theorem 108.67 Weinberg's principle

open in the book · parts/11-qft-standard-model/10-renormalization-group.tex:2512 · p. 2283

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theorem 108.67: Weinberg's principle108.67equation 108.6: eq:rg-effective-strength108.6equation 108.3: eq:rg-operator-dimension108.3theorem 108.26: Power counting in 3+1108.26proof : ch:10-renormalization-group@proof-29proofphenomenon 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 100.1: eq:qed-mass-shell100.1corollary 108.27: The three classes108.27proof : ch:10-renormalization-group@proof-12proof

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typedirectionnode provenancewhere
cites Effective Field Theory derived parts/11-qft-standard-model/10-renormalization-group.tex:2522
cites Phenomenological Lagrangians derived parts/11-qft-standard-model/10-renormalization-group.tex:2522
depends_on eq:rg-effective-strength declared parts/11-qft-standard-model/10-renormalization-group.tex:2523
depends_on eq:rg-operator-dimension declared parts/11-qft-standard-model/10-renormalization-group.tex:2523
depends_on Power counting in $3+1$ declared parts/11-qft-standard-model/10-renormalization-group.tex:2523
proves ch:10-renormalization-group@proof-29 declared parts/11-qft-standard-model/10-renormalization-group.tex:2527