Srednicki — Quantum Field Theory · Problem 39.3

Canonical Quantization of Scalar Fields — Mark Srednicki

Physics — QFT · canonical-quantization-spinor-fields-ii

Problem

Show that U(Λ)−1bs†(p)U(Λ)=bs†(Λ−1p) ,U(\Lambda)^{-1}b_s^\dagger(\mathbf{p})U(\Lambda) = b_s^\dagger(\Lambda^{-1}\mathbf{p})\,, U(Λ)−1ds†(p)U(Λ)=ds†(Λ−1p) ,(39.39)U(\Lambda)^{-1}d_s^\dagger(\mathbf{p})U(\Lambda) = d_s^\dagger(\Lambda^{-1}\mathbf{p})\,, \tag{39.39} and hence that U(Λ)∣p,s,q⟩=∣Λp,s,q⟩ ,(39.40)U(\Lambda)|p,s,q\rangle = |\Lambda p,s,q\rangle\,, \tag{39.40} where ∣p,s,+⟩≡bs†(p)∣0⟩ ,|p,s,+\rangle \equiv b_s^\dagger(\mathbf{p})|0\rangle\,, ∣p,s,−⟩≡ds†(p)∣0⟩(39.41)|p,s,-\rangle \equiv d_s^\dagger(\mathbf{p})|0\rangle \tag{39.41} are single-particle states.

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