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 is a smooth manifold of dimension and called manifold of infinitely near points on M of kind A [1] - [3] , or simply the Weil bundle [4] [5] .
If is a smooth function, then the map
is differentiable of class [4] [6] . The set, of smooth functions on with values on A, is a commutative algebra over A with unit and the map
is an injective homomorphism of algebras. Then, we have:
We denote, the set of vector fields on and the set of A-linear maps
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 [4] [6] , such that
Let be the -module of Kälher differentials of and
the canonical derivation which the image of generates the -module i.e. for ,
with for any [7] et [8] .
We denote, the -module of Kälher differentials of which are A-linear. In this case, for, we denote, the class of in.
The map
is a derivation and there exists a unique A-linear derivation
such that
for any [9] . Moreover the map
is an injective homomorphism of -modules. Thus, the pair satisfies the following universal property: for every -module E and every A-derivation
there exists a unique -linear map
such that
In other words, there exists a unique which makes the following diagram commutative
This fact implies the existence of a natural isomorphism of -modules
In particular, if, we have
For any, denotes the - module of skew-symmetric multilinear forms of degree p from into and
the exterior -algebra of called algebra of Kähler forms on.
If then η is of the form with. Thus,
the -module is generated by elements of the form
with.
Let
be the -skew-symmetric multilinear map such that
for any and, where
is a unique -linear map such that [8] . Then,
is a unique -skew-symmetric multilinear map such that
We denote
the unique -skew-symmetric multilinear map such that
i.e. induces a derivation
of degree −1 [9] .
We recall that a Poisson structure on a smooth manifold M is due to the existence of a bracket on such that the pair is a real Lie algebra such that, for any the map
is a derivation of commutative algebra i.e.
for. In this case we say that is a Poisson algebra and M is a Poisson manifold [10] [11] .
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 [8] . In this case, we say that is the Poisson 2-form of the Poisson manifold M and we denote the Poisson manifold of Poisson 2-form.
2. Poisson 2-Form on Weil Bundles
When is a Poisson manifold, the map
such that for any, is a derivation. Thus, there exists a derivation
such that
Let
be a unique -linear map such that
Let us consider the canonical isomorphism
and let
be the map.
Proposition 1. [9] If is a Poisson manifold, then the map,
such that for any
is a skew-symmetric 2-form on such that
for any x and y in. Moreover, is a Poisson manifold.
Theorem 2. [9] The manifold is a Poisson manifold if and only if there exists a skew-symmetric 2-form
such that for any and in,
defines a structure of A-Lie algebra over. Moreover, for any f and g in,
In this case, we will say that is the Poisson 2-form of the A-Poisson manifold and we denote the A-Poisson manifold of Poisson 2-form [9] .
3. Poisson Vector Field on Weil Bundles
Proposition 3. For any and for any, we have
Proof. If, then there exists, such that . Thus,
3.1. Lie Derivative
The Lie derivative with respect to is the derivation of degree 0
Proposition 4. For any, lthe map
is a unique A-linear derivation such that
for any.
Proof. For any, we have
A vector field on a Poisson manifold is called Poisson vector field if the Lie derivative of with respect to vanishes i.e.. A vector field
on a A-Poisson manifold of Poisson 2-form will be said Poisson vector field if.
Proposition 5. If is a Poisson manifold, then a vector field
is a Poisson vector field if and only if
is a Poisson vector field.
Proof. indeed, for any,
Thus, if and only if.
Proposition 6. Let be a A-Poisson manifold. Then, all globally hamiltonian vector fields are Poisson vector fields.
Proof. Let X be a globally hamiltonian vector field, then there exists such that i.e. X is the interior derivation of the Poisson A-algebra [6] . For any and,
Thus, all globally hamiltonian vector fields are Poisson vector fields.
When is a symplectic manifold, then is a symplectic A-manifold [6] [12] . For
, we denote the unique vector field on, considered as a derivation of into, such that
where
denotes the operator of cohomology associated with the representation
When is a symplectic A-manifold, then for any,
Therefore, all globally hamiltonian vector fields are Poisson vector fields.
Proposition 7. For any and for any Poisson vector field Y, we have
Proof.
Thus,
3.2. Example
When is a Liouville form, where is a local system of coordinates in the cotangent bundle of M, then (,) is a symplectic manifold on [7] . Let be the unique differential A-form of degree −1 on such that
Thus,
Therefore, (,) is a symplectic A-manifold.
For, let be the globally hamiltonian vector field
As [13]
we have
As
and
As,
Thus,
where. An integral curve of is a solution the following system of ordinary equation
When is a local system of coordinates corresponding at a chart U of M,
Thus,
where for. For,
As
we have