Sidney Coleman — Quantum Field Theory Lectures · Problem 1.1

September 23 - Units; Translational invariance, Rotational invariance and Lorentz invariance for a single free particle — Sidney Coleman

Physics — QFT · rotational-invariance-single-particle

Problem

Prove that U(R)†HU(R)=HU(R)^\dagger H U(R) = H (equation (1.8)), where U(R)∣k⃗⟩=∣Rk⃗⟩U(R)|\vec{k}\rangle = |R\vec{k}\rangle and H∣k⃗⟩=ωk⃗∣k⃗⟩=∣k⃗∣2+μ2∣k⃗⟩H|\vec{k}\rangle = \omega_{\vec{k}}|\vec{k}\rangle = \sqrt{|\vec{k}|^2 + \mu^2}|\vec{k}\rangle.

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