Analyses of the pion valence-quark distribution function (DF), , which explicitly incorporate the behaviour of the pion wave function prescribed by quantum chromodynamics (QCD), predict , β(ζ≳mp)>2, where mp is the proton mass. Nevertheless, more than forty years after the first experiment to collect data suitable for extracting the x≃1 behaviour of , the empirical status remains uncertain because some methods used to fit existing data return a result for that violates this constraint. Such disagreement entails one of the following conclusions: the analysis concerned is incomplete; not all data being considered are a true expression of qualities intrinsic to the pion; or QCD, as it is currently understood, is not the theory of strong interactions. New, precise data are necessary before a final conclusion is possible. In developing these positions, we exploit a single proposition, viz. there is an effective charge which defines an evolution scheme for parton DFs that is all-orders exact. This proposition has numerous corollaries, which can be used to test the character of any DF, whether fitted or calculated.

Concerning pion parton distributions

D. Binosi;
2022-01-01

Abstract

Analyses of the pion valence-quark distribution function (DF), , which explicitly incorporate the behaviour of the pion wave function prescribed by quantum chromodynamics (QCD), predict , β(ζ≳mp)>2, where mp is the proton mass. Nevertheless, more than forty years after the first experiment to collect data suitable for extracting the x≃1 behaviour of , the empirical status remains uncertain because some methods used to fit existing data return a result for that violates this constraint. Such disagreement entails one of the following conclusions: the analysis concerned is incomplete; not all data being considered are a true expression of qualities intrinsic to the pion; or QCD, as it is currently understood, is not the theory of strong interactions. New, precise data are necessary before a final conclusion is possible. In developing these positions, we exploit a single proposition, viz. there is an effective charge which defines an evolution scheme for parton DFs that is all-orders exact. This proposition has numerous corollaries, which can be used to test the character of any DF, whether fitted or calculated.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11582/330370
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