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Schouten-Nijenhuis bracket

Let $M$ be a smooth manifold of dimension $M$. Recall
\begin{align*}
\Om^p(M) &= \Ga(\La^p T^*M)\text{ differential $p$-forms, }p\geq ...
...{\bullet}(M) &= \bigoplus_{p}\gX^p(M) \text{ graded vector spaces.}
\end{align*}
External product gives both spaces a structure of graded, associative algebra, $\bZ_2$-commutative (supercommutative) i.e.

\begin{displaymath}
P\land Q=(-1)^{\deg Q \deg P}Q\land P.
\end{displaymath}

The natural duality pairing between $T_xM$ and $T_x^*M$ extends to a natural pairing between $\Om^{\bullet}(M)$ and $\gX^{\bullet}(M)$ as follows
\begin{align*}
\bracket{\al}{X}_x &:= \bracket{\underbrace{\al(x)}_{\in T_x^* M}...
...=X_1\wyw X_p,\\ & \al_i\in\Om^1(M),\; X_j\in \gX^1(M).
\end{cases}}
\end{align*}

\begin{remark}
$\bracket{\om}{P}(x)$\ depends only on $\om(x)$,
$P(x)$. Locally ...
... above defines a $\Coo(M)$-bilinear
pairing on the whole space $M$.
\end{remark}
Inner product for $P\in\gX^{\bullet}(M)$, $\om\in\Om^{\bullet}(M)$:

\begin{displaymath}
\bracket{i_P\om}{Q}=\bracket{\om}{P\land Q}\quad \forall\;
Q\in\gX^{\bullet}(M).
\end{displaymath}

It is the left transpose of external product.

$\gX^1(M)$ is a Lie algebra with bracket $[X, Y]=XY-YX$ of vector fields. Let $\gerg$ be a Lie algebra over $\bK$.
\begin{prop}
There is a unique bracket on $\La^{\bullet}\gerg$\ which extends th...
...{\bullet}$\ with an element in
$\La^0\gerg=\bK$\ is 0.
\end{enumerate}\end{prop}
Remark: It is not correct to say that $\La^{\bullet }\gerg$ is a graded Lie algebra. In fact in a graded Lie algebra the 0-component should be a Lie subalgebra, therefore the 0-component should be $\gerg$. $\La^{\bullet + 1}\gerg$ is a graded Lie algebra.
\begin{proof}
Start from 2 to prove a formula for
\begin{displaymath}[A, B_1\wyw...
... by
$\bK$-linearity to sum of decomposables. Verify Jacobi identity.
\end{proof}

\begin{prop}
Let $M$\ be a manifold. Then there exists a unique $\bR$-bilinear
b...
...P]] + (-1)^{(r-1)(q-1)}[R, [P, Q]]=0.
\end{displaymath}\end{enumerate}\end{prop}

\begin{proof}
% latex2html id marker 2085The first step is to proof that such ...
...result. Other properties are
proved by direct (lengthy) computation.
\end{proof}

\begin{defn}
A \textbf{Gerstenhaber algebra} is a triple $(\gA, \land, [-,-])$\ ...
...t a\vert-1)\vert b\vert}b\land [a,c].
\end{displaymath}\end{enumerate}\end{defn}

\begin{examples}
% latex2html id marker 2109\mbox{}
\begin{itemize}
\item Mult...
...infty}$-algebra structures and Kontsevich formality.
\end{itemize}\end{examples}
Let $(\gA, \land, [-,-])$ be a Gerstenhaber algebra. An operator $D\:
\gA^{\bullet}\to \gA^{\bullet -1}$ is said to generate the Gerstenhaber algebra if for all $a\in\gA^i$, $b\in \gA$

\begin{displaymath}[a, b]=(-1)^i(D(a\land b)- Da\land b- (-1)^ia\land Db).
\end{displaymath}

If $D^2=0$ we say that our Gerstenhaber algebra is exact or Batalin-Vilkovisky algebra.

We will show that the Gerstenhaber algebra of differential forms on a Poisson manifold is a Batalin-Vilkovisky algebra. Its generating operator will be called Poisson (or canonical or Brylinski) differential.



Subsections
next up previous contents
Next: Schouten-Nijenhuis bracket computations Up: Schouten-Nijenhuis bracket Previous: Lie-Poisson bracket   Contents
Pawel Witkowski 2006-06-26