2004
DOI: 10.1103/physrevd.70.074032
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NLO QCD procedure of the semi-inclusive deep inelastic scattering data analysis with respect to the light quark polarized sea

Abstract: The semi-inclusive deep inelastic scattering (SIDIS) process is considered. A theoretical procedure is proposed allowing the direct extraction from the SIDIS data of the first moments of the polarized valence distributions and of the first moment difference of the light sea quark polarized distributions in the next to leading QCD order. The validity of the procedure is confirmed by the respective simulations

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Cited by 18 publications
(5 citation statements)
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“…The unpolarised distributions s(x) and G(x) used in this test are taken from the MRST parametrisation [26]. This procedure leads to asymmetric errors on the parameters when the fitted value is close to the allowed limit.The fits have been performed with two different programs: the first one uses the DGLAP evolution equations for the spin structure functions [27], the other one, referred to in [28], uses the evolution of moments. The fitted PDF parameters are compatible within one standard deviation and the two programs give the same χ 2 -probabilities.…”
mentioning
confidence: 99%
“…The unpolarised distributions s(x) and G(x) used in this test are taken from the MRST parametrisation [26]. This procedure leads to asymmetric errors on the parameters when the fitted value is close to the allowed limit.The fits have been performed with two different programs: the first one uses the DGLAP evolution equations for the spin structure functions [27], the other one, referred to in [28], uses the evolution of moments. The fitted PDF parameters are compatible within one standard deviation and the two programs give the same χ 2 -probabilities.…”
mentioning
confidence: 99%
“…moments ∆ 1 ū and ∆ 1 d even in the case of rather narrow HERMES x-range, while for the wide COMPASS x-range we deal with here this approximation works very well -see the respective numerical tests in Ref. [5]. The point is that since the valence PDFs (contrary to the sea PDFs) are suppressed near the low boundary x = 0 (so that ∆q = ∆q V + ∆q → ∆q as x → 0), the omitted in r.h.s.…”
mentioning
confidence: 58%
“…For the scenario preserving SU f (2) symmetry (AKK08 parametrization for FFs here) the procedure of direct extraction in NLO QCD of n-th moments of the valence PDFs from the measured difference asymmetries is described in Refs. [5], [7] in details. Let us recall the key necessary equations.…”
mentioning
confidence: 99%
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