equation 99.31 eq:canq-ladder

open in the book · parts/11-qft-standard-model/01-canonical-quantization.tex:766

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equation 99.31: eq:canq-ladder99.31lemma 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 states99.12proposition 99.24: Translations act correctly on the field99.24equation 99.37: eq:canq-invariant-measure99.37equation 99.29: eq:canq-mode-phi99.29proof : ch:01-canonical-quantization@proof-18proofequation 99.28: eq:canq-dispersion99.28proof : ch:01-canonical-quantization@proof-5proofequation 99.91: eq:canq-wightman99.91corollary 99.50: Compatible field averages99.50corollary 99.45: No signalling99.45proposition 99.48: Integer spin cannot be quantized with anticommutators99.48proof : ch:01-canonical-quantization@proof-26proofequation 99.38: eq:canq-relativistic-normalization99.38proof : ch:01-canonical-quantization@proof-6proofequation 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-12proof

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depends_on The Wightman function declared parts/11-qft-standard-model/01-canonical-quantization.tex:2358
depends_on The invariant measure and the relativistic normalization declared parts/11-qft-standard-model/01-canonical-quantization.tex:948
depends_on The free scalar commutator declared parts/11-qft-standard-model/01-canonical-quantization.tex:2914
depends_on Normalization of the $n$-quantum states declared parts/11-qft-standard-model/01-canonical-quantization.tex:1088
depends_on Translations act correctly on the field declared parts/11-qft-standard-model/01-canonical-quantization.tex:1692