<?xml version="1.0" encoding="UTF-8"?>

<record version="13" id="7509">
 <title>Lie superalgebra</title>
 <name>LieSuperalgebra3</name>
 <created>2005-11-30 18:48:42</created>
 <modified>2009-02-01 14:06:06</modified>
 <type>Definition</type>
 <creator id="20947" name="bci1"/>
 <author id="20947" name="bci1"/>
 <author id="11774" name="plinko"/>
 <classification>
	<category scheme="msc" code="17B01"/>
	<category scheme="msc" code="81Q60"/>
	<category scheme="msc" code="17B60"/>
	<category scheme="msc" code="81R50"/>
 </classification>
 <defines>
	<concept>vector superspace</concept>
	<concept>Lie superbracket</concept>
	<concept>supercommutator bracket</concept>
 </defines>
 <synonyms>
	<synonym concept="Lie superalgebra" alias="Lie super algebra"/>
	<synonym concept="Lie superalgebra" alias="graded Lie algebra"/>
 </synonyms>
 <related>
	<object name="CartanCalculus"/>
	<object name="Superalgebra"/>
	<object name="GradedAlgebra"/>
	<object name="LieAlgebroids"/>
	<object name="SuperfieldsSuperspace"/>
	<object name="SupersymmetryOrSupersymmetries"/>
	<object name="LieAlgebroids"/>
	<object name="JordanBanachAndJordanLieAlgebras"/>
	<object name="LieAlgebra"/>
	<object name="LieAlgebraCohomology"/>
	<object name="SuperAlgebra"/>
	<object name="CartanCalculus"/>
	<object name="QuantumGravityTheories"/>
	<object name="FunctionalBiology"/>
 </related>
 <keywords>
	<term>supergeometry</term>
	<term>supersymmetry</term>
 </keywords>
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\newcommand{\lie}{\mathcal{L}}</preamble>
 <content>\begin{dfn}
  A \emph{Lie superalgebra} is a vector superspace equipped with a bilinear map
\begin{equation}
\begin{split}
[\cdot,\cdot]: V \otimes V &amp;\rightarrow V, \\
v \otimes w &amp;\mapsto [v, w],
\end{split}
\end{equation}
satisfying the following properties:
\begin{enumerate}
\item If $v$ and $w$ are homogeneous vectors, then $[v,w]$ is a homogeneous vector of degree $|v| + |w| \pmod 2$,
\item For any homogeneous vectors $v, w$, $[v,w] = (-1)^{|v||w| + 1} [w,v]$,
\item For any homogeneous vectors $u,v,w$, $(-1)^{|u||w|}[u, [v,w]] + (-1)^{|v||u|} [v, [w, u]] + (-1)^{|w||v|} [w,[u,v]]$ = 0.
\end{enumerate}
The map $[\cdot,\cdot]$ is called a \emph{Lie superbracket}.
\end{dfn}

\begin{ex}
A Lie algebra $V$ can be considered as a Lie superalgebra by setting $V = V_0$ and, therefore, $V_1 = \{0\}$.
\end{ex}

\begin{ex}
Any associative superalgebra $A$ has a Lie superalgebra structure where, for any homogeneous elements $a,b \in A$, the Lie superbracket is defined by the equation
\begin{equation}\label{supercomm}
[a, b] = ab - (-1)^{|a||b|}ba.
\end{equation}

 The Lie superbracket (\ref{supercomm}) is called the \emph{supercommutator bracket} on $A$.
\end{ex}



\begin{ex}
  The space of graded derivations of a supercommutative superalgebra, equipped with the supercommutator bracket, is a Lie superalgebra.
\end{ex}



\begin{dfn}
A \emph{vector superspace} is a vector space $V$ equipped with a decomposition $V = V_0 \oplus V_1$.  
\end{dfn}

Let $V = V_0 \oplus V_1$ be a vector superspace.  Then any element of $V_0$ is said to be \emph{even}, and any element of $V_1$ is said to be \emph{odd}.  By the definition of the direct sum, any element $v$ of $V$ can be uniquely written as $v = v_0 + v_1$, where $v_0 \in V_0$ and $v_1 \in V_1$.

\begin{dfn}
A vector $v \in V$ is \emph{homogeneous} of degree $i$ if $v \in V_i$ for $i = 0$ or $1$.
\end{dfn}

If $v \in V$ is homogeneous, then the degree of $v$ is denoted by $|v|$.  In other words, if $v \in V_i$, then $|v| = i$ by definition.

\begin{rmk}
The vector $0$ is homogeneous of both degree $0$ and $1$, and thus $|0|$ is not well-defined.
\end{rmk}

</content>
</record>
