Imaginary eigenvalues of gamma matrices

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Discussion Overview

The discussion revolves around the properties of gamma matrices in the context of the Dirac equation and quantum field theory (QFT). Participants explore the implications of the squares of these matrices leading to real and imaginary eigenvalues, as well as the challenges in manipulating matrix exponentials involving these matrices.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Some participants reference David Tong's notes, noting that if (\gamma^0)^2 = 1, then the eigenvalues are real, while if (\gamma^i)^2 = -1, the eigenvalues are imaginary.
  • One participant explains that if A is a matrix and x is an eigenvector with eigenvalue a, then A^2 x = a^2 x, leading to the conclusion that eigenvalues must satisfy a^2 = 1 or a^2 = -1, resulting in real or imaginary eigenvalues, respectively.
  • Another participant expresses confusion about the exponential expansion involving gamma matrices and the implications of the property (\gamma^0)^2 = 1.
  • Concerns are raised about the non-commutativity of matrices in the context of the exponential expansion, with one participant correcting another's assumption about the form of the expansion.
  • Participants discuss the presence of gamma matrices in the expansion and the resulting complications in the calculations.

Areas of Agreement / Disagreement

Participants show some agreement on the mathematical properties of eigenvalues related to the squares of matrices, but there is disagreement regarding the correct approach to the exponential expansion involving gamma matrices. The discussion remains unresolved regarding the correct handling of these expansions.

Contextual Notes

There are limitations in the discussion regarding assumptions about the commutativity of matrices and the implications of the exponential function for non-commuting operators. Participants do not fully resolve these issues.

center o bass
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Hi! I'm reading David Tong's notes on QFT and I'm now reading on the chapter on the dirac equation

http://www.damtp.cam.ac.uk/user/tong/qft/four.pdf

and I stumbled across a statement where he claims that

(\gamma^0)^2 = 1 \ \ \Rightarrow \text{real eigenvalues}

while

(\gamma^i)^2 = -1 \ \ \Rightarrow \text{imaginary eigenvalues}.

I'm a bit rusty on my linear algebra and just wondered why this is necessarily true. Why does the square of a matrix being positive and negative respectively mean real and imaginary eigenvalues?
 
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Suppose x is an eigenvector of the matrix A with eigenvalue a, so that Ax = ax. Then A^2 x = a^2 x.

Suppose A^2 x = x for all x (including the eigenvectors of A). Then in view of the above, all eigenvalues of A satisfy a^2 = 1. So the possible eigenvalues are +1 and -1.

Now suppose A^2 x = -x for all x. Then all eigenvalues of A satisfy a^2 = -1. So the possible eigenvalues are +i and -i.
 
Ah thanks a lot! :)
 
The_Duck said:
Suppose x is an eigenvector of the matrix A with eigenvalue a, so that Ax = ax. Then A^2 x = a^2 x.

Suppose A^2 x = x for all x (including the eigenvectors of A). Then in view of the above, all eigenvalues of A satisfy a^2 = 1. So the possible eigenvalues are +1 and -1.

Now suppose A^2 x = -x for all x. Then all eigenvalues of A satisfy a^2 = -1. So the possible eigenvalues are +i and -i.
Maybe you could help me with the next thing I'm stuck on? :)

After obtaining that

(S^{\mu \nu})^\dagger = \frac{1}4 [\gamma^\mu, \gamma^\nu]^\dagger = - \gamma^0 S^{\mu \nu} \gamma^0

D. Tong claims that

\exp ( \frac{1}{2} \Omega_{\mu \nu} (S^{\mu \nu})^\dagger ) = \gamma^0 \exp( -\frac{1}{2} \Omega_{\mu \nu} S^{\mu \nu} ) \gamma^0.

I tried obtaining this by doing an exponential expansion and factorizing out the gammas, plus the property that
(\gamma^0)^2 = 1

but I get problems with the even terms in the expansion.
 
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center o bass said:
I tried obtaining this by doing an exponential expansion and factorizing out the gammas, plus the property that
(\gamma^0)^2 = 1

but I get problems with the even terms in the expansion.

What problems? Could you write out what you think the expansions of the left and right-hand sides of the equations are?
 
The_Duck said:
What problems? Could you write out what you think the expansions of the left and right-hand sides of the equations are?

Ofcourse.

\exp(\gamma^0 (-\frac{1}2 \Omega_{\mu \nu} S^{\mu \nu}) \gamma^0)<br /> = 1 + \gamma^0 A \gamma^0 + \frac{1}{2!} (\gamma^0)^2 A^2 (\gamma^0)^2 + \frac{1}{3!}(\gamma^0)^3 A^3 (\gamma^0)^3 + \ldots = \gamma^0 ( 1 + A + \frac{1}{2!} \gamma^0 A \gamma^0 + \frac{1}{3!} A^3 + \ldots )\gamma^0

where i have defined

A = -\frac{1}2 \Omega_{\mu \nu} S^{\mu \nu}
 
OK, two things:

1) Your expansion of the LHS isn't right because gamma-0 and A don't necessarily commute. If A and B are not-necessarily commuting matrices or operators, then

exp(AB) = 1 + AB + (1/2!)ABAB + (1/3!)ABABAB + ...

(recall that, for instance, (AB)^2 = (AB)*(AB)). But you seem to be assuming the incorrect form

exp(AB) = 1 + AB + (1/2!)AABB + (1/3!)AAABBB + ...

which is only equivalent to the correct form if A and B commute (because (AB)(AB) != AABB unless A and B commute). (Of course, you need to apply the equivalent statement for the exponential of the product of three matrices, not just two).2) Why are there some gamma-0's inside the parentheses in your expansion of the RHS?
 
The_Duck said:
OK, two things:

1) Your expansion of the LHS isn't right because gamma-0 and A don't necessarily commute. If A and B are not-necessarily commuting matrices or operators, then

exp(AB) = 1 + AB + (1/2!)ABAB + (1/3!)ABABAB + ...

(recall that, for instance, (AB)^2 = (AB)*(AB)). But you seem to be assuming the incorrect form

exp(AB) = 1 + AB + (1/2!)AABB + (1/3!)AAABBB + ...

which is only equivalent to the correct form if A and B commute (because (AB)(AB) != AABB unless A and B commute). (Of course, you need to apply the equivalent statement for the exponential of the product of three matrices, not just two).


2) Why are there some gamma-0's inside the parentheses in your expansion of the RHS?

Ah, thank you again. The problem lied in the wrong expansion :) The gamma-0's were there due to this wrong expansion. When i tried to factor out gamma-0's to the left and right of the sum gamma-0's remained at the even terms.
 

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