Proof of traceless gamma matrices

In summary, the proof of the tracelessness of gamma matrices is found under the 'trace identities' section on Wikipedia, using the Clifford algebra relation and assuming that \mu \neq \nu. By anticommuting the matrices, it can be shown that Tr(\gamma^\nu) = 0.
  • #1
center o bass
560
2
Hi I'm trying to figure out the proof of why the gamma matrices are traceless. I found a proof at wikipedia under 'trace identities' here

http://en.wikipedia.org/wiki/Gamma_matrices

(it's the 0'th identity)
and from the clifford algebra relation

[tex] \{\gamma^\mu, \gamma^\nu\} = 2\eta^{\mu \nu}[/tex]

one get that

[tex] \frac{\gamma^\mu \gamma^\mu}{\eta^{\mu \mu}} = I[/tex]

thus

[tex] Tr(\gamma^\nu) = \frac{1}{\eta^{\mu \mu}} Tr(\gamma^\nu \gamma^\mu \gamma^\mu) = \frac{1}{\eta^{\mu \mu}} Tr(\{\gamma^\nu, \gamma^\mu\} \gamma^\mu - \gamma^\mu \gamma^\nu \gamma^\mu)[/tex]

and here it seems like they set

[tex]\frac{1}{\eta^{\mu \mu}} Tr(\{\gamma^\nu, \gamma^\mu\} \gamma^\mu) = \frac{1}{\eta^{\mu \mu}} Tr(2 \eta^{\nu \mu} \gamma^\mu ) = 0.[/tex]

But why is this true?
 
Last edited:
Physics news on Phys.org
  • #2
Ah it seems like it was assumed that [tex]\mu \neq \nu[/tex].
 
  • #3
If you assume $$\mu\neq \nu$$ then you have $$\gamma^{\nu}\gamma^{\mu}=-\gamma^{\mu}\gamma^{\nu}$$ and so you have (using the invariance of the trace under cyclic permutations of the matrices):

$$Tr(\gamma^{\nu})=\frac{1}{\eta^{\mu\mu}}Tr( \gamma^{\nu} \gamma^\mu \gamma^\mu)=\frac{1}{\eta^{\mu\mu}}Tr( \gamma^\mu \gamma^\nu \gamma^\mu)$$

You can now anticommutate and thus obtain:

$$-\frac{1}{\eta^{\mu\mu}}Tr(\gamma^\nu \gamma^\mu \gamma^\mu)=-Tr(\gamma^\nu) \Rightarrow Tr(\gamma^\nu)=-Tr(\gamma^\nu)=0$$
 

1. What are traceless gamma matrices?

Traceless gamma matrices are a set of mathematical objects used in physics and mathematics. They are a generalization of the concept of matrices, which are arrays of numbers used to represent linear transformations. In particular, traceless gamma matrices are used in quantum field theory to represent spinor fields.

2. How are traceless gamma matrices different from regular gamma matrices?

Regular gamma matrices are defined as 4x4 matrices with complex entries that satisfy a set of specific properties. Traceless gamma matrices, on the other hand, are a special subset of these matrices with the additional property that the sum of the diagonal elements is equal to zero. This property makes them useful in certain calculations and equations in quantum field theory.

3. What is the significance of traceless gamma matrices in quantum field theory?

Traceless gamma matrices are important in quantum field theory because they are used to represent spinor fields, which are fundamental to describing the behavior of particles with spin. They also play a crucial role in the formulation of the Dirac equation, which describes the behavior of fermions in quantum mechanics.

4. How are traceless gamma matrices used to simplify calculations?

Traceless gamma matrices are used in calculations in quantum field theory because they have certain properties that make them easier to work with. For example, the traceless property means that certain terms in equations and calculations can be simplified or dropped altogether, leading to more efficient and streamlined calculations.

5. Can traceless gamma matrices be extended to higher dimensions?

Yes, traceless gamma matrices can be extended to higher dimensions. While the most commonly used traceless gamma matrices are 4x4 matrices, they can be defined for any dimension that is a multiple of 4. This allows for their use in higher dimensional quantum field theories or mathematical models that require larger matrices.

Similar threads

Replies
24
Views
2K
Replies
1
Views
857
Replies
1
Views
1K
Replies
5
Views
2K
  • Quantum Physics
Replies
3
Views
2K
  • Quantum Physics
Replies
10
Views
2K
Replies
6
Views
1K
Replies
7
Views
3K
  • Quantum Physics
Replies
6
Views
815
  • Quantum Physics
Replies
6
Views
1K
Back
Top