In the study of Dirac fields in quantum field theory, Richard Feynman introduced the convenient Feynman slash notation (less commonly known as the Dirac slash notation). If A is a covariant vector (i.e., a 1-form),

where γ are the gamma matrices. Using the Einstein summation notation, the expression is simply

Using the anticommutators of the gamma matrices, one can show that for any ${\displaystyle a_{\mu }}$ and ${\displaystyle b_{\mu }}$,

where ${\displaystyle I_{4}}$ is the identity matrix in four dimensions.

In particular,

Further identities can be read off directly from the gamma matrix identities by replacing the metric tensor with inner products. For example,

where:

This section uses the (+ − − −) metric signature. Often, when using the Dirac equation and solving for cross sections, one finds the slash notation used on four-momentum: using the Dirac basis for the gamma matrices,