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(1)

R ENDICONTI

del

S EMINARIO M ATEMATICO

della

U NIVERSITÀ DI P ADOVA

S. Z AIDMAN

On asymptotic series of symbols and of general pseudo-differential operators

Rendiconti del Seminario Matematico della Università di Padova, tome 63 (1980), p. 231-246

<http://www.numdam.org/item?id=RSMUP_1980__63__231_0>

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(2)

Asymptotic Symbols

and of General Pseudo-Differential Operators.

S. ZAIDMAN

(*)

Introduction.

In their

study

of an

algebra

of

pseudo-differential operators [6],

Kohn and

Nirenberg presented concepts

of canonical

pseudo-differential operators, asymptotic

series of such

operators-related

to the notion of order and

true-order,

-,

homogeneous symbols

of real

degree, asymptotic

sums of such

symbols

and the mutual connection between them. A very

interesting

existential

result, apparently belonging

to

H6rmander is

given

in Theorem 2

(iv)

of

[6] (see

also

[4]

and

[1]).

Similar facts are known in various other classes of

symbols

and

associated

pseudo-differential operators (see [5], [8], [10], [11], [12]).

In the

present

work we

introduce, following [6]

and

[13],

a class

of

symbols

which are

only

measurable with

respect to ~

E Rn -

{0}

and C°° for x E

(precise

definition will

follow)

and we indicate how the above mentionned

concepts

and results can be extended to this

new situation. We will refer to

[14]

for a

preliminary

version of a

part

of this paper

(general pseudo-differential operators

were not con- sidered

there).

1. - We consider a class of

symbols

which is denoted

by 6;

it

consists of measurable

complex-valued

functions

a(x, ~)

which are

defined on

(*)

Author’s address:

Department

of Mathematics, Universite de Montr6al Case

postale

6128, Montreal, P.Q., Canada.

This is a research

supported through

a

grant

of the Natural Sciences and

Engineering

Research Council, Canada and

by

the C.N.R. of

Italy.

(3)

We assume the

following properties:

a)

lim

a(x, ~)

= exists for

all $

and is a

x-oo

measurable bounded function

there;

b)

if

cr’(x, ~)

means the difference

6(x, ~) -

then

n

where x - 21 =

I x,271, q c- Rn,

while

6’(n, E)

is a

complex-valued

func-

1

tion defined on Rn xRn -

{0}

which is measurable

in q

for

all ~

c

c Rn -

{0},

is measurable

in E

for

all n

c- Rn and satisfies an estimate

REMARK. The function

c~’ (~, ~)

is the Fourier transform in the

sense of

temperate

distributions of the bounded function

~).

Furthermore

6’(x, E)

and

a(x, $)

are

OCO(R:)

x and

sup

(x,E) &#x3E;

/D:a(x, E)|

oo,

Va =

(«1... «n),

a multi-index of

non-negative integers.

Let us consider now an infinite sequence of functions in

6,

and a

strictly decreasing

sequence of real numbers

convergent

to - oo, ro &#x3E; r2 ...;

also,

we consider a

OCO(Rn)

function

C($),

which

is

non-negative, equals

0 for

~~~ c 2 , equals

one for such that

0~)1,

Our main interest in this section is about series of the form

and is a

(conveniently chosen)

sequence of real numbers.

Note

0

that for any

fixed ~

E

{01

the sum is finite

it equals

and in any it is written also as

(4)

We may define the function

Obviously

that

a(x, ~)

- 0 for

I~I 1,

x E Rn and that it is a measur-

able

complex-valued

function. The limit

~)

exists

f or ~

e Rn -

{o}

being given by

accordingly,

the difference

a’(x, ~)

-

a(x, ~)

-

a(oo, ~)

is

expressed by

We see that

~(x, ~)

is

infinitely

differentiable with

respect

to x, for any

2. - In this section we shall

give

a

global

estimate

(i.e.

on Rn x

fOI)of

the above defined function

a(x, ~)

and of the remainders of order N:

Precisely

we will prove the

following

THEOREM 1. - It is

possible

to choose a sequence

of

real numbers

to

=

1,

such that the

inequalities :

be

satisfied. (In particular,

the estimates

(5)

PROOF. -

Any

function in the class Q5 is bounded on Rn

xRn- ~0~ ;

let be

Mj

= (z,.;)

sup E)|, j

=

0, 1, 2,

....

We indicate a choice of the sequence in such a way that the estimates

be all verified.

Actually,

for

’(Eft;)

= 0 and the estimates are obvious.

For we remark

firstly (using

the

inequality

Consequently,

we can obtain

(2.3)

as a consequence of the

stronger inequalities

or

We know that r~_1- ri &#x3E;

0,

7

b’~

=

1, 2, ...

hence

We choose

now t,

in such a way as to have

that is

This

special

choice of the sequence

( t~ ) i

has

(2.3)

as a

corollary.

We

have seen that

a(x, ~)

= 0 for x E

I~I:!;

consider

now ) I~I : 1.

In this

Assume

ti =

2 or

bigger.

Then =

1, 2, ...

and = 0

for j

=

1, 2, ...:

Hence

~)

reduces for

these ~

to the

single

term

~)

=

E)

and we

get E) c

0

1$1 1,

x C Rn.

(6)

Consider now

I~I:&#x3E; 1.

In this case

Vj = 1, 2, ....

We

can deduce that

Let us estimate now

b,(x, $)

for N =

1, 2, ...:

-.

If and because

i&#x3E;2,

= 0

for j = ~ ~ +1,...;

thus

for

1~11,

For we have when

j

&#x3E; N. Therefore we

get

Consequently

This ends the

proof.

3. - We shall use here formula:

It follows that

~)

admits a

partial

Fourier

transform,

with

respect

taken in

8’(R")-sense,

which

equals

We can write also:

which is a finite sum for any

Let us consider

also,

as in

previous section,

the remainders of order N:

(7)

and their

partial

Fourier transform:

Therefore we are now

ready

to state the

following

THEOREM 2. A convenient selection

o f

the real sequence

(t,)’

where

to

=

1,

I

t1 &#x3E; 2 ,

allows

inequalities

where

PROOF. We

know,

because each

belongs

to

Q5,

that

~(~,~)~~(~)

where

We shall define a real sequence in such a way that the

inequalities

be all verified =

(1 -~- ~~,~2)~1~~(~,)~.

We shall look for

(t3)o

such

that,

if

~j&#x3E;~,,

then

This is

equivalent

with

and is

obviously implied by

(8)

Thus,

a

good

sequence

(t~)o

should

satisfy

the estimates

We see now that

(3.3)

is indeed true.

This is obvious all terms at left are null.

For we have

obviously

and we

apply (3.4)

and

get (3.3).

We are now

ready

to establish the

estimate

(3.1 ). Again

we see that

~(~~)E=0

for

1~I:t; next,

for

! : I~I : 1,

if and

~&#x3E;2,

we see that

a’(~,, ~) _ ~(~) ~~~r~a"co(~,, ~)

and

accordingly

will be :

Now,

for we see that

~~~% ~==1,2,...;

then

00

If

K(2)

=

(a

measurable function which has ob-

?=i

viously

a finite

integral, -using

Th. of B.

Levi-(see [3], [7]),

because

we obtained:

and we have

only

to prove that

(9)

Returning

to the definition of

K(Â)

we see that:

The first sum is

finite,

therefore E L1 as

requested.

In the second sum I is smaller

than j,

therefore

(

; (1 +

=

1~~ (~,)

and it follows that

Another

application

of B. Levi’s theorem

implies

the result.

Similar

reasonings apply

in order to prove

(3.2).

For

6’ (A, ~)

= 0 VA =

17 2,

...: -. For

1~1&#x3E;1

we shall use the same

sequence as above. We

get:

00

The

integrable

function

l~N(~,) (it

is so

again by

N+1

monotone sequences

theorem)

will be denoted with

K~V(£).

We still have to show that

(1 + Vp

=

1, 2, ... ,

which is a consequence of:

In

fact,

for we have

while for p

&#x3E; N +

1 we write:

(10)

The first sum at

right

is

finite,

thus

E Ll;

in the second sum,

(1 +

so that

again

B. Levi’s theorem will

give

the

requested

result.

4. - Here we start considerations on

pseudo-differential operators

associated to

symbols

in

6;

canonical

pseudo-differential operators

associated to

symbols

of

degree r, (i.e.

of the form

~) ~(~ jt) ~~ ~r,

r E E

R+) asymptotic

series of such canonical

operators

and

pseudo-

differential

operators

which are sums of these

series,

associated to

symbols verifying (2 .1 ), (2.2),

and

(3.1).

Our main

interest,

as indi-

cated in the

Introduction,

y is to state and prove an

analogous

of the

existential result Theorem 2

(iv)

of

[6]

for our-somewhat different- classes of

symbols.

To start let us remark that the class C is more

general

than that

defined in our paper

[13];

we

kept i)

and

iv)

but not

ii)

and

iii).

This

is

enough

however in order to define the

operator a(x, D)

=

A, by

formula:

and prove that where HS

are the Sobolev spaces of real order s

(on Rn).

Therefore

a(x, D)

will extend

by continuity

to a linear continuous

operator

from into

itself, ds E R,

therefore from

-

n

into itself. Consider now a function

~/~ ~

e

l~t

as

seR

defined in section

1~

and then for a

real r,

a function

~r(~/t)

= 0 for

-- ~(~/t) I ~ ~r9

for

~~ I ~ 2 t.

Remark now that

~)(1 + )$)2)I

and

~~~r~ (~ -~-- l~12)rI2

for r~ 0

while for and

(1 + j~j~~j-2~ 1 + ~)-2~i-)-4~-2~~~

Therefore we can derive

We can define an

operator given by

the formula:

(11)

being

the inverse Fourier transform.

Estimating

the

g’s-norm

we

get

Therefore,

extends

by continuity

to an

operator

in

Hs-r)

V real s, and

consequently

it will map Hoo into itself. We

call,

follow-

ing [6],

y any

operator Cr(D/t)a(m, D),

Hoo - Hoo a canonical

operator

of

degree

r. We see that

Now we shall define the

concept

of an

asymptotic representation

of a

linear

operator through

a sequence of canonical

operators

of

degree

r,,

(r,)’ being

a

strictly decreasing

sequence of reals con-

vergent

to - oo

(or

a finite sequence, ... &#x3E;

rN).

We need the

definition of order and true order of a linear

operator

in which is

given

below in a form

slightly

more detailed than in

[6] (see [1]

for

a

different,

« non-linear » definition of the

order).

Denote

by

Lin

(Hoo)

the vector space of all linear

operators,

Hoo - Hoo. Given an

operator

we associate to it a subset of the real

line, (order

of

Z),

which can be the

empty

set

too, by

means of the

following:

DEFINITION 4.1. such

that,

with

property

that

Let us remark that if and

r’ &#x3E; ro ,

then too.

Next,

the true order of .L is

by

definition:

t.o.

(L)

= inf

c~ (.L) ,

the

greatest

lower bound of

0 (L) .

If

0(L)

is the whole real

line,

t.o.

(L)

_ - oo.

The true order can

belong

to the order set or

not;

a

thorough

discus-

sion of these

concepts

in a

slightly

more

general

frame-work will be

presented

in

[15].

(12)

We are thus able to

give

DEFINITION 4.2. Let

(r~)o

be a

strictly decreasing

sequence

of

real

numbers,

and

D))§’

be a sequence

of

canoni-

cal

operators of degree corresponding

to a sequence

of positive

reals

and to a sequence

of symbols E)}oo0

c 6. A linear

operator M,

0

0

- Hoo is

asymptotically expanded

in to the series

ECrj((1/tj) D)aj(x, D)

if

the

following

holds : ~"°

We say that

Our main

goal

in the

remaining

of this paper is to prove the

following

THEOREM 3. Let be

given

a sequence

of symbols

in 6

and a

strictly decreasing

to - oo

in f inite

sequence

o f

real

numbers, Then,

there exists a sequence

of

canonical

operators of degree Kj

and

a linear

operator

P in

Hoo,

such that :

PROOF. We shall construct canonical

operators Xi

in the

following

way: First consider a fixed function

C($), 0 c ~( ~ ) c 1, ~(~) = 0

for

~~ ~ c 2 ~ ~(~) = ~

for

[ $ ] &#x3E; 1 ,

Next define a sequence of real numbers

(t~)o

as follows :

where,

y we

remember,

y

being

associated to as in

(1.2).

(13)

This choice of the sequence

(t~)o

will

permit, according

to Theo-

rems 1 and

2,

construction of a function

~) verifying (2.1), (2.2), (3.1), (3.2) simultaneously.

Now, K;

is

by

definition the

operator D)

cor-

responding

to the

symbol a;(x, ~)

and to the real rj

given

and

tj

chosen in the way indicated above. In terms of Fourier transform we have the

following representation

formula for the action of a canonical oper- ator on

Let us define now the

operator P;

remark that

satisfies estimates which are somewhat different from those

defining

the class

6;

still we can associate to it a linear

operator

in H’

by

means of similar formulas as those

defining a(x, D)

when

a(x, ~)

E 6.

Therefore,

let us

put,

for u

e 8(Rn)

If we consider

separately

the

operator

we

have

immediately

(when

we use

(2.2)

and the fact that

~)

= 0 for

l~l ~ 2

because

then

+ ~~~2)’’’~2

for

1~1&#x3E;!,

for any real

ro).

If we look now

at the

integral:

we see first its absolute

R.

convergence, for

(14)

Remember that

(1’ (Â, g)

= 0 for

c 2 ,

therefore

too

for ~

in the same

sphere.

For

bigger

we can use estimate

(3.1); accordingly

-because is bounded on

Rn;

now 00.

Rn -

Therefore,

the function

for ~

E Rn is well defined

for ~ verifying

the

inequality ~G(~) ~ 1 Cz(1 + I ~ ‘2 )r®~2 ; G ( ~ )

is also a measurable function as

easily

seen

(the

is

convergent

when S2 is

bounded).

Accordingly

we can take the inverse Fourier-transform of

(2~)’~C(~)

in

S’(Rn)

sense and obtain

P’ (z, D) u

E

8’(Rn).

We establish now an estimate in Sobolev spaces for P’ too. We shall see that

We must therefore

give

an upper bound for the norm of the function

it results

(15)

Substituting q’ for $ - q

and

applying

Minkowski’s

inequality

for

integrals

we obtain the

required

result.

Accordingly, P(x, D)

=

P(c&#x3E;o, D) + P’(x, D)

will

verify

the same

inequality,

for any real number s.

Thus,

and t.o.

(P)

c ro.

The final

part

of our

proof

deals with upper bounds for the true

N

orders of all

operators

N =

1, 1, 2, ... :

;=0 N -

Let us

give

first the

representation

formula

o

J

We know that

K; maps 8

in

H’,

we take Y in We have:

Therefore it is:

Using

notations

in § 2 and §3

we have:

and because of

(2.2)

and of

vanishing

of

bN

near the

origin

we

get

also

and the estimate

(16)

Therefore

In the same way as above we derive:

Therefore t.o. which is

strictly

rN as

requested.

This ends our

proof.

REFERENCES

[1]

A. ANDREOTTI,

Operatori pseudodifferenziali (Note

di S.

Spagnolo),

Uni-

versità

degli

Studi di Pisa

(1966-67),

pp. 1-171.

[2]

J. BARROS-NETO, An Introduction to the

Theory of

Distributions, Marcel Dekker Inc., New York (1973), pp. 1-215.

[3]

W. H. FLEMING, Functions

of

several variables,

Addison-Wesley

Publ.

Comp.

Inc. (1965).

[4] L. HÖRMANDER,

Pseudo-differential

operators, Comm. Pure

Appl.

Math.,

18,

n. 3 (1965), pp. 501-517.

[5]

L. HÖRMANDER,

Pseudo-differential

operators and

hypoelliptic equations (Singular Integrals,

Proc.

Symp.

Pure Math. X, Amer. Math. Soc. 1967),

pp. 138-183.

[6]

J. J. KOHN - L. NIRFNBFRG, An

algebra of pseudo-differential

operators, Comm. Pure

Appl. Math.,

18 (1965), pp. 269-305.

[7] I. P. NATANSON,

Theory of functions of

a real variable

(russian),

Moscow-

Leningrad,

1950.

[8]

L.

NIRENBERG, Pseudo-differenlial

operators,

(Notes by

W.

Sweeney),

Lectures at Global

Analysis Symposium, Berkeley,

1968.

[9]

R. SEELEY,

Topics

in

pseudo-differential

operators, Lectures at C.I.M.E., Stresa, 1968; Edizioni

Cremonese,

Roma, 1969.

[10]

M. TAYLOR,

Pseudo-differential

operators,

Springer-Verlag,

vol. 416, Lec-

ture Notes in Mathematics, 1974.

[11] F.

TREVES,

An introduction to

pseudo-differential

operators and Fourier

integrals

operators, Universidade Federal de Pernambuco, Instituto de

Matematica,

Recife, 1973.

(17)

[12]

F. TREVES,

Boundary

value

problems for elliptic equations,

Lectures at C.I.M.E., Bressanone, 1967,

Liguori

Editore.

[13]

S. ZAIDMAN, Some

non-homogeneous symbols

and associated

pseudo-dif- ferential

operators, Ann. Sc. Norm.

Sup.

Pisa, 31

(1967),

pp. 547-574.

[14] S. ZAIDMAN, Notices Amer. Math.

Soc.,

October 1978.

[15]

S. ZAIDMAN, Order and true order ...

(in preparation).

Manoscritto

pervenuto

in redazione il 23 novembre 1979.

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