Measuring anomalous ``spin'' in elastic e-p or ν-p and deep inelastic e-p scattering

dc.creatorBass, S. D.
dc.creatorCrewther, R. J.
dc.creatorSteffens, F. M.
dc.creatorThomas, A. W.
dc.date1997-01-03
dc.date1997-03-06
dc.date.accessioned2026-07-07T09:03:26Z
dc.date.available2026-07-07T09:03:26Z
dc.descriptionWe obtain a general rule that the O(1/log m_h) term due to the current \bar{h}γ_μγ_5h of a mass-m_h quark h in f-flavour theory is -3\bar{g}^2_f(m_h)/{2π^2(33-2f)} times the flavour singlet current of the residual (f-1)-flavour theory, where \bar{g}_f is the f-flavour running coupling constant in a mass-independent renormalization scheme. The rule is applied to the Ellis-Jaffe moment below and well above charm threshold, and to low-energy Z^0-exchange amplitudes. The singlet axial charge of the proton common to these experiments is both scale and gauge invariant, but is related to the axial anomaly and the ``gluon spin'' by a non-perturbative renormalization factor.
dc.description11 pages, LaTeX 2.09, no figures; at the end of the text, ``anti-parallel'' replaced by ``aligned'' and a new paragraph referring to the work of Altarelli and Lampe added
dc.identifierhttps://arxiv.org/abs/hep-ph/9701213
dc.identifierhttp://arxiv.org/abs/hep-ph/9701213
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/149010
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectHigh Energy Physics - Experiment
dc.subjectNuclear Theory
dc.titleMeasuring anomalous ``spin'' in elastic e-p or ν-p and deep inelastic e-p scattering
dc.typetext

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