theorem 106.72 Confinement at strong coupling

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theorem 106.72: Confinement at strong coupling106.72equation 106.81: eq:pathint-wilson-action106.81equation 106.83: eq:pathint-wilson-potential106.83theorem 5.158: Schur's first lemma5.158theorem 102.60: Confinement at strong coupling, and what it proves102.60proof : ch:08-path-integral-quantization@proof-50proofphenomenon 102.64: Almost none of the proton's mass comes from quark masses102.64proposition 109.82: Wilson's action is reflection positive109.82definition 5.37: Linear transformation5.37definition 5.147: Invariant subspace5.147definition 5.148: Irreducible representation5.148corollary 14.18: A Casimir acts as a number on an irreducible representation14.18lemma A.427: Invariant bilinear forms on a simple algebraA.427lemma A.405: Schur, algebra formA.405phenomenon 102.1: Hadron masses obey an octet mass formula102.1proposition 5.161: Irreducible representations of an abelian group5.161theorem 102.12: Which quark combinations can be colour singlets102.12proof : ch:03-linear-algebra-representations@proof-67proofequation 106.84: eq:pathint-strong-coupling106.84theorem 100.25: One-photon exchange is the Coulomb potential100.25proof : ch:04-qcd@proof-30proof

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typedirectionnode provenancewhere
depends_on eq:pathint-wilson-action declared parts/11-qft-standard-model/08-path-integral-quantization.tex:3384
depends_on eq:pathint-wilson-potential declared parts/11-qft-standard-model/08-path-integral-quantization.tex:3384
depends_on Schur's first lemma declared parts/11-qft-standard-model/08-path-integral-quantization.tex:3384
depends_on Confinement at strong coupling, and what it proves declared parts/11-qft-standard-model/04-qcd.tex:2498
proves ch:08-path-integral-quantization@proof-50 declared parts/11-qft-standard-model/08-path-integral-quantization.tex:3388