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