theorem 108.26 Power counting in $3+1$

open in the book · parts/11-qft-standard-model/10-renormalization-group.tex:936 · p. 2265

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theorem 108.26: Power counting in 3+1108.26equation 100.1: eq:qed-mass-shell100.1equation 108.3: eq:rg-operator-dimension108.3corollary 108.27: The three classes108.27theorem 108.67: Weinberg's principle108.67proof : ch:10-renormalization-group@proof-12proofcorollary 108.81: Almost all of the proton's mass is anomalous108.81phenomenon 100.20: The Compton shift100.20phenomenon 108.76: The proton does not decay108.76proposition 108.3: The SI dimension of a coupling108.3proposition 108.72: There is exactly one operator of dimension five108.72equation 108.29: eq:rg-superficial-degree108.29proof : ch:10-renormalization-group@proof-13proofequation 108.6: eq:rg-effective-strength108.6proof : ch:10-renormalization-group@proof-29proof

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typedirectionnode provenancewhere
depends_on eq:qed-mass-shell declared parts/11-qft-standard-model/10-renormalization-group.tex:948
depends_on eq:rg-operator-dimension declared parts/11-qft-standard-model/10-renormalization-group.tex:948
depends_on The three classes declared parts/11-qft-standard-model/10-renormalization-group.tex:1011
depends_on Weinberg's principle declared parts/11-qft-standard-model/10-renormalization-group.tex:2523
proves ch:10-renormalization-group@proof-12 declared parts/11-qft-standard-model/10-renormalization-group.tex:951