phenomenon 108.56 The strong coupling runs as predicted

open in the book · parts/11-qft-standard-model/10-renormalization-group.tex:1950 · p. 2277

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phenomenon 108.56: The strong coupling runs as predicted108.56equation 102.19: eq:qcd-alpha-s-def102.19equation 102.42: eq:qcd-beta-qcd102.42proposition 108.52: Asymptotic freedom as a property of the flow108.52proof : ch:10-renormalization-group@proof-25prooflemma 102.31: The vacuum's two responses are reciprocal102.31phenomenon 102.39: A mass scale from a dimensionless coupling102.39theorem 102.33: The one-loop coefficient, from a magnetic response102.33corollary 102.50: Moments diagonalise the evolution102.50corollary 108.53: The condition on the number of flavours108.53phenomenon 102.41: The strong coupling weakens with energy102.41corollary 108.8: The flow is integrable in closed form108.8equation 108.24: eq:rg-beta-series108.24corollary 108.62: Two Standard Model sectors are effective108.62proof : ch:10-renormalization-group@proof-23proof

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typedirectionnode provenancewhere
cites The 2009 world average of $\alpha$ s derived parts/11-qft-standard-model/10-renormalization-group.tex:1960
cites The 2009 world average of $\alpha$ s derived parts/11-qft-standard-model/10-renormalization-group.tex:1968
cites Review of Particle Physics derived parts/11-qft-standard-model/10-renormalization-group.tex:1960
cites Review of Particle Physics derived parts/11-qft-standard-model/10-renormalization-group.tex:1967
cites Review of Particle Physics derived parts/11-qft-standard-model/10-renormalization-group.tex:1970
depends_on eq:qcd-alpha-s-def declared parts/11-qft-standard-model/10-renormalization-group.tex:1974
depends_on eq:qcd-beta-qcd declared parts/11-qft-standard-model/10-renormalization-group.tex:1974
depends_on Asymptotic freedom as a property of the flow declared parts/11-qft-standard-model/10-renormalization-group.tex:1974
proves ch:10-renormalization-group@proof-25 declared parts/11-qft-standard-model/10-renormalization-group.tex:1978