(adsbygoogle = window.adsbygoogle || []).push({}); 1. The problem statement, all variables and given/known data

Dirac proposed that a relativistic wave equation that is linear in both space and time (unlike the Klein-Gordon equation, which is second order) has the form

[itex]i\frac{\partial}{\partial t}\Psi = (\mathbf{\alpha} \cdot \mathbf{p)+\beta m)\Psi[/itex]

After squaring this, we'd like it to satisfy the equation [itex]E^2=p^2+m^2[/itex]. So, after some algebra, you conclude that α and β must be matrices that satisfy:

[itex][\alpha_{i}, \alpha_{j}]_{+} \equiv \alpha_{i}\alpha_{j}+\alpha_{j}\alpha_{i}=0 [/itex]

[itex][\alpha_{i}, \beta]_{+}=0[/itex]

[itex](\alpha_{i})^2=(\beta)^2=1[/itex]

Show that α and β are traceless, Hermetian, have eigenvalues +1 and -1, are of even dimension greater than 4

2. Relevant equations

The commutation relations I gave above.

3. The attempt at a solution

I honestly have no idea where to start...

Maybe write out the equations in terms of the trace?

Ugh, I'm such an idiot....

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# Stupid question on Dirac alpha and beta matrices

Can you offer guidance or do you also need help?

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