Jacobi identity

This entry is about the identity in Lie theory. For another identity named after Jacobi, see at

Jacobi theta-functionandJacobi form.

**∞-Lie theory** (higher geometry)

The Jacobi identity is an important equational identity that holds in Lie algebras and is also of interest in other algebras. It can be generalised to higher algebras.

There is a non-additive non-abelian form of the Jacobi identity that occurs in considering certain examples in identities among relations in the presentation of certain groups. There it is also called the Hall-Witt identity.

Given a nonassociative algebra $\mathfrak{g}$ over a field or a ring $k$, whose bilinear product is denoted by bracket $[,]:\mathfrak{g}\otimes\mathfrak{g}\to\mathfrak{g}$, the **Jacobi identity** holds for a triple of elements $x,y,z \in \mathfrak{g}$ if

$[x,[y,z]] + [y,[z,x]] + [z,[x,y]] = 0
\,.$

The principal example is that of a Lie algebra: here the Jacobi identity by definition holds for all triples of elements (and the bracket is skew-symmetric).

If the bracket $[-,-]$ is skew-symmetric the Jacobi identity for all triples is equivalent to the **Leibniz identity** that for all $x,a,b$, the linear map $ad_x = [x,-] : \mathfrak{g} \to \mathfrak{g}$ is a derivation with respect to the Lie bracket:

$\left[x,\left[a,b\right]\right] = \left[\left[x,a\right],b\right] + \left[a,\left[x,b\right]\right]
\,.$

One can also consider right derivations (right Leibniz identity), what is again equivalent in the presence of antisymmetry:

$\left[\left[a,b\right],x\right] = \left[\left[a,x\right],b\right] + \left[a,\left[b,x\right]\right]
\,.$

Left and right Leibniz algebras generalize Lie algebras by having a left or right Leibniz identity, but not necessarily antisymmetry of the bracket. In particular, Jacobi identity, and left and right Leibniz identities do not need to coincide without antisymmetry.

A useful way to think of Jacobi identity for finite-dimensional Lie algebras, is dually in terms of the Chevalley-Eilenberg algebra $CE(\mathfrak{g})$ of the Lie algebra $\mathfrak{g}$ (see there for details). In terms of this dg-algebra $(\wedge^\bullet \mathfrak{g}^*, d_{\mathfrak{g}})$, the Lie bracket is encoded in the differential

$d_{\mathfrak{g}}|_{\mathfrak{g}^*} := [-,-]^* : \mathfrak{g}^* \to \mathfrak{g}^* \wedge \mathfrak{g}^*$

and the Jacobi identity is equivalent to the statement that this differential squares to $0$

$d \circ d = 0
\,.$

When Lie algebras are generalized to ∞-Lie algebras, the Jacobi identity in terms of the binary bracket is relaxed to hold only up to a natural isomorphism called the **jacobiator**, $[-,-,-] : \mathfrak{g}_0 \vee \mathfrak{g}_0 \vee \mathfrak{g}_0 \to \mathfrak{g}_1$,

$\left[x,\left[y,z\right]\right] + \left[y,\left[z,x\right]\right] + \left[z,\left[x,y\right]\right] =
\delta \left[x,y,z\right]
\,,$

where $\delta$ is the differential.

On the other hand, in terms of the Chevalley-Eilenberg algebra this is still encoded in just $d \circ d = 0$ (see there for details).

Last revised on July 31, 2018 at 09:55:51. See the history of this page for a list of all contributions to it.