1998
DOI: 10.1103/physrevd.59.014013
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Quark orbital-angular-momentum distribution in the nucleon

Abstract: We introduce gauge-invariant quark and gluon angular momentum distributions after making a generalization of the angular momentum density operators. From the quark angular momentum distribution, we define the gauge-invariant and leading-twist quark orbital angular momentum distribution L q (x). The latter can be extracted from data on the polarized and unpolarized quark distributions and the off-forward distribution E(x) in the forward limit. We comment upon the evolution equations obeyed by this as well as ot… Show more

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Cited by 86 publications
(98 citation statements)
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References 22 publications
(21 reference statements)
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“…In the forward limit, GPDs reproduce the usual PDFs, and thus a description of GPDs can also be built with the help of the experimental data of PDFs [11]. In addition, the moments of GPDs can provide other new information as well, such as the neutron asymmetry [13] and the quark orbital angular momentum [14,15].…”
Section: Introductionmentioning
confidence: 99%
“…In the forward limit, GPDs reproduce the usual PDFs, and thus a description of GPDs can also be built with the help of the experimental data of PDFs [11]. In addition, the moments of GPDs can provide other new information as well, such as the neutron asymmetry [13] and the quark orbital angular momentum [14,15].…”
Section: Introductionmentioning
confidence: 99%
“…The correct treatment of orbital angular momentum is one of the theoretically most important and probably also most controversal problems in hadron spin physics [1][2][3][4][5][6][7][8][9][10][11][12][13]. On the one hand the ususal NLO-fits to deep inelastic data predict a very large gluon spin (of order 1 ) which has to be balanced by a correspondingly large negative orbital angular momentum contribution.…”
Section: Introductionmentioning
confidence: 99%
“…A similar expression holds for gluons. The balance between the different flavors is ruled by evolution equations of DGLAP type [46], because the Mellin moments in x do not alter the short-distance behaviour of QCD. In the asymptotic limit Q 2 → ∞ of the IMF, the nucleon spin is shared approximately in equal parts by (anti)quarks and gluons (for n f = 5 flavors).…”
Section: Generalized Parton Distributions (Gpds)mentioning
confidence: 99%