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SOME RESULTS FOR GENERALIZED COCHAINS

Dorin Wainberg

Abstract. In the first part of the paper a generalized p-cochain on C∞

(M) is defined, followed in the second part by some of its properties and applications in distributional symplectic geometry.

2000 Mathematics Subject Classification: 70E50.

1. Introduction

LetM be a smooth 2n-dimmensional manifold andωa symplectic structure onM. We denote byC∞

(M) (resp. X′

(M), resp. p D′

(M)) the space of smooth (C∞

) functions (resp. the spaced of generalized vector fields, resp. the space of p-De Rham currents) on M endowed with the uniform convergence topology. We remind that in local chart a generalized vector field (resp. anp-De Rham current) is a smooth vector field (resp. a smooth p-form) with distributions coefficients instead of smooth ones.

Definition 1.1. A generalized p-cochain on C∞

(M) is an alternating p-linear map

m:C∞

(M)×...×C∞

(M)−→ 0

D′

(M). We shall denote by

p C′

(C∞

) the space of generalizedp-cochains onC∞

(M). Examples. 1) Each generalized vector field X ∈ X′

(M) defines in a natural way a generalized 1-cochain.

2) The map ℑ defined by K :

p D′

(M)−→K(T)∈

p C′

(C∞

), K(T)(f1, ..., fp)

def

(2)

is a generalized 1-cochain.

3) There exists a linear map K from the space of De Rham currents into the space of generalized cochains, namely:

K : p D′

(M)−→K(T)∈

p C′

(C∞

), K(T)(f1, ..., fp)

def

= T(ξf1, ..., ξfp)

for any f1, ..., fp ∈C∞(M) and whereξfi is the Hamiltonian vector field

asso-ciated to fi (i.e. Lξfiω+dfi).

The coboundary of generalized p-cochains is defined as usual; in the par-ticular case of a generalized 1-cochain we have:

∂m(f1, f2) =Lξfim(f2)−Lξf2m(f1)−m{f1, f2}.

2. Some properties of generalized cochains

Some properties for generalized cochains are given in the following state-ments:

Proposition 2.1. i)K is an injective map.

ii)IfT =Tω is the form like2-current defind by the symplectic formω (i.e. Tω : ϕ ∈ 2n

−2

D (M)−→< Tω, ϕ >= R

M

ω∧ϕ, where p

D(M) denotes the space of p-forms with compact support on M), then

K(Tω) =−∂ℑ.

iii) For each α∈R, S ∈D1′

(M) we have

K(αTω+dS) = −∂(αℑ+K(S)).

The proof can be obtained immediately using the definitions of K and ℑ. Proposition 2.2. i)If ω˜ is the canonical isomorphism given by

˜

ω :X ∈X′

(M)−→ω(X)˜ def= X y ω∈

1

D′

(3)

then

K

1

D′

(M) =−ω˜−1

.

ii) Let X be a generalized vector field on M. Then for each f, g ∈C∞

(M) we have:

X(f, g) =−LXω(ξf, ξg).

iii) X ∈ X′

(M) is a generalized 1-cocycle (i.e. ∂X = 0) if and only if X ∈X′

loc(M) (i.e. LXω = 0). iv) X ∈X′

(M) is a generalized 1-coboundary if and only if X ∈X′

glob(M) (i.e. X y ω+dH = 0).

Proof. i) Since the space D1′

(M) can be identified with {X y ω | X ∈ X′

(M)}, for anyf ∈C∞

(M), we get successively:

Kω(X)(f˜ ) = ˜ω(X)(ξf) = (X y ω)(ξf) =−X(f). so

K◦ω˜ =−IdX′(M),

or equivalent:

K =−ω˜−1

.

ii) For any f, g ∈C∞

(M) we can write: ∂X(f, g) =∂ω˜ω˜−1

(X)(f, g) =−dω(X)(ξf˜ , ξg) =−d(X y ω)(ξf, ξg) =−LXω(ξf, ξg).

Now the relation iii) and iv) can be derived immediately from ii) Definition 2.1. We say thatm∈C1′

(C∞

)is a locally generalizedp-cochain if, given an open set U ⊂M and p-functions f1, ..., fp with

f1|U =f2|U =...=fp|U, then

m(f1, ..., fp)|U = 0. Proposition 2.3. Let T ∈D2′

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i) K(T) is a locally generalized 2-cochain. ii) For any f, g ∈C∞

(M) the following equality holds: K(T)(f2, g) = 2f K(T)(f, g).

Proof. i) LetU be an open set in M and f ∈ C∞

(M) such that f|U = 0. Then for each g ∈C∞

(M) we have:

K(T)(f, g)|U =T(ξf, ξg)|U. Since

ξf = n

X

i=1

∂f ∂pi

∂ ∂qi −

∂f ∂qi

∂ ∂pi

,

and

T|U = n

X

i,j=1

(Tijdpidpj +Tijdqidqj+...),

it follows that:

T(ξf, ξg)|U = n

X

i,j=1

Tij∂f ∂qi

∂g ∂qj +Tij

∂f ∂pi

∂g ∂pj +...

.

Since each term involves a partial derivative of f, clearly T(ξf, ξg) vanishes onU, so K(T) is a locally generalized 2-cochain.

ii) For any f, g ∈C∞

(M) we can write successively: K(T)(f2, g) =T(ξf

2, ξg)

=T(2f ξf, ξg) = 2f T(ξf, ξg) = 2f K(T)(f, g).

Also, as for classical cochains we can prove the following result:

Remark 2.1 Let (M, ω) be a non-compact symplectic manifold and m ∈ 2

C′

(C∞

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References

[1] J. E. Marsden, Generalized Hamiltonian mechanics, Arch. Rational Mech. Anal., 28, pp 323-361, 1968.

[2] Phillip E. Parker, Distributional geometry, Journal of Mathematical Physics, Volume 20, pp. 1423-1426, 1979.

[3] M. Puta, Hamiltonian Mechanical Systems and Geometric Quantiniza-tion, Kluwer, 1993.

[4] M. Puta, Poisson integrators, Analele Universitatii Timisoara, 1993, 267-272

[5] C. J. Isham, Some Quantum Field Theory Aspects of the Superspace Quantization of General Relativity, Proc. of the Royal Soc. of London., Math-ematical and Physical Sciences, No. 1665 , pp. 209-232, 1976

[6] L.Hormander,Linear partial differential operators, Springer-Verlag, 1964 [7] H. Lewy, An example of an smooth linear partial equation without solu-tion, An. Math. (2) 66, 1957

Author: Dorin Wainberg

Department of Mathematics ”1 Decembrie 1918” University Alba Iulia

Romania

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