equation 108.3 eq:rg-operator-dimension

open in the book · parts/11-qft-standard-model/10-renormalization-group.tex:92

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equation 108.3: eq:rg-operator-dimension108.3phenomenon 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 five108.72theorem 108.26: Power counting in 3+1108.26theorem 108.67: Weinberg's principle108.67equation 108.5: eq:rg-hatted-coupling108.5proof : ch:10-renormalization-group@proof-32proofequation 100.2: eq:qed-action100.2proof : ch:10-renormalization-group@proof-1proofequation 108.2: eq:rg-reduced-scalar108.2proof : ch:10-renormalization-group@proof-30proofequation 100.1: eq:qed-mass-shell100.1corollary 108.27: The three classes108.27proof : ch:10-renormalization-group@proof-12proofequation 108.6: eq:rg-effective-strength108.6proof : ch:10-renormalization-group@proof-29proof

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depends_on The proton does not decay declared parts/11-qft-standard-model/10-renormalization-group.tex:2876
depends_on The SI dimension of a coupling declared parts/11-qft-standard-model/10-renormalization-group.tex:125
depends_on There is exactly one operator of dimension five declared parts/11-qft-standard-model/10-renormalization-group.tex:2692
depends_on Power counting in $3+1$ declared parts/11-qft-standard-model/10-renormalization-group.tex:948
depends_on Weinberg's principle declared parts/11-qft-standard-model/10-renormalization-group.tex:2523