- #1
sunkesheng said:thanks ,i found it in weinberge`s book vol.1
ansgar said:cool, the image you posted is from Peskin right?
The symbols \gamma{\mu} and \gamma{\nu} represent the gamma matrices in the Dirac equation, which is a fundamental equation in quantum field theory. In Rows 1,2,3, they represent the first, second, and third components of a four-component spinor, respectively.
The gamma matrices \gamma{\mu} and \gamma{\nu} are related through the Clifford algebra, which describes the algebraic properties of these matrices. Specifically, they satisfy the anticommutation relation \{\gamma{\mu}, \gamma{\nu}\} = 2\eta_{\mu\nu}, where \eta_{\mu\nu} is the Minkowski metric.
The gamma matrices \gamma{\mu} and \gamma{\nu} have a physical interpretation as representing the spin of a particle. In quantum field theory, particles are described as excitations of fields, and the spin is a quantum number that characterizes the behavior of these excitations.
The gamma matrices \gamma{\mu} and \gamma{\nu} act on a spinor by multiplying it from the left. For example, \gamma^{\mu}\psi is the result of applying the gamma matrix \gamma^{\mu} to the spinor \psi. This action is important in the Dirac equation, where the gamma matrices act on the spinor field to describe the dynamics of particles.
The gamma matrices \gamma{\mu} and \gamma{\nu} are closely related to Lorentz transformations, which are transformations that preserve the form of the laws of physics in different inertial frames. In particular, the gamma matrices can be used to construct the generators of Lorentz transformations, which are used to generate the rotation and boost transformations in special relativity.