Commutator of Dirac gamma matrices Quick question...For some reason I'm having trouble finding an identity or discussion for the commutator of the gamma matrices at the moment...i.e $$\gamma^u\gamma^v-\gamma^v \gamma^u$$ but I am not finding this anywhere. I have an idea of what it may be, but then again I'm not always right.  Can anyone fill me in here fill me in? (I already know the anticommutator, i.e $$\gamma^u\gamma^v+\gamma^v\gamma^u=2g^{uv}I.)$$
 A: The OP wrote in a comment on the commutators of gamma-matrices: "to clarify a discussion of what it represents would be useful. I read its related to the Lie Algebra somewhere but as to further details (as in details beyond being a commutator)... not finding them."
In some sense, the Dirac gamma matrices can be identified with mutually orthogonal unit vectors (orts) of the Cartesian basis in 3+1 spacetime, with their anticommutators corresponding to scalar products of the orts (this approach is used, e.g., in the book "The Theory of Spinors" by Cartan, the discoverer of spinors). Then the non-vanishing commutators of gamma-matrices (say, in the form $\sigma^{\mu\nu}=\frac{1}{2}[\gamma^\mu,\gamma^\nu]$) can be identified with the so called bivectors (2-dimensional planes in the spacetime spanned by two orts).
@TheDarkSide asked if the commutator is useful anywhere. Some uses are mentioned in other answers, but let me tell you how it was useful for me. Some time ago, I showed that the Dirac equation (which is a system of four first-order equations for four components of the Dirac spinor) is generally equivalent to just one fourth-order equation for one component of the Dirac spinor (http://akhmeteli.org/wp-content/uploads/2011/08/JMAPAQ528082303_1.pdf, published in the Journal of Mathematical Physics). Recently, I derived a relativistically covariant form of the equation ((https://arxiv.org/abs/1502.02351 , eq. (27)), where the following linear combination of the commutators of gamma-matrices is heavily used: $F=\frac{1}{2}F_{\mu\nu}\sigma^{\mu\nu}$, where $F_{\mu\nu}$ is the electromagnetic field. 
A: Although the Clifford algebra $\{\gamma^\mu,\gamma^\nu\}$ is the most famous, there is an expression for the commutator:
$$[\gamma^\mu,\gamma^\nu] = 2\gamma^\mu \gamma^\nu - 2 \eta^{\mu\nu}$$
The matrix defined by $[\gamma^\mu,\gamma^\nu]$ actually has a purpose: it forms a representation of the Lorentz algebra. If we define $S^{\mu\nu}$ as $1/4$ the commutator, then we have,
$$[S^{\mu\nu},S^{\rho\sigma}] = \eta^{\nu\rho}S^{\mu\sigma} - \eta^{\mu\rho}S^{\nu\sigma} + \eta^{\mu\sigma}S^{\nu\rho} - \eta^{\nu\sigma}S^{\mu\rho}= \eta^{\rho[\nu}S^{\mu]\sigma} + \eta^{\sigma [\mu}S^{\nu]\rho}$$
which is the Lorentz algebra. One can verify this by simply using the first commutator, and the rule for the commutator involving a product.

There is a particularly important use for the commutator, namely defining $\sigma^{\mu\nu} = \frac{i}{2} [\gamma^\mu,\gamma^\nu]$, the action of a spin-$\frac32$ particle is given by,
$$\mathcal L = -\frac{1}{2}\bar{\psi}_\mu \left( \varepsilon^{\mu\lambda \sigma \nu} \gamma_5 \gamma_\lambda \partial_\sigma -im\sigma^{\mu\nu}\right)\psi_v,$$
which can be used to describe the superpartner to the graviton, namely the gravitino, thus making it necessary for supergravity theories.
A: The above answers are good, yet I'm suprised that no one has mentioned that the commutator of the Dirac matrices is required in the description of ANY fermion in a general non-flat space. In such a space the Dirac equation reads (utilizing the tetrad formulation): 
$$\left(i\gamma^{a}e_{a}^{\mu}D_{\mu}-m\right)\psi=0$$
Where:
$$D_{\mu}=\partial_{\mu}-\frac{i}{4}\omega_{\mu}^{ab}\sigma_{ab}$$
where $\omega$ is the so-called spin connection and $\sigma$ is defined as in JamalS's answer above. If you want to do quantum mechanics with fermions in curved spacetime, you will certainly need to utilize the commutator of Dirac matrices.
A: Ok,
$\gamma^u\gamma^v=-\gamma^v\gamma^u$ for $u\neq v$  
Therfore $\gamma^u\gamma^v-\gamma^v\gamma^u=2\gamma^u\gamma ^v$ for $u \neq v$  
