A. Zee, Quantum Field Theory in a Nutshell · Problem II.3.3

Field Theory Redux

Physics — QFT

Problem

Show that e−iϕKγ0eiϕK=(0e−ϕσeϕσ0)e^{-i\phi K}\gamma^0 e^{i\phi K} = \begin{pmatrix} 0 & e^{-\phi\sigma} \\ e^{\phi\sigma} & 0 \end{pmatrix} and eϕσ=cosh⁡ϕ+σ⃗⋅ϕ^sinh⁡ϕe^{\phi\sigma} = \cosh \phi + \vec{\sigma} \cdot \hat{\phi} \sinh \phi with the unit vector ϕ^≡ϕ⃗/ϕ\hat{\phi} \equiv \vec{\phi}/\phi. Identifying p⃗=mϕ^sinh⁡ϕ\vec{p} = m\hat{\phi} \sinh \phi, derive the Dirac equation. Show that γi=(0σi−σi0)\gamma^i = \begin{pmatrix} 0 & \sigma^i \\ -\sigma^i & 0 \end{pmatrix}

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