Dirac's Gamma Matrices: What Are They & Do They Have Many Forms?

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SUMMARY

Dirac's gamma matrices are fundamental in quantum mechanics, particularly in the formulation of the Dirac equation. They can be represented in various forms, notably the Weyl (or chiral) basis and the Dirac basis. The Weyl basis is optimal for analyzing relativistic particles, while the Dirac basis is preferred for non-relativistic scenarios. Understanding these representations is crucial for applications in high energy physics and quantum field theory.

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pallab
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what are Dirac's gamma matrices
\{\gamma ^{0},\gamma ^{1},\gamma ^{2},\gamma ^{3}\}
. especially ,
\gamma ^{0}
does it have many forms?
 
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pallab said:
what are Dirac's gamma matrices
\{\gamma ^{0},\gamma ^{1},\gamma ^{2},\gamma ^{3}\}
. especially ,
\gamma ^{0}
does it have many forms?

There are some different ways to define them. The Dirac equation, in which a matrix with differential operators as its entries is acting on the spinor field, looks a bit different depending on the representation (assuming you write it explicitly in matrix-spinor form).
 
Michael Price said:
Of the choices, I find the Weyl or chiral basis the best one to use..

Generally speaking, the Weyl basis (in which ##\gamma^5## is diagonal) is most useful for studying relativistic particles, such as in high energy physics experiments, while the Dirac basis (in which ##\gamma^0## is diagonal) is most useful for studying non-relativistic particles. (Here "relativistic" and "non-relativistic" is relative to the lab frame in which the measuring equipment is assumed to be at rest.)
 
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