• Aucun résultat trouvé

Cohomology of the Lagrange complex

N/A
N/A
Protected

Academic year: 2022

Partager "Cohomology of the Lagrange complex"

Copied!
12
0
0

Texte intégral

(1)

A NNALI DELLA

S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze

W. M. T ULCZYJEW

Cohomology of the Lagrange complex

Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4

e

série, tome 14, n

o

2 (1987), p. 217-227

<http://www.numdam.org/item?id=ASNSP_1987_4_14_2_217_0>

© Scuola Normale Superiore, Pisa, 1987, tous droits réservés.

L’accès aux archives de la revue « Annali della Scuola Normale Superiore di Pisa, Classe di Scienze » (http://www.sns.it/it/edizioni/riviste/annaliscienze/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une infraction pénale.

Toute copie ou impression de ce fichier doit contenir la présente mention de copyright.

Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques

http://www.numdam.org/

(2)

W.M. TULCZYJEW

Introduction

The

Lagrange complex

was introduced in connection with the inverse

problem

of the calculus of variations of curves in a differential manifold

[6], [7].

Only

the Poincar6 lemma was

proved.

The

cohomology

of the

complex

was not

studied. Similar

complexes

were introduced later

by

other authors in the calculus of variations of sections of differential fibrations and

cohomology

theorems were

proved [1], [5], [9].

These results are not

applicable

to the calculus of variations of curves.

Cohomology

of the

Lagrange complex

is studied in the present note.

A theorem

relating

the

cohomology

of the

complex

to de Rham

cohomology

of the manifold is

proved.

Bundles of k-velocities introduced

by

Ehresmann

[2]

are used

together

with the

theory

of derivations formulated

by

Fr6licher

and

Nijenhuis [3]

and

adapted

to the present

application

in

[4].

The relation between the

Lagrange complex

and the

Euler-Lagrange equations

of the calculus

~

of variations was discussed in

[8].

1. - Bundles of k-velocities

Let M be a differential manifold. In the set

of

smooth curves in M we introduce an

equivalence

relation for each

nonnegative integer

k. Two

curves

1: 1R -+

M and

k-equivalent

if

Db(1

o

~’) - Do( f

o

7)

for each smooth function

f

on M

and j

=

0,..., k).

The

symbol DIF

denotes

the derivative of

order j

of a function F:11~ -~ R at 0. The

k-equivalence

class of a curve 1 will be denoted

by

The set of all

k-equivalence

classes

of smooth curves is denoted

by T~M

and called the bundle of k-velocities in M. The bundle

projection r1: Tk M ---+

M is defined

by 7-kM(tk-f) = ~(0).

Pervenuto alla Redazione il 6 Febbraio 1986.

(3)

For k’ &#x3E; k a

mapping Tk’k~ : T ~~ M -~

is defined

by TMk~ (t~~7) - tb.

Relations TM kk

o

k’,k"

=

hold

for

"k’’ &#x3E; k’’ &#x3E;

k. The

mapping ToM

is

bijective.

Consequently

we

indentify T°M

with M and

TM

with

rt.

The

1-velocity

bundle

T 1 M

is the tangent bundle T M of M.

Let

f

be a smooth function on M.

For j = 0,...,

k we define functions

Ii

on

TkM by

o

1). For j

0 we set 0. The bundle

TkM

can be

given

a

unique

structure of a differential manifold such that if

are coordinates in an open submanifold U C M then

are coordinates in

TkU -

c

TkM. Mappings

are differential fibrations. The fibration M is of

fibre-type R km

if m is the

dimension of M.

2. - Forms and derivations

00

Let

4$k = $ 4S§J

be the exterior

algebra

of differential forms on

TkM.

For q=o

each k, is a differential

graded algebra

with the exterior

product

denoted

by

A and the exterior differential denoted

by

d.

Mappings

defined

by

, are

injective homomorphisms

and

satisfy

relations

for k" &#x3E; k’ &#x3E; k. It follows that the system

((Dk, p~, )

is a direct system.

Let C = be the direct limit of this system. We use a canoni- cal contruction of the direct limit. Each space (Dq is defined as the quo- tient of the

disjoint

union

by

the

equivalence

relation

according

to which two

elements 1L

and

//

of and

respectively

are

equivalent

if there is an

integer

k" such that

k" &#x3E;

k, k" &#x3E; k’ and The

space I&#x3E;

is defined as the

quotient

of the

disjoint

union

Uk by

the same

equivalence

relation. It is

canonically

identified with the

product

of the spaces Each

mapping pk

defined as the restriction to of the canonical

projection

of

Uk (Dk

onto I&#x3E; is

injective. Spaces

have

unique

vector space structures and tb has a

unique

structure of a differential

graded algebra

such that

mappings pk

are differential

graded algebra homomorphisms.

The exterior

product

in (D is

denoted

by

A and the exterior differential is denoted

by

d. We

identify

elements

of with their

images

in (D

by p*’.

(4)

Let e: R :--; be the

mapping

which turns numbers into constant functions.

The sequence

is a cochain

complex.

For q &#x3E; 0 the

quotient

space Ker

(d :

-~

1&#x3E;6+ I) jlm (d :

1&#x3E;6-1

I ---&#x3E; denoted

by Hq (M;R)

and called a de Rham

.cohomology

space.

We will denote

by

the

quotient

space Ker

(d :

-. Since

TkM

is a bundle with Euclidean fibres the

cohomology

spaces for the chain comnlex

are

isomorphic

to the de Rham

cohomology

spaces. The same is true of the direct limit

complex

A derivation of O of

degree

r is a linear operator a: tb - C such that

and

if tL

E (Dq. The exterior differential d is a derivation of

degree

1. We denote

by

i the derivation of

degree

0 defined

by

= qlL

if IL

E (Dq. If a is a derivation

of

degree

r then

The commutator

of derivations a and b of

degrees

r and s

rispectively

is a derivation of

degree

r + s.

A derivation is said to be of

type i*

if it acts

trivially

in A derivation a is said to be of type d* if

[a, d]

= 0. If

iA

is a derivation of

type i*

then

dA

=

[iA, d]

is a derivation of type d*. All derivations of type d* can be constructed in this way from derivations of

type i* [4].

A derivation of

type i*

is

completely

characterized

by

its action Derivations are local operators and for each k

an element of is

locally expressed

as a sum of differentials of coordinates

multiplied by

functions on

TkM.

If follows that to define a derivation of

type

i* it is

enough

to

specify

its action on the differentials

dfj

of functions

fj

defined in Section 1.

A derivation

iT

of

type i*

and

degree -1

I is defined

by

(5)

for . The

corresponding

derivation

is of

degree

0.

For each

nonnegative integer n

a derivation

iF(n)

of

type i*

and

degree

0 is

defined

by

..

The derivation is the derivation i defined above. For n 0 we set = 0.

Relations

are

easily

verified.

3. - The

Lagrange complex

Let a linear operator r : O - 4S be defined

by

The series converges since for

each 1L

in ~, = 0 for

sufficiently large

n.

PROPOSITION 3.1.

T dT

= 0, T T = Ti a nd T d T = 7-di.

PROOF. The first

equality

is

proved by

The

remaining

two

equalities

follow

immediately

from the first.

Q.E.D.,

Q.E.D.

I

We define a sequence of

operators

(Dq

by

and

rqtt

if

q &#x3E; 0. It follows from

Proposition

3.1 that

TqdTO

= 0 for q &#x3E; 0. Also TqTq = 7-q and

Tq+ ’d 7-q

=

for q

&#x3E; 0. We introduce a sequence of

subspaces

Aq c 4S~

defined

by

Aq = and a sequence of linear

operators

Aq+1

(6)

PROPOSITION 3.2. The sequence

is a cochain

complex.

PROOF. From it follows that

we have

DEFINITION 3.1. The sequence

is called the

Lagrange complex.

Local exactness of the

Lagrange complex (the

Poincar6

lemma)

was

proved

in an earlier

publication [6].

The

following

theorem relates the

cohomology

of

the

Lagrange comples

to the de Rham

cohomology

of the manifold M.

THEOREM 3.1. For

q &#x3E;

0 the

Lagrange cohomology

space

Lq(M) =

Ker

isomorphic

to the direct sum

(M; R) ED Hq(M; 1R) of

de

Rham

cohomology

spaces, and

L-1 (M)

is

isomorphic

to

HO(M; R).

4. - Proof of the

cohomology

theorem

Let a linear be defined

by

This operator is related to the operator r

(7)

PROPOSITION 4.1.

PROOF.

The

remaining

two

equalities

are

easily

verified.

Q.E.D.

For q &#x3E; 0 we define operators 0, q: (Dq -&#x3E;

by (J q J.L =

q Relations

7-q +

dT(Jq =

1,

(1qdT =

1, QqTq = 0 and

0, q, ’d -

daqfollow from

Proposition

4.1.

We will denote the direct sum of vector spaces r and A

by (0)

and

adopt

matrix notation for linear

mappings

between direct sums of vector spaces.

In terms of this notation we write A-’ =

((DO), ( h-2 = (Õ) 0

and

6&#x3E;1 = (dT, 6)-

A cochain

complex

is defined

by

and

We introduce a sequence

of linear operators defined

by

(8)

LEMMA 4.1. The

diagram

is commutative.

PROOF.

is

obviously

true.

Hence,

From

and

it follows that

Hence,

From

and

for q &#x3E; 0 it follows that

Hence,

(9)

Let a sequence

of linear operators be defined

by

LEMMA 4.2. The

diagram

is commutative.

PROOF.

is

obviously

satisfied. Hence, From

-

and

it follows that

Hence,

From

and

for

q &#x3E;

0 it follows that

(10)

Hence,

LEMMA 4.3.

PROOF. The first two

equalities

are obvious. For

q &#x3E;

0 we have

1.

For q &#x3E; 0 we define linear

operators

LEMMA 4.4.

and

PROOF. The first two

equalities

are obvious. For

q &#x3E;

0 we have

(11)

PROOF OF THEOREM 3.1. It follows from Lemma 4.1 and Lemma 4.2 that sequences

and

define cochain

morphisms /c

and A between the

Lagrange complex

and the

complex

These

morphisms

induce linear

mappings Sq(M)

and

Lq(M)

between the

Lagrange cohomology

spaces

L q (M)

Ker

8q 11m bq-’

I and the

cohomology

spaces

Sq(M)

=

Ker

bq/Im

bq-1 for

q &#x3E;

-1. Lemma 4.3 and Lemma 4.4

imply

that the

mappings rq

and

Aq

are

isomorphisms. Lagrange cohomology

spaces

Lq(M)

are thus

canonically isomorphic

to the

cohomology

spaces

Sq (M),

and each

space

Sq(M)

is in turn

isomorphic

to

Q.E.D.

REFERENCES

[1]

LM. ANDERSON - T. DUCHAMP, On the existence of global variational principles,

Amer. J. Math., 102 (1980), pp. 781-868.

[2]

C. EHRESMANN, Les prolongements d’ une variété différentiable, C.R. Acad. Sci. Paris, 233

(1951),

pp. 598-600.

[3]

A. FRÖLICHER - A. NIJENHUIS, Theory of vector valued differential forms, Nederl.

Akad. Wetensch. Proc. Ser. A., 59 (1956), pp. 338-359.

[4]

G. PIDELLO - W.M. TULCZYJEW, Derivations of differential forms on jet bundles, (to appear).

[5]

F. TAKENS, A global version of the inverse problem of the calculus of variations, J.

Differential Geometry, 14 (1979), pp.

543-562.

[6]

W.M. TULCZYJEW, Sur la différentielle de Lagrange, C.R. Acad. Sci. Paris Sér. A., 280 (1975), pp. 1295-1298.

(12)

[7]

W.M. TULCZYJEW, The Lagrange differential, Bull. Acad. Polon. Sci., 24 (1976).

[8]

W.M. TULCZYJEW, The Lagrange complex, Bull. Soc. Math. France, 105 (1977), pp.

419-431.

[9]

A.M. VINOGRADOV, A spectral sequence associated with a nonlinear differential equation, and algebro-geometric foundation of Lagrangian field theory with constraints, Soviet Math. Dokl., 19 (1978), pp. 144-148.

Department of Mathematics The University of Calgary

Calgary, Alberta T2N IN4, Canada

Références

Documents relatifs

The result is proved in the setting of Banach manifolds, and is applied to study representations on cohomology groups induced by a holomorphic action of a complex reductive Lie group

For a compact subset K of a complex manifold f^, a topological linear space F^(K) is defined by the inductive limit of locally convex spaces (see [K]).. F^(K) =

(iv) The map Ds gives another construction of the Poincare-Cartan form e for a class of Lagrangians in the multivariate higher order calculus of variations.. Section

There, it is proven that a cohomology theory on smooth manifolds is naturally isomorphic to ordinary integral cohomology if it satisfies the homotopy axiom, the Mayer-Vietoris

It is thus strict exact, and from this it easily follows that H^M) -^ H^M&#34;) is strict and surjective. Since M is strict, H^M) is separated and finite-dimensional, so the same

Since the above result follows from (1.3) and (1.10) if ^ is affine, we deduce the general case from the Cech spectral sequence as above.. ANNALES SCIENTIFIQUES DE I/ECOLE

In [13] the Mostow condition was studied for simply connected almost Abelian Lie groups and the first Betti number of a compact quotient of a simply connected almost Abelian Lie

Sheaves of germs of holomorphic differential forms on a complex analytic space.. In the following we shall consider analytic sets rather than