Advances in Pure Mathematics
Vol.05 No.13(2015), Article ID:60941,10 pages
10.4236/apm.2015.513069
Poisson Vector Fields on Weil Bundles
Norbert Mahoungou Moukala1, Basile Guy Richard Bossoto1,2
1Faculty of Sciences and Technology, Marien NGOUABI University, Brazzaville, Congo
2Institut de Recherche en Sciences Exactes et Naturelles (IRSEN), Brazzaville, Congo

Copyright © 2015 by authors and Scientific Research Publishing Inc.
This work is licensed under the Creative Commons Attribution International License (CC BY).
http://creativecommons.org/licenses/by/4.0/


Received 2 October 2015; accepted 6 November 2015; published 9 November 2015
ABSTRACT
In this paper, M is a smooth manifold of finite dimension n, A is a local algebra and MA is the associated Weil bundle. We study Poisson vector fields on MA and we prove that all globally hamiltonian vector fields on MA are Poisson vector fields.
Keywords:
Weil Algebra, Weil Bundle, Poisson Manifold, Lie Derivative, Poisson 2-Form

1. Introduction
A Weil algebra or local algebra (in the sense of André Weil) [1] , is a finite dimensional, associative, commutative and unitary algebra A over
in which there exists a unique maximum ideal
of codimension 1. In his case, the factor space
is one-dimensional and is identified with the algebra of real numbers
. Thus
and
is identified with
, where
is the unit of A.
In what follows we denote by A a Weil algebra, M a smooth manifold,
the algebra of smooth functions on M.
A near point of
of kind A is a homomorphism of algebras

such that for any
,
.
We denote by
the set of near points of x of kind A and
the set of near points on M of
kind A. The set 

If 
is differentiable of class 


is an injective homomorphism of algebras. Then, we have:
We denote


such that
Thus [4] ,
If
is a vector field on M, then there exists one and only one A-linear derivation
called prolongation of the vector field 
Let 


the canonical derivation which the image of 



with 

We denote






The map
is a derivation and there exists a unique A-linear derivation
such that
for any 
is an injective homomorphism of 


there exists a unique 
such that
In other words, there exists a unique 
This fact implies the existence of a natural isomorphism of 
In particular, if
For any




the exterior 


If 


the 

with
Let
be the 
for any 
is a unique 

is a unique 
We denote
the unique 
i.e. 
of degree −1 [9] .
We recall that a Poisson structure on a smooth manifold M is due to the existence of a bracket 



is a derivation of commutative algebra i.e.
for

The manifold M is a Poisson manifold if and only if there exists a skew-symmetric 2-form
such that for any f and g in
defines a structure of Lie algebra over 



2. Poisson 2-Form on Weil Bundles
When 
such that 

such that
Let
be a unique 
Let us consider the canonical isomorphism
and let
be the map.
Proposition 1. [9] If 
such that for any
is a skew-symmetric 2-form on 
for any x and y in

Theorem 2. [9] The manifold 
such that for any 


defines a structure of A-Lie algebra over

In this case, we will say that 



3. Poisson Vector Field on Weil Bundles
Proposition 3. For any 

Proof. If


3.1. Lie Derivative
The Lie derivative with respect to 
Proposition 4. For any
is a unique A-linear derivation such that
for any
Proof. For any
A vector field 




on a A-Poisson manifold of Poisson 2-form 

Proposition 5. If 
is a Poisson vector field if and only if
is a Poisson vector field.
Proof. indeed, for any
Thus, 

Proposition 6. Let 
Proof. Let X be a globally hamiltonian vector field, then there exists 




Thus, all globally hamiltonian vector fields are Poisson vector fields.
When 






where
denotes the operator of cohomology associated with the representation
When 

Therefore, all globally hamiltonian vector fields are Poisson vector fields.
Proposition 7. For any 
Proof.
Thus,
3.2. Example
When 







Thus,
Therefore, (

For

As [13]
we have
As
and
As,
Thus,
where

When 
Thus,
where 


As
we have
Cite this paper
Norbert Mahoungou Moukala,Basile Guy Richard Bossoto, (2015) Poisson Vector Fields on Weil Bundles. Advances in Pure Mathematics,05,757-766. doi: 10.4236/apm.2015.513069
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