phenomenon 101.73 The weak interaction is carried by heavy bosons

open in the book · parts/11-qft-standard-model/03-weak-interactions.tex:3553 · p. 1981

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phenomenon 101.73: The weak interaction is carried by heavy bosons101.73equation 101.78: eq:weak-gf-mw101.78proposition 100.63: The QED beta function100.63proposition 101.71: Neutrino–electron elastic scattering101.71proof : ch:03-weak-interactions@proof-51proofequation 100.82: eq:qed-alpha-effective100.82equation 100.83: eq:qed-pi-log100.83proof : ch:02-qed-renormalization@proof-33proofequation 101.60: eq:weak-contact-cross-section101.60equation 101.79: eq:weak-nc-lagrangian101.79phenomenon 101.72: Neutrinos scatter without becoming charged leptons101.72proof : ch:03-weak-interactions@proof-49proof

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typedirectionnode provenancewhere
cites Experimental observation of isolated large transverse energy electrons with associated missing energy at $\sqrt{s}=540$ GeV derived parts/11-qft-standard-model/03-weak-interactions.tex:3558
cites Experimental observation of lepton pairs of invariant mass around 95 GeV/c2 at the CERN SPS collider derived parts/11-qft-standard-model/03-weak-interactions.tex:3560
cites Evidence for Z0$\to$e+e$-$ at the CERN p collider derived parts/11-qft-standard-model/03-weak-interactions.tex:3560
cites Observation of single isolated electrons of high transverse momentum in events with missing transverse energy at the CERN p collider derived parts/11-qft-standard-model/03-weak-interactions.tex:3558
cites Review of Particle Physics derived parts/11-qft-standard-model/03-weak-interactions.tex:3565
depends_on eq:weak-gf-mw declared parts/11-qft-standard-model/03-weak-interactions.tex:3569
depends_on The QED beta function declared parts/11-qft-standard-model/03-weak-interactions.tex:3569
depends_on Neutrino–electron elastic scattering declared parts/11-qft-standard-model/03-weak-interactions.tex:3569
proves ch:03-weak-interactions@proof-51 declared parts/11-qft-standard-model/03-weak-interactions.tex:3572