proposition 99.24 Translations act correctly on the field

open in the book · parts/11-qft-standard-model/01-canonical-quantization.tex:1687 · p. 1874

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proposition 99.24: Translations act correctly on the field99.24equation 99.31: eq:canq-ladder99.31equation 99.34: eq:canq-momentum-modes99.34proposition 99.6: The Heisenberg equations reproduce the field equation99.6proposition 99.25: The one-quantum sector is an irreducible representation99.25proof : ch:01-canonical-quantization@proof-12prooflemma 99.33: The Wightman function99.33proposition 99.10: The invariant measure and the relativistic normalization99.10proposition 99.44: The free scalar commutator99.44proposition 99.12: Normalization of the n-quantum states99.12equation 99.23: eq:canq-ccr99.23equation 99.24: eq:canq-ccr-zero99.24equation 99.21: eq:canq-scalar-hamiltonian99.21proof : ch:01-canonical-quantization@proof-2proofdefinition 94.15: Pauli–Lubanski vector94.15theorem 94.18: The Casimir invariants of the Poincaré group94.18proof : ch:01-canonical-quantization@proof-13proof

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typedirectionnode provenancewhere
depends_on eq:canq-ladder declared parts/11-qft-standard-model/01-canonical-quantization.tex:1692
depends_on eq:canq-momentum-modes declared parts/11-qft-standard-model/01-canonical-quantization.tex:1692
depends_on The Heisenberg equations reproduce the field equation declared parts/11-qft-standard-model/01-canonical-quantization.tex:1692
depends_on The one-quantum sector is an irreducible representation declared parts/11-qft-standard-model/01-canonical-quantization.tex:1723
proves ch:01-canonical-quantization@proof-12 declared parts/11-qft-standard-model/01-canonical-quantization.tex:1695