Notation relating to gamma matrices

In summary, the conversation discusses the notation for gamma matrices and the meaning of the notation on the right hand side. It is explained that the notation is a commutator and involves adding every possible permutation with the appropriate sign and possible division by a factor. The sign of a permutation is determined by whether it is a cyclic or anticyclic permutation, with the former being positive and the latter being negative. For more than three indices, the sign is determined by counting the number of pairwise interchanges needed to bring the indices back to numerical order.
  • #1
vertices
62
0
Hi

My QFT course assumes the following notation for gamma matrices:

[tex]\gamma ^{\mu_1 \mu_2 \mu_3 \mu_4} = {\gamma ^ {[\mu_1}}{\gamma ^ {\mu_2}}{\gamma ^ {\mu_3}}{\gamma ^ {\mu_4 ]}}[/tex]

what does the thing on the right hand side actually mean? Its seems to be a commutator of some sort.
 
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  • #2
Hi vertices! :smile:

(have a gamma: γ and a mu: µ :wink:)

It means you add every possible permutation (just as in γµ[1µ2] you'd add every possible permutation, but there'd only be two of them! :wink:).
 
  • #3
tiny-tim said:
Hi vertices! :smile:

(have a gamma: γ and a mu: µ :wink:)

It means you add every possible permutation (just as in γµ[1µ2] you'd add every possible permutation, but there'd only be two of them! :wink:).


Thanks tiny-tim:)

So for example, would I be right in saying that:

γµ1µ2µ1γµ2µ2γµ1?
 
  • #4
Tiny-Tim forgot to tell you that you also must multiply each term by the sign of its permutation. That is, you must take a totally-antisymmetrized sum. You might also have to divide by N afterward, depending on the convention you're using (where N is the number of gamma matrices being antisymmetrized).
 
  • #5
vertices said:
Thanks tiny-tim:)

So for example, would I be right in saying that:

γµ1µ2µ1γµ2µ2γµ1?

Actually, the usual definition for the square bracket, like [tex]\gamma^{\mu\nu} \equiv \gamma^{[\mu} \gamma^{\nu]} [/tex] is the anti-symmetrization of the indices. For this case I just mentioned,
[tex] \gamma^{\mu\nu} = \gamma^\mu\gamma^\nu - \gamma^\nu\gamma^\mu [/tex]
And for example,
[tex]\gamma^{\mu\nu\rho}
\equiv \gamma^{[\mu}\gamma^{\nu}\gamma^{\rho]}
= \frac{1}{3!}\left( \gamma^\mu\gamma^\nu\gamma^\rho - \gamma^\mu\gamma^\rho\gamma^\nu + \gamma^\nu\gamma^\rho\gamma^\mu -\gamma^\nu\gamma^\mu\gamma^\rho +\gamma^\rho\gamma^\mu\gamma^\nu -\gamma^\rho\gamma^\nu\gamma^\mu \right)
[/tex]
 
  • #6
Ben Niehoff said:
Tiny-Tim forgot to tell you that you also must multiply each term by the sign of its permutation. That is, you must take a totally-antisymmetrized sum. You might also have to divide by N afterward, depending on the convention you're using (where N is the number of gamma matrices being antisymmetrized).

sorry can I ask a stupid question: what is the 'sign' of a permutation?
 
  • #7
ismaili said:
Actually, the usual definition for the square bracket, like [tex]\gamma^{\mu\nu} \equiv \gamma^{[\mu} \gamma^{\nu]} [/tex] is the anti-symmetrization of the indices. For this case I just mentioned,
[tex] \gamma^{\mu\nu} = \gamma^\mu\gamma^\nu - \gamma^\nu\gamma^\mu [/tex]
And for example,
[tex]\gamma^{\mu\nu\rho}
\equiv \gamma^{[\mu}\gamma^{\nu}\gamma^{\rho]}
= \frac{1}{3!}\left( \gamma^\mu\gamma^\nu\gamma^\rho - \gamma^\mu\gamma^\rho\gamma^\nu + \gamma^\nu\gamma^\rho\gamma^\mu -\gamma^\nu\gamma^\mu\gamma^\rho +\gamma^\rho\gamma^\mu\gamma^\nu -\gamma^\rho\gamma^\nu\gamma^\mu \right)
[/tex]

can i ask you how the the sign of each term is determined? How do you decide which term is positive and which term is negative?

thanks.
 
  • #8
Aahh I've figured it out i think - cyclic permutations are positive; anticyclic permutations are negative. A bit like the levi-civita thingy..
 
  • #9
vertices said:
Aahh I've figured it out i think - cyclic permutations are positive; anticyclic permutations are negative. A bit like the levi-civita thingy..

This works for 3 indices or less. For N indices, you check whether it is an even or odd permutation of {1,2,3,4,...,N}. That is, you count the number of pairwise interchanges required to bring the indices back to numerical order. If it takes an even number of switches, the term gets a plus sign; otherwise, a minus sign.
 
  • #10
Ben Niehoff said:
This works for 3 indices or less. For N indices, you check whether it is an even or odd permutation of {1,2,3,4,...,N}. That is, you count the number of pairwise interchanges required to bring the indices back to numerical order. If it takes an even number of switches, the term gets a plus sign; otherwise, a minus sign.

interesting. thanks for pointing this out Ben.
 

FAQ: Notation relating to gamma matrices

What are gamma matrices?

Gamma matrices are a set of mathematical objects used in quantum field theory to represent the Dirac spinor wave function, which describes the behavior of spin-1/2 particles such as electrons and quarks. They are essentially matrices containing the Pauli matrices and the identity matrix.

Why are gamma matrices important in physics?

Gamma matrices are important because they allow us to describe the behavior of fundamental particles in a consistent and mathematically elegant way. They are used in many areas of theoretical physics, including quantum mechanics, quantum field theory, and particle physics.

How are gamma matrices used to represent spin?

Gamma matrices are used to represent spin by assigning a different gamma matrix to each of the three spatial dimensions and the time dimension. These matrices then act on the spinor wave function to give information about the particle's spin and its interaction with other particles.

What is the notation used for gamma matrices?

The notation used for gamma matrices varies depending on the context, but it often involves Greek letters such as gamma (γ) and epsilon (ε). In addition, the gamma matrices are often denoted by the symbol Γ with a subscript indicating which direction it corresponds to.

Can gamma matrices be used to describe particles with spin other than 1/2?

Yes, gamma matrices can be used to describe particles with spin other than 1/2. In fact, in higher dimensions (greater than 4), the gamma matrices can be used to describe particles with a wide range of spins, including 1, 3/2, 2, and so on.

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