (l ), l + k = n + 1. We separate out the variable O"t, and let o-1 = (o-2, ... , o-k)i in Cauchy's problem o-1 plays the role of a variable dual to time. Let q = 2b be an even positive integer. In what follows we shall assign the weights q and I to the variables o- and (, respectively.
Definition 1. A (q, ... ., q, I, ... , I)-homogeneous polynomial P0 (a, 0 is said to be strictly pluriparabolic (see Gindikin [2), and Volevich and Gindikin [5]) if (i) the polynomial P0 ( o-, 0) is strictly hyperbolic; (ii) there is .X > 0 such that ImToj(o-',0 ~ .XI(Iq,
j = I, ... ,m,
where Toj( o- 1 , 0 are the roots of the polynomial P with respect to o-1.
Definition 2. A polynomial P( o-, 0 is said to be strictly pluriparabolic if its principal (q, ... , q, I, ... , I)-homogeneous part possesses this property. The strict hyperbolicity of P( o-, 0) implies that this polynomial and, conse~ quently, the polynomial P(o-, 0 as well can be solved with respect to the highest power o-i (the coefficient in o-i is assumed to be equal to I):
P(o-, ()=o-r+ Laix.ao-~-ia'"(.B .
(II)
j~1
Proposition. Let q > 0 be even. Then for polynomial (II) the following conditions are equivalent: (I) polynomial (11) is strictly pluriparabolic; (II) there are ro and c > 0 such that for r:::;; ro we have
where the notation ry = ( o-', 0
Hp((,a,r) = -Im(P(o-1 +ir,o-',08P(o-1 + ir,o-',()/8a 1 )
(I3)
is used; (III) there are ro and c1 > 0 such that
(I4)
243
The Method of Energy Estimates in Cauchy's Problem
Proof. (!)===}(II). 1) We first assume that Pis a (q, . .. , q, I, ... , I)-homogeneous polynomial, and let roj(a',(), j =I, ... ,m, be its roots. According to (1.11), for 1 < 0 we have m
2:C -~+1m rok( a',()) II Iat + i1- rok( a', ~)1 2
Hp( (,a, 1) =
k=l
~
j#k
(lfl + .\j(jq)H( (,a, 'Y),
where n
H( (,a, 1) =
2: II [( a1 k=l
Re rok( a', ~)) 2
+ (-~ + Im rok( a', 0) 2 ]
(I5)
i#k
is a ( q, ... , q, I, ... , I)-homogeneous function of degree 2( m - I )q. To prove ( I2) in the quasi-homogeneous case it suffices to show that (I6) Since -1 + lm rok( a',() ~ Ill+ .\l(lq, it suffices to verify (I6) only for 1 = 0, ( = 0 (i.e. for the strictly hyperbolic polynomial P( a, 0) ). Since the roots rok( a', 0) are real and are distinct for ja'l # 0, one of the numbers a1- Rerok(a',O) is nonzero, whence follows (16). In case u' = 0, we have
2) Now let P(a, () = Po(a, () + Q( a,(), where Po is a (q, ... , q, I , .. . , I)-homogeneous polynomial and the (q, .. . , q, 1, ... , I )-degree of Q does not exceed mq - I. By v:hat was proved, for P = P0 inequality (I2) has already been proved. To prove it in the general case we show that
To prove ( 17) we note that H p - H p 0 = {Po, Q} + {Q, P 0 } + {Q, Q} is a polynomial in ~, a, and 1 of ( q, 1, ... , I )-degree no higher than 2mq - q - I, i.e. is a linear combination of monomials of the form of
These monomials can be represented as 'the expressions
which are obviously estimated by means of the right-hand side of (17) with c(1) = const 111-l/q.
Chapter 7
244
(II)=?(III). Since 8Pf8a 1 is a polynomial of (q, ... , q, I, ... , I)-degree no higher than (m- I)q, we have
whence for large -1 follows (14). (III)=?(I). Inequality (14) for the polynomial P implies an analogous inequality with 'Yo = 0 for its (q, ... ,q, I, ... , I)-homogeneous part. As was already done many times, to show this one should replace (a,() by (tqa, t() and pass to the limit for t ~ +oo. In what follows we assume that the polynomial P is (q, I, ... , I)homogeneous. If we set ( = 0 in (14), this results in
whence it follows that P( a, 0) is strictly hyperbolic. It now remains to verify condition (ii) in Definition 1. In view of the quasihomogeneity, it suffices to show that there is >. > 0 such that
P(a1
+ i1,a',() =I- 0
for
I~>.,
1(1 =I,
a E IRk.
(18)
By virtue of (I4), we have to consider only the case I ;;:::: 0. Setting I = 0 in (I4) and assuming that 1(1 = I we find
whence
IP(a1
Taki>.1g >.
+ i1, a', ()I > IP(a, ()1-IP(ai + i1, a',()- P(a, ()I ;;::: CJ (1 +a )m-1 - C2"!((1 + lal)m-1 + 'Ym-1 ].
< cJ/4c 2 and
1 ~
>.
~ I we obtain (I8).
Remark 1. Let P( a,() be a strictly pluriparabolic polynomial and let Toj( a',() be the roots of its principal (q, ... , q, I, ... , I)-homogeneous part. Then, by virtue of condition (i), there is b > 0 such that
!Toj(a',O)- Tok(a',O)I > bla'l,
j =I- k.
(19)
A careful examination of the proof of the proposition shows that the constant c in (12) depends on b (this follows form (19)), >. (by the condition (II)), and the maximum of the moduli of the coefficients of the polynomial P. We now consider a symbol P(y; ~' () with smooth stabilized coefficients, solved with respect to a1 (the highest power of a!), the coefficient in a! being equal to 1.
245
The Method of Energy Estimates in Cauchy's Problem
Definition 3. A symbol P(y; ~' () is said to be strictly pluriparabolic if the polynomial P(y 0 ; a,() is strictly pluriparabolic for each y0 and, moreover, the roots Toj(y'; a',() of the principal ( q, ... , q, 1, ... , 1)-homogeneous part of P satisfy for some ..\, 8 > 0 the inequalities
lroj(y;a',O ) - Tok(y;a',O)I > 8ja'j, Im Toj(y; a',() > ..\j(jq ·
j
=/=-
k,
(20) (21)
Theorem. A symbol P satisfying the conditions of Definition 3 satisfies conditions of Theorem B. Proof. With account of Remark 1, inequality (12) holds for P = P(y; a,() with a unified constant c. It follows that the condition of constant strength holds for Hp. Condition (1.15) is a direct consequence of inequality (14) for P = P(y; a,() (recall that, by virtue of Remark 1, the constant c 1 in (14) does not depend on y ). To prove (3) we note that the symbol P(a), a > 0, does not contain the highest power of a 1 and is represented as k
P(a)(y;a,() = 'LajPaj(y;a,() j=l
l
+ L(jPai(y;a,z) + Pao, i=l
where the ( q, 1, ... , 1 )-degrees of the symbols Paj, Pai, and Pao do not exceed (m- 1)q, mq- 1, and mq- 1, respectively. Relation (3) now follows immediately from (14). Remark 2. Applying the argument used in the proof of the proposition one can easily show that the symbol in Definition 3 satisfies the conditions of Theorem 3.3. Remark 9. In case of pluriparabolic operators the method in §2 can be specified to obtain energy estimates in norms that take into account the quasi-homogeneity of the principal part of the operator, and a rather accurate result on the smoothness of the solution to Cauchy's problem for these equations (see Volevich and Gindikin [5]).
3.5. Remarks on Cauchy's problem in spaces of increasing and decreasing functions. It was noted in Section 2.5. 7 that for exponentially correct symbols of constant strength we have estimates in the spaces H((s)) . Similar estiu ,"'{ mates also take place under the condition ofTheorem B. Moreover, it is possible to generalize the Propositions 1 '.a nd 2 in Section 2.1 to the case of the II II~:)),"Y n<)rrn but we shall not dwell on this question. Theorem. Under the conditions of Theorem B the inequality m Cs"Y
'L:Cro- 1)1llp(l)(y, D)uii~~),"Y ~ IIP(y, D)ull~~),"'f' l=O
1 ~ 1 ( s, a ) ,
(=) u E H "Y+ ,
(22)
Chapter 7
246
bolds. An analogous inequality can also be derived for the adjoint operator P*. A simple reduction of Theorem A makes it possible to prove the solvability of Cauchy's problem in the spaces Hf;~,-y+' Proof. We set u = (1 + IYI 2)-uf 2v. We shall derive two estimates (for sufficiently large -1; for the notation see Section 2.1): m
m
L(lo- 1) llp(l)(y, D)ull~~),-y ~ const L L(lo- 1) llp(l)(fi\y, D)vll, 1
1
l=O
I=O
- Im +[(1
(23)
p~o
+ IYI 2)u/ 2P(y, D)u, (1 + IYI 2t/ 2p(l)(y, D)u]~)
~ c{ v }(s),-y·
(24)
We note that under the conditions of Propositions 1 and 2 in Section 2.1 one can prove a somewhat stronger estimate (as compared to (2.15)) following from (2.17): m
Cs
L L( lo - 1? 1=1
1- 1 llp(l)(fi)(y, D)v11Is),-y
~ { vll(s),-y·
(25)
p~o
Comparing (23) and (25) with (24) we obtain (22). Inequality (23) is a trivial consequence of Leibniz' formula: (1
+ IYI2)u/2 p(l)(y, D)((1 + IYI2)-uf2v) =
L((l
+ IYI2)u/2 Dfi(1 + IYI2)-uf2)/{3!)
p~o
X
p(l)(fi)(y, D)v def
L hupp(l)(fi)(y, D)v.
Similarly, the indicated formula makes it possible to rewrite the left-hand side of (24) as - Im +[Pv
+ }-: hupp(P)v, p(l)v + L
= - Im +[Pv, p(l)v)-
L
hu8p(l)(<5)v](s),-y
+[hupp(P)v, hu8p(<5)v].
(26)
p,8~0
IPI+I8I>o
According to (2.10), the first term on the right-hand side is estimated by means of {V
}(s),-y'
The argument in Section 3.2 implies that {P(fi),P( 8)}(y,1J,' r) ~ c(I){P,P}(y,1J,1'),
where 1/31 + 181 > 0 and c(1') ~ 0 as 1 ~ -oo. In view of this, the second term on the right-hand side of (:26) can be estimate from above by means of c( 1 ){ v )2, whence follows inequality (24). The theorem is proved. Remark. Under the conditions of Theorem B it is possible to derive estimates in norms involving exponentially increasing (decreasing) weights. For more detail see Volevich [1] .
The Method of Energy Estimates in Cauchy's Problem
247
§4. Cauchy's problem for dominantly correct differential operators 4.1. In this section we shall prove that a dominantly correct symbol P(y; ~' r) solved with respect to the highest power of r:
P(y; ~' r) =
Tm
+L
Pa 1 .•• anf3(Y)~~ 1
• ••
~~nrf3
(1)
f3<m
satisfies all conditions of Theorem B, and hence Cauchy's problem is uniquely solvable for the corresponding differential operator P(y; D). Recall that, according to the definitions in Section 3.4.2, symbol (1) is said to be dominantly correct if the following conditions hold: (i) the polygons 8(P(y)) do not depend on y; (ii) Vy 0 E Rn+l the polynomial P(~,r) = P(y 0 ;~,r) is dominantly correct. For symbols satisfying (i) and (ii) we shall establish a strengthened version of Theorem 3.3, in which the conditions of the theorem are supplemented with a condition of "equivalence" of the variables 6, ... , ~n· We state the necessary definitions. Consider a symbol
(2) We denote by tl.(H(P(y))) the polyhedron in R 3 spanned on the triples (Ia I, /3, r) for which ha 1 ... anf3r(Y) =/= 0 for a1 +···+an = Ia I and on their projections on the coordinate axes. As usual, let fl.( H p) denote the convex hull of the union of all f'l.(Hp(y)) over y E Rn+I. We have
Theorem C. For a dominantly correct symbol (1) the following assertions bold: (a) f'l.(Hp(y)) = tl.(Hp) Vy E Rn+I; (b) :3/o, c > 0 such that tl1e estimate from below
Hp(y; 7J,/) > c
(3) (a,f3,r)Efl(Hp)
balds; (c) Vy E Rn+I and for any polynomials Q 1 (~,r), Q 2 (~,r), f'l.(Q 1 ) C f'l.(P),l) f'l.(Q2) C 8(P), there .is a function c:(1) such that c:(1)-+ 0 as 1-+ -oo and
(4) It is clear that symbol (1) satisfying the ccmditions (a), (b), and (c) satisfies the conditions of Theorem 3.3 and, consequently, the conditions of Theorem B. The proof of Theorem C is based on an equivalent description of dominantly correct polynomials in terms of the functions H p, and it is this question that is treated in the present section. l ) For
the notation 6.(P) see the Introduction to Chapter 2.
Chapter 7
248
4.2. The description of dominantly correct and stable-correct polynomials in terms of Hp. We have Theorem 1. For a polynomial P(~, T) solved with respect to the highest power ofT the following conditions are equivalent.
(I)
P(~, T)
is a dominantly correct polynomial (i.e. the equivalent conditions of Theorem 3.4.1 lwld for it). (II) The following conditions are fulfilled: (a) the polyhedron ~(Hp) C IR3 is reconstructed uniquely from the polygon h(P). (b) 3/o, c > 0 such that the estimate from below ( cf. ( 3))
(5) (a,fi,r)ED..(Hp)
holds; (c) For any polynomials Q 1 (~,T), Q2(~,T), ~(Ql) C ~(P), ~(Q2) C h(P), there is a function c(/), c('Y)--+ 0 as{--+ -oo, such that
(6)
The implication (Il)==?(I) is an immediate consequence of Theorem 3.4.1. Indeed, (5) implies that the polynomial P is correct in Petrovskil's sense. Further, let Q( ~, T) be a polynomial and let ~( Q) C h( P). In view of the relation
HP+Q = {P
+ Q,P + Q} =
Hp
+ {P,Q} + {Q,P} + {Q,Q}
(7)
and condition (c), there is 1( Q) such that
Hence, the polynomial P + Q is also correct in Petrovskil's sense, whence it follows that the original polynomial is dominantly correct. The proof of the implication (I)==?(II) is rather cumbersome and occupies the entire remaining part of this section. As in the case of Theorem 3.4.1, the central point here is the proof of the corresponding assertion for the case n = 1, while the proof for the case of n > 1 is obtained from the former by passing to polar coordinates ( ~ = pv.;). In the course of the proof of Theorem 1 we shall obtain an analogous description for the stable-correct polynomials as well. We shall prove
The Method of Energy Estimates in Cauchy's Problem
249
Theorem 2. For a polynomial P(C 7) solved with respect to the highest power of 7 the conditions below are equivalent.
(I) P(e, 7) is a stable-correct polynomial (i.e. it satisfies the equivalent conditions of Theorem 2.4.5; also see Theorem 3.4.3). (II) Conditions (a) and(b) of Theorem 1 are fulfilled as well as the strengthened version of condition (e): (cmax) VQi(e,7),~(Qi) C ~(P), i = 1,2, 3/'I ')' ~ /'I ·
(8)
Condition (cmax) and relation (7) imply that all polynomials P + c:Q, where ~(Q) C D.(P), are correct in Petrovski!'s sense for sufficiently small c. Therefore the polynomial P is stable-correct, i.e. the implication (II)===?(I) has been proved. Relations (c) and ( Cmax) are purely geometric conditions. The second of them is equivalent to the condition ( c~ax) if D.( Qi) C ~(P), i = 1, 2, then
D.({Q1,Q2})
C D.({P,P}).
As to the first of these conditions, to investigate it we need the following Definition. A point (a, /3, r) E D.(Hp) is said to be minor if there is a point (a', f3', r') E D.(H p) such that a ~ a', f3 ~ f3', and r < r'. The convex hull of the minor (integral) points of D.(Hp) will be denoted 8(Hp ). A geometrical equivalent of condition (c) is the condition (c') If Q1 and Q2 are polynomials and ~(Qt) C D.(P), ~(Q 2 ) C D.(P), then
The equivalence of (c) and ( c') follows from a simple lemma that will be presented below. Let Q(zo, z1, ... , zk) be a polynomial in k+1 variables with Newton's polyhedron N( Q) . A point (ao, ... , ak) E N( Q) is said to be minor if 3( a~, ... , ak) E N( Q), ao < a~, CXj ~ aj, j = 1 . .. , k. The points of N(Q) that are not minor are called senior. The set of the senior points will be denoted as 1r N( Q). The senior points belong to those faces of N(Q) which do not lie in coordinate planes and do not cont ain segments of straight lines parallel to the axis {a 0 }. Lemma. The condition
lzal ~ ca(zo)
L
lzPI,
ca(zo) ~ 0
;3EN(Q)
is fulfilled if and only if a E
N(Q) \ 1rN(Q).
as
lzo l ~ oo,
(9)
Chapter 7
250
Proof. Sufficiency. If a~ 1rN(Q), then a straight line parallel to the axis {ao} can be drawn through the point a, and let a = ( ao, ... , a k), ao > ao, be the point of intersection of this line with the boundary of the polyhedron N( Q). Then we have lzal/3(z):::::; const jzal/lzal = const lzolao-ao. Necessity. A point a E N(Q) \ 1rN(Q) is characterized by the property that no supporting plane {q, {J} = c > 0, q = eqo, . .. , qk), qo > 0, lq1l + · · · + lqk I > 0, can be drawn through it. It now remains to note that if such plane passes through a, then e9) cannot hold. Indeed, if there is q = eqo, ... , qk), qo > 0, such that
(q, a}
~
(q, {J} V{J
E
Ne Q),
then condition e9) is violated along the curve Zjet) = tqi, j = 0, ... , k. 4.3. The general scheme of the proof of the Theorems in Section 4.2.
As has already been mentioned, the most laborious part of the proof of the assertions stated in Section 4.2 is their verification for n = 1. According to Theorem 3.2.3, a dominantly correct polynomial Pee, r), e E IR, has the form
Pee,r) = .Pee,r) + Q(e,r),
NeQ) c h(P),
e1o) e11)
.Pee, r) = rb Ree, r)cee, r), where p.
R(e,r) =ITer- aiek),
Imai > 0,
bk are even numbers,
e12)
k=l
h
cee,r) =ITer -cje),
Imc·0 J- '
for
j
#
k.
e13)
k=l
It is obvious that if all assertions in Theorem 1 are proved for the polynomial
P,
then they will also be true for polynomial (10) with any Q, and the relation
N(Hp)
= N(H?)
(14)
will hold. Theorem 2 in Section 4 . 2 with n = 1 corresponds to the simpler case G Thus, we shall prove the following assertions. Proposition 1. Let a polynomial c > 0 such that
P h~ve
the form en)-e13). Then :3/o and
I:::::; /o,
HpefJ,!)>c
=1. e15)
(a,f3,r)EN(H j>)
where the constants /o and c in e15) depend on max lai I, max lei I, max elm aj) - l , ~ax lei - Ck l- 1 eon b and the numbers b1 , ••• , bk) solely. rf.k
251
The Method of Energy Estimates in Cauchy's Problem
Proposition 2. (i) Let a polynomial P have the fonn (11)-(13) and let C 1 and C 2 be polynomials such that N(C1 ) c N(P) and N(C2) c 8(P). Then
(ii) If G
=1 in (13) then i = 1, 2.
Proposition 3. If a polynomial P has the form (11)-(13), then the polygon N(H p) C ~ 3 is reconstructed uniquely from the polygon 8(P). Assuming that Propositions 1, 2, and 3 have already been proved we shall complete the proof of Theorems 1 and 2 in the foregoing section. As in Chapters 2 and 3, we put ~ = pw, p ~ 0, lwl = 1, and associate with the polynomial P( ~, T), ~ E ~ n, the set of polynomials
Pw(P, r) = P(pw, r).
(16)
According to Theorem 3.4.1, if the polynomial P is dominantly correct, then all polynomials (16) (in the variables p and r) are also dominantly correct, and we have (17) In case the polynomial Pis stable-correct, polynomial (16) is N -stable correct, and we have N(Pw) = fl(P) Vw E sn- 1. (17') Using (17) and Proposition 3 we conclude that the polyhedra N(Hpw) do not depend on w and are uniquely determined by the polygon 8(P):
(18) By virtue of Proposition 1, for each w E
Hpw(p, a, I)> c(w)
sn-I
L
(a,,B,r)
we can write the estimate from below
IPI 1ai,Bhlr, 0
(:(lo(w).
(19)
We can select unified constants c(w) and lo(w) for all w E sn-1 . Indeed, if P is a dominantly correct polynomial, then the polynomials Pw(P, T) have the roots Tj(p,w)
= aj(w)pb;(w) + o(pb;(w)), Tj(p,w)
= Cj(w)p + o(1),
Tj ( p, W) = Q ( 1),
p ~ oo,
j
j = 1, ... , k(w),
= 1, ... , h(w),
j = 1, ... , b(W),
Chapter 7
252
where the numbers bj(w), k(w), h(w), and b(w) are reconstructed uniquely from the polygon 8(Pw) and, according to (17), do not depend on w. The coefficients aj(W) and cj ( w) are determined from the polynomials PH] in §1.1. Since the coefficients of these polynomials are smooth functions of w, it can be shown that the numbers iaj(w)i and jcj(w)l are uniformly bounded from above and the numbers Imaj(w) and !aj(w)-ak(w)l, j -f. k, are uniformly bounded from below by nonzero constants. Thus, it can be assumed that "Yo and c in (19) do not depend on w. Noting that
we obtain assertion (b) in Theorem 1. Assertion (c) and, the more so, assertion ( Cmax) readily follow from Proposition 3. 4.4. The proof of Proposition 1 in Section 4.3. According to Theorem 5.2.2, the fulfilment of (15) is equivalent to the property that for any nonnegative vector q = (q 1, q2, q3), q3 > 0, we have
(20) provided that
")' < 0,
~
-f. 0
(if q1
> 0);
a
-f. 0
(if q2
> 0).
(21)
However, it is difficult to determine from Theorem 5.2.2 the character of the dependence of the constants c and "Yo in (15) on the coefficients of polynomials (11 ). In this connection we shall prove inequality (15) in two stages. We first estimate H P from above and below via a positive function T(~, a, 1') not depending on the coefficients aj and Cj in (12) and (13) and after that show that under conditions (21) we have
(22) Proposition. There are constants c, c', and 'Yo depending on the same parameters as c and "Yo in (15), such that the inequality
(23) holds, where IL
T( ~'a,")')
=
11'1( a2
+ 1'2)b-1 ( a2 + 1'2 + e)h II (a2 + 1'2 + ebj) j=l IL
+ ca2 + '1'2)b+h I:)I"YI + 1 ~ 1 bj) II ca2 + 1 2 + ebk) j=l
k-:f:.j
c24)
253
The Method of Energy Estimates in Cauchy's Problem forb~
1 and IL
T(e,a,,) =
bl(a2 +'2 +e)h-1 IIca2 +'2 +ebi) j=1 IL
+ (a2 + ,2)h l::cbl + ej) II (a2 + '2 + ebk) j=1 k=f.j forb= 0. Tbe constants c, and maxjc1· - ckl- 1 .
c',
(24')
and lo depend on max !ail, max lei!, max(Imaj)- 1 ,
j=f.k
Proof. Replacing the derivative 8PI 8T in the expression H P = - Im P8P I 8T by
we represent H P as a sum of three nonnegative terms:
(25) Letnma 1. If a polynomial R bas tbe form (12), tben for 1 ~ 0 we bave
,.,
d1 ~ IR(e, 7)1 21II (o- 2 + , 2 + ebj) ~ d~, j=1
(26)
a2 ~ HR(~,o-,,)II)I,I +ei) II
(27)
,.,
where d1 and
d2
depend on max !ail and max(Imaj)- 1 .
P·roof. In view of the (1, 1lbi )-homogeneity, it is easily shown that (28) where d depends on (Im ai )- 1 and !ai 1. Multiplying these inequalities we obtain (26). Estimating each factor in the expression HR =
l:::C-1 + lmajei) II IT- akek! 2 k=f.j
by means of (28) we derive (27).
Chapter 7
254
Len.tma 2. If G is a strictly hyperbolic polynomial, then
where d 3 depends on
lf,Jtlci- Ckl- 1
and max lei I·
This assertion is contained in Proposition 3.4. With account of (26)-(28), the right-hand side of (25) is estimated from above and below by means of
!Tic 0"2
+ ,2)bc 0"2 + ,2 + e)h-1 IIc0"2 + ,2 + ebj) + blfl(a2 + 12)b-liG(~, r)l2 II(a2 + ,2 + ebj) + (a2 +--?)biG(~, r)12 L(I'"YI + ej) II (a2 + ,2 + ebk) k#j
(29) We derive estimate (29) in t he case b ~ 1 leaving the simpler case b = 0 to the reader. Since all the terms in (29) are nonnegative, the right-hand side of this expression can be estimated from below by means of J 1 +c: 2 J 2 +c: 3 J 3 , where c: 2 , c: 3 < 1. We note that
Under the substitution of this inequality into c: 2 J 2 the second term on the righthand side yields an expression that can be estimated via J 1 for a sufficiently small c: 2 . In view of this, the factor IGI 2 in the expression for ]z can be replaced by ~2h. Therefore the sum of J1 and J2 is estimated from above and below by means of the first term on the right-hand side of (24). Similarly, in J3 we replace IGI 2 by
Since b1
~
. ..
~
b11
~
2, we have p.
e 2:)1,1 + ~~~bj) II ca2 + ,2 + ebk) ~~-"II (a2 + ,2 + ebj ), k=l
j#k
and therefore for a sufficiently small C:3 the sum J 1 + c: 2 J2 + c: 3 J 3 can be estimated from above by means of (24). The proposition is proved. Expressions (24) and (24') are polynomials in each of the octants of JR3 , and therefore the polyhedron N(T) C JR3 can naturally be defined. Since H P is estimated from above and below by means of T, we have
N(T) = N(H p)·
255
The Method of Energy Estimates in Cauchy's Problem
It follows that to prove Proposition 1 in Section 4.3 it suffices to verify the fulfilment of (22). If we open the parenthesis in expression (24) for T, this results in an expression of the form of T(~, u, 1) = ca,areau 2 ,allr,
L
which does not vanish outside the planes {~ = 0} and {u = 0} (we remind the reader that, according to (21), we have 1 < 0). Thus, (22) has been proved for the case ql,q2 > 0. Now let q2 = 0. Since u is involved in (24) only via expressions of the form of u 2 + 1 2 , the elimination of the monomials containing u in ( 29) .does not result in a reduction of the q-degree, that is
whence Tq(~,u,1) ~ Tq(~,0,1),
and it suffices to show that the right-hand side does not vanish. In application to T(~, 0, 1) we can repeat the above argument. If q1 > 0, then Tq(~, 0, 1) =/= 0. In case q1 = 0, it suffices to note that T(O, 0, I)= (J.L
+ 1)1fl2b+2h+2tt-1 =J 0,
Similarly, in the case q1 = 0, q2 > 0 it should be noted that
lui =J 0,
1 < 0.
Proposition 1 in Section 4.3 has been proved completely. 4.5. The proof of Proposition 2 in Section 4.3. To begin with, we prove the simpler assertion (ii). By virtue of Lemma 4.2, the inclusion relations in the proposition are equivalent to the corresponding inequalities for the monomials. In view of the lemmas in Section 4.4, it is more convenient to deal with the inequalities. By the linearity, it suffices to consider the case when Q1 and Q2 are monomials: Ql = rtt-i~a,
Q2 = rtt-k~.B,
a~ Bj,
f3 ~ Bk,
where Since {Q1, Q 2 } = -((J.L- k)r _ (J.L- j)r]rtt-i-s 7tt-k-l~a+.B,
the verification of (ii) reduces to the proof of the inequalities
enj ~ constHR(~,r,1),
(30)
lr12J.t-i-k-I~Bj-Bk ~ constHR(~,r,l)·
(31)
l1llrl 2"'- 2i- 2
Chapter 7
256
According to Lemma 1 in Section 4.4, we have ~J.-l
const hi
II (lrl 2 + ebt) ~ HR(~,r,,). 1=1
If t he terms lrl 2 are discarded in the factors corresponding to l = 1, ... , j and the terms ebt are discarded in the other factors, we obtain inequality (30). Before proving (31) we note that from the definition of the numbers Bj it follows that Bi
+ Bk < Bi-1 + Bk+1·
Thus, (31) is a consequence of the inequalities lri2~J.-21 ~Bt-Bt-1 ~ const
HR(C a,!),
(30')
lri2~J.-21-1 ~Bt+l +Bt-l ~ const HR(~, a,!)·
(30")
According to (27), we have
HR > const et
II(lrl 2 + ebj) > const lri 2
(1L-l) eBt-l+bt
= const lri 2(1J.-l) ~BI-l +Bt.
i¥=1
Similarly,
HR > constel+l
II (lrl + ei) II (lrl + ei) j-#1+1
> const
j-#1+1
[lri~-L-1-1 ~B,+bt+l] [lri~-L-1 ~Bt-l]
= const lr12~J.-2I-I aB1-1 +Bt+
1 •
We now turn to the proof of (i). Let us divide the polygon N(P) 3 (o:, !3) by means of the lines f3 = b + h and f3 = b into the three polygons N1 = {(o:, /3) E N(P), b + h ~
f3
~ b+ h
+ JL},
f3 ~ b+ h}, ~ f3 ~ b},
N2 = {(o:,/3) E N(P),b ~ N3
= {(o:,/3) E N(P),O
and let 81, 82, 83 be the corresponding partition of 8(P). Denote by ( a1, bz), l = 1, 2, 3, the points of N 1, N 2, and N 3 and by ( c,x, d,x) , ). = 1, 2, 3, the points of 81, 82 , and 83 . As in the case •(ii), the proof of (i) reduces to the proof of the inequalities lfllrlbt+d;x.-2l~la,+ c;x. ~ c(!)Hp(~ , a,/),
d_x = bt,
(32)
lrlbt+d;x.-ll~la,+ c;x. ~ c(!)Hp(~,r,/),
d_x =/:- bt,
(33)
The verification of these inequalities is quite simple and is based on the explicit form of the function (24). We shall consider some typical situations leaving the rest to the reader as a simple exercise.
257
The Method of Energy Estimates in Cauchy's Problem
1) Let l =.X= 1. Then bt = b+h+J-L-j, d1 = b+h+J-L-k, (j and c1 ~ Bk - 1, i.e. the left-hand side of (33) is no greater than
"#
k),
a1
~ Bj,
(34) As was shown in the proof of (ii), the point
{3 + r ~ 2J.L- j - k- 1, belongs to N(HR), and therefore, with account of the second term in (24), expression ( 34) can be estimated by means of c:( 1 )~o, 1 ~oo.
2) Let l = _,\ = 2. Then b2 = b + h- j, d2 = b + h- k, (k "# j), a2 ~ BJ-L + j and c 2 ~ BJ-L + k- 1, and the left-hand side of (33) is equal to (or no greater than)
1712b+2h-j-k-llci2B!'+j+k-l
=
1712b-2 [72h-j-k+llclj+k-l]
~ 1712b-2(1712
3) Let l =.X= 3. then a3,c3 ~ BIL left-hand side of (33) one should take
+ h,
eBI'
+ e)hiR(C, 7)12
~ const 111-1 H p·
b3 ~ b, and d3 ~ b- 1, and as the
4) Let l = 1 and .X= 2. Then on the left-hand side of (33) we shall have
The first and second square brackets are estimated by means of IRI2 and the last square bracket is estimated via (171 2 + e)h' the whole expression being estimated by means of const 111-l H p· The other cases are considered in the same simple manner.
4.6. The proof of Proposition 3 in Section ,4.3. Let b1 > b2 > · · · > bk ~ 2, bk+l = 1, and bk+ 2 = 0 be the degrees of the roots of the polynomial P and let J-lll ... , J-lk+l be the multiplicities of the roots. As was proved in Section 3.2.1, if the polygon 8(P) has a vertical side, then J-lk+ 2 ~ 2, and all the numbers (bj,J.Lj), j = 1, ... , k + 2, are reconstructed uniquely from 8(P). Since the behavior of function (24) depends in fact only on the numbers (bj,J-lj), the polygon t::..(Hp) is completely determined by the polygon 8(P). A similar situation takes place when the side of 8(P) adjoining the axis of abscissas intersects it at an angle no greater than 1r /4 (in this case J-l k+ 2 is sure to be equal to zero).
Chapter 7
258
We now consider the case when the side of 8(P) adjoining the axis of abscissas intersects it at an angle of 7r /4. In this case two different sets of the degrees of the roots and their multiplicities may correspond to the polygon 8(P), and the degrees of the roots greater than 1 (and the multiplicities of these roots) coincide, but in one of these cases we have J..lk+l
= h,
and in the other case f-lk+I
+ 1,
= h
J..lk+2
= 0.
In the former case H P is estimated from below by means of function (24) in which one should put b = 1. In the latter case H P is estimated from below using function (24') in which h should be replaced by h+ 1. As is easy to see, the indicated functions coincide, which proves the desired assertion. 4. 7. Concluding remarks. Dominantly correct and stable-correct polynomials and symbols are characterized by the invariance of their properties under linear tran~formations of the variables 6, ... , ~n· We shall briefly discuss the generalization of these notions to the case when no such invariance takes place.
e'
Definition 1. A polynomial P( T) solved with respect to the highest power of r is said to be N -dominantly correct if it is correct in Petrovskil's sense and if this property is not violated under the addition of the monomials c~ 0 rf3, where (a 1 , ..• ,an,f3) E 8°(P) (see Section 3.3). Definition 1'. A polynomial P(e,r) solved with respect to the highest power of r is said to be '}-{-correct if it satisfies conditions (ii) and (iii) of Theorem 3.3.
It is clear that every '}-{-correct polynomial is N -dominantly correct. The classes of polynomials in Definitions 1 and 1' were studied in detail by Gindikin [1]. These results imply that the property of '}-{-correctness is stronger as compared to the N-dominant correctness. We give an example of an '}-{-stable correct polynomial of the first degree with respect to the variable T. We divide the variables E Rn into two groups: = (f, e'), e' E JRk, E Rn-k, and consider the polynomial
e
e"
P(e,r) = r + (A,e")
e
+ Q(e') + iH(e'),
where H(e') is anN quasi-elliptic polynomial bounded from below; (A, e") is a real linear form on Rn-k; and Q(e') is a real polynomial, the integral minor points of N ( Q) being minor poiHts of N (H). Then the polynomial P is '}-{-correct. In Section 5.2.4 the definition of N -stable correct polynomials was stated. These are polynomials correct in Petrovski'i''s sense which are solved with res'p ect to the highest power of r, satisfy an inequality of the form of c3(~, r) ~
IP(e, r)l
for
eE Rn'
lm T ~ /o,
and have a complete and regular polyhedron N(P). We present some other definitions of these polynomials.
The Method of Energy Estimates in Cauchy's Problem
259
Definition 2. A polynomial P(e, r) solved with respect to the highest power of r is said to beN-stable correct if for any polynomial Q(e,r), N(Q) C N(P), there is
£
such that the polynomial P
+ cQ is correct in Petrovski1's sense.
Definition 2'. A polynomial P( e, r) solved with respect to the highest power of r is ~aid to beN-stable correct if it satisfies conditions (i) and (ii) in Theorem 3.3, and instead of (iii) a stronger condition is fulfilled:
N({Q 11 Q 2 }) C N(Hp);
N(Qt),N(Q 2 ) c N(P) .
In the above-mentioned paper by Gindikin [1] it is proved that Definitions 2, 2' , and 5.2.2 are equivalent.
REFERENCES
M.S. Agranovich and M. I. Vishik. 1. Elliptic Problems with a Parameter and General Parabolic Problems, Uspechi Mat . Nauk 19 n;.; . 3 (1964), 53-161. (Russian) V . M . Borok. 1. On Numerical Characteristics of Systems Correct in Petrovski1's Sense, Izv. Vyssh. Uchebn. Zaved. Mat. 1 no. 8 (1959), 16-22 . (Russian) A. D . Bryuno . 1. Lo kal'ny1 metod nelindnogo analiza differensial'nykh uravneni1 (A Local Method for Nonlinear Analysis of Differential Equations), "Nauka", Moscow, 1979. (Russian) N. G. Chebotarev . 1. T eoriya algebraicheskikh funktsi1 (Theory of Algebraic Functions), "Gostekhizdat" , Moscow, 1948. (Russian) Yu. V. Egorov. 1. Lin e'tnye differentsial 'nye uravneniya glavnogo tipa (Linear Differential Equations of Principal Type), "Nauka", Moscow, 1984. (Russian) 2. On the Solvability of Differential Equations with Simple Characteristics, Uspechi Mat. Nauk 26 no . 2 (1971), 183-198. (Russian) G. l . Eskin. 1. K raevye zadachi dlya ellipticheskikh psevdodifferentsial 'nykh uravnenit, "N auka", Moscow, 1973 (Russian); English transl. in Boundary-value Problems for Pseudodofferential Equations, vol. 52, Amer. Math. Soc., Providence, R.I., 1981. 2. Ca·u.chy's Problem for Hyperbolic Convolution Equations, Mat. Sb. 74 (1967), 262-297. (Russian) J . Friberg.
1. M'IJ.lliquasielliptic Polynomials, Ann. Sckola Norm. Super. Pisa 21 no . 2 (1967), 233-260 . B . A. Fuks and V. I. Levin. 1. Funksii kompleks.n ogo peremennogo i nekotorye ikh prilozheniya. Spetsial'nye glavy (Functions of a Complex Variabl~s and Some of Their Applications. Special Chapters), Gostekhizdat, Moscow, 1951. {Russian) S. G . Gindikin. 1. En ergy Estimates Relating to Newton's Polygon, Trudy Moskov . Mat . Obshch. 31 {1974), 189- 236. (Russian) 2 . On a Generalization of Paraboli c Differential Operators to the Case of Multidimensional Time, Dokl. Akad. Nauk SSSR 173 no . 3 (1967), 499-502. (Russian) 261
References
262 V. V. Grushin and N. A. Shananin.
1. Some Theorems on Singu.larities of Solutions to Differential Equations with Weighted Principal Symbols, Mat. Sb. 103 no. 1 (1977), 37-51. (Russian)
G. H. Hardy, J. E. Littlewood, and G. Polya. 1. Ineq·ualities, Cambridge Univ. Press, Cambridge, 1934. L. Jlormander. 1. Analysis of Linear Partial Differential Operators. II, III, Springer-Verlag, Berlin, Heidebberg,
New York, Toronto, Tokyo, 1983, 1985. 2. On the Theory of General Partial Differential Operators, Acta. Math. 99 (1958), 255-264. 3. Linear Partial Differential Operators, Springer-Verlag, Berlin, Gottingen, Heidelberg, 1963. 4:. Pse-udo-differential Operators and Hypoelliptic Equations, in: Amer. Math. Soc. Symp. on singular integrals (1966), 138-183. G. G. Kazaryan. 1. Estimates for Differential Operators, and Hypoelliptic Operators, Trudy Mat. Inst. Steklov.
HO (1976), 130-161. (Russian)
J ..J. Kohn and L. Nirenberg. 1. On the Algebra of Pseudo .. differential Operators, CPAM 18 (1965), 269-305.
R. Lascar. 1. Propagation des singularities des solution d'equation pseudo-differentialles quasi homogenes, Ann. lnst. Fourier 27 no. 2 (1977), 79-123.
J. Leray. 1. Hyperbolic Differential Equations, The Institute for Advances Study, Princeton, N .J ., 1953.
V. P. Mikhallov. 1. On the Behaviour at Infinity of a Class of Polynomials, Trudy Mat. lnst. Steklov. 91 (1967), 59-8 L (Russian) 2. The First Boundary-value Problems for Quasi-elliptic and Quasi-parabolic Equations, Trudy Mat. Inst. Steklov. 91 (1967), 81-99. (Russian) L. Nirenberg and F. Trevers. 1. On Local Solvability of Linear Partial Differential Equations II. Suficient Conditions, CPAM 24 (1971), 459-509. B. P. Paneyakh. 1. Some Inequalities for,. Functions of Exponential Type and a Priori Estimates for General Diff'erential Operators, Uspekhi Mat. Nauk 21 no. 3 (1966), 75-114. (Russian) I. G. Petrovski1.
1. On Cauchy's Problem for Systems of Linear Partial Differential Equations for Non-analytic Functions, in: Izbrannye trudy. Systemy uravnenit s chastnymi proizvodnymi. Algebraiches/.:.aya geometriya (Selected works. Systems of Partial Differential Equations), "Nauka", Moscow, 1986, pp. 98- 168. (Russian) 2. On Cauchy's Problem for Systems of Partial Differential Equations in: Izbrannye trudy. System·l.f uravnenit s chastnymi proizvodnymi. Algebraicheskaya geometriya (Selected Works. Syste'lll.s of Partial Differential Equations), "Nauka", Moscow, 1986, pp. 34-97. (Russian)
References
263
N. /\. Shananin. 1. On Docal Solvability of Equations of Quasi-principal Type, Mat. Sb. 97 no. 4 (1975), 503-513.
( R u,:;sian) 2. An Example of a Locally Unsolvable Differential Equation of Quasi-principal Type With Real Weighted Principal symbol, Mat. Zametki 19 no. 5 (1976), 755-761. (Russian) G. E. Shilov. 1. Matematicheskit analiz. Vtoroi' spesial'nyi' kurs (Mathematical Analysis. The Second Special Co-u.rse), "Nauka", Moscow, 1965. (Russian)
M. Taylor. 1. PsC'Ildo-differential Operators, Princeton Univ. Press, Princeton, 1971.
L. IL Volevich. 1. EneTgy Method in Cauchy's Problem for Differential Operators Correct in Petrovskii"s Sense, Trudy Moskov. Mat. Obshch. 31 (1974), 147-187. (Russian) 2. Local Properties of Solutions to Quasi-elliptic Systems, Mat . Sb. 59 {101) (1962), 3- 52. (Rus-
sian) L. fL Volevich and S. G. Gindikin. 1. O!Joshennye funksii' i uravneniya v svertkakh (Distributions and Convolution Equations), "Naukn", Moscow, 1992, (in print) (Russian) English transl. in Distributions and Convolution EqulLtions, Gordon and Breach science Publishers, London, 1992. 2. On a Class of Hypoelliptic Polynomials, Mat. Sb. 75 (117) no. 3 (1968), 400-416. (Russian) 3. Pscudodifferential Operators and Cauchy's Problem for Differential Equations with Variable Coefficients, Funktsional Anal. i Prilozhen. 1 no. 4 (1967), 8-25. (Russian) 4. Ca.'nchy 's Problem for Differential Operators with Dominating Principal Part, Funktsional Anal. i Prilozhen. 3 no. 3 (1968), 22- 40. (Russian) 5 . Cauchy's Problem for Pluriparabolic Differential Equations I, II, Mat. Sb. 75 no, 1 (1968), 64- 105 (Russian) 78 no. 2 (1969), 214- 236. 6. Ccmchy's Problem, VINITI. Sovremennye problemy matematiki. Fundamental'nye napravleniya 32 (1988), 4-98. (Russian) 7. N e-wton's Polyhedron and Local Solvability of Partial Linear Differential Equations, Trudy Mos kov. Mat. Obshch. 48 (1985), 211- 262, Moscow. (Russian)
L. H . Volevich and B. P. Paneyakh. 1. S ome Spaces of Generalized Functions and Embedding Theorems, Uspekhi Mat. Nauk 20 no. 1 (1lJ65), 3-74. (Russian)
K. Yosida. 1. Fun ctional Analysis, Springer-Verlag, Berlin, Gottingen, Heidelberg, 1965.
INDEX
2b-parabolic polynomials
54
1r-cones 181 1r-cylinder 181 q- homogeneous part 1 q- homogeneous polynomial 6
q-order part of a polynomial 5 q-principal part 1,12 q-principal part of a polynomial 5 Complete polyhedron 112 Differential operator of N -principal type 13 5 Direction vector 5 Direction vector of a half-space 179 Dominantly correct polynomial 93 Equivalent polynomials 1 Essent]al variable 121 Exponentially correct polynomial 51 Exponentially correct symbol of constant strength 85 Fourier transform 29 for inversion formula 30 Homogeneous Cauchy problem 12 Hyperbolic polynomial 54 Hypoelliptic polynomial 24-25 Minor monomials Minor point 4
4, 58
N quasi-elliptic differential operator 27, 3 3 N quasi-elliptic differential operators with variable coefficients 33 N quasi-elliptic polynomials 22, 25 N-parabolic polynomials 60 265
266
N-parabolic polynomials and operators 175 N -stable correct polynomials 61 Newton's polygon of a polynomial 2 Newton's polyhedron of a polynomial 158 Normal cone 5 Normal cone of a face 179 Operator of principal type 119 Operators of q-principal or quasi-principal type 120 Operators of constant strength 45 Parabolic polynomials 80 Parseval relation 30 Polynomial of N -principal type 119, 127, 184 Polynomials correct in Petrovski1 sense 51 Polynomials of N -principal type 124 Polynomials with regular Newton's polygons 24 Puiseux's series 10 Quasi-elliptic polynomial 114 Quasi-homogeneous polynomial 6 Quasi-homogeneous polynomials correct in Petrovski1's sense 52 Regular Newton polygon 24 Regular polyhedron 173 Semi-cylinders 195 Senior point (monomial) 4 Stable-correct and parabolic polynomials in several variables 75 Stable-correct polynomials 80 Strictly pluriparabolic polynomial 24 2 Strictly pluriparabolic symbol 24 5 Supporting half-plane 5 Supporting half-space 179 Supporting line of a polygon 5
Index