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17044387923
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B. Frois, V. W. Hughes, N. de Groot
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N. Isgur, in The Spin Structure of the Nucleon, Proceedings of the 1995 Erice School, edited by B. Frois, V. W. Hughes, and N. de Groot (World Scientific, Singapore, 1997), p. 260.
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Isgur, N.1
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7
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33744577451
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Phys. Rev. DA. Chodos, R. L. Jaffe, K. Johnson, and C. B. Thorn, 10, 2599 (1974);
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Chodos, A.1
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10
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85038335166
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See, for example, the pedagogical review by B. L. Ioffe, in The Spin Structure of the Nucleon
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See, for example, the pedagogical review by B. L. Ioffe, in The Spin Structure of the Nucleon 1, p. 215.
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13
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0000763762
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E143 Collaboration, K. Abe, Phys. Rev. Lett. 74, 346 (1995);
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Phys. Rev. Lett.
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Abe, K.1
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7244240884
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Phys. Rev. Lett.E154 Collaboration, K. Abe, 79, 26 (1997);
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EMC Collaboration, J. Ashman, Nucl. Phys. B328, 1 (1989);
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Ashman, J.1
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17044415779
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SMC Collaboration, D. Adams, Phys. Lett. B 329, 199 (1994);
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17044439924
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V. Hughes, C. Cavata
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For a pedagogical discussion see A. H. Mueller, in Internal Spin Structure of the Nucleon, edited by V. Hughes and C. Cavata (World Scientific, Singapore, 1995), p. 91;
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Mueller, A.H.1
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22
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30944433125
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The (Formula presented) basis used here sacrifices explicit flavor symmetry in favor of a more compact and physically transparent wave function. See, e.g., N. Isgur and G. Karl, Phys. Rev. D 19, 2653 (1979).
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Phys. Rev. D
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Isgur, N.1
Karl, G.2
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26
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0037851554
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In lectures at the 1977 Zakopane Summer School [N. Isgur, Acta Phys. Pol. B 8, 1081 (1977)], I argued that the (Formula presented) splitting suggests that (Formula presented) is broken in such a way that the neutron charge radius and the observation that (Formula presented) as (Formula presented) in deep inelastic scattering might be explained as related effects. This discussion was based on the observation that the spin wave function (7) may be written in the form (Formula presented) and interpreted as an expansion of (Formula presented) in the nonorthogonal basis (Formula presented) in which the (Formula presented) pairs (13) and (23), respectively, form a tightly bound spin zero “core.” While qualitatively correct, as with Refs. 12131415 it is unclear whether the conclusions drawn in this framework about the full valence region survive antisymmetrization.
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Acta Phys. Pol. B
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Isgur, N.1
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27
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4243757394
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In addition to valence quark models based on the nucleon’s confinement-dominated wave function, there is a proposal by Farrar and Jackson that as (Formula presented) the distribution functions will be dominated by hard perturbative precesses [G. Farrar and D. Jackson, Phys. Rev. Lett. 35, 1416 (1975);
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Phys. Rev. Lett.
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Jackson, D.2
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28
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0000518551
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for a recent exposition see S. J. Brodsky, M. Burkardt, and I. Schmidt, Nucl. Phys. B441, 197 (1995)]. In that case near (Formula presented) (Formula presented) (Formula presented) (Formula presented) and (Formula presented) where now the parallel distribution function (Formula presented) dominates over the antiparallel distribution function (Formula presented) as (Formula presented) This model thus leads to (Formula presented) as (Formula presented) but still predicts that both (Formula presented) and (Formula presented) as (Formula presented) While (Formula presented) seems to have fallen well below (Formula presented) it could be argued that this discrepancy is due to errors in extracting (Formula presented) from deuterium data. This issue would be worth examining in the light of new high precision data and modern theories of the deuteron’s high momentum structure.
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Nucl. Phys.
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Brodsky, S.J.1
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Schmidt, I.3
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29
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0000143812
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See, e.g., the analysis of S. Liuti and F. Gross, Phys. Lett. B 356, 157 (1995) which supports (Formula presented) and that of
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Phys. Lett. B
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Liuti, S.1
Gross, F.2
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33
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17044404839
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see also F. E. Close, Introduction to Quarks and Partons (Academic, New York, 1979), p. 197
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F. E. CloseNucl. Phys. B80, 269 (1974);see also F. E. Close, Introduction to Quarks and Partons (Academic, New York, 1979), p. 197.
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Close, F.E.1
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26144470410
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A. Le Yaouanc, L. Oliver, O. Péne, and J. C. Raynal, Phys. Rev. D 11, 680 (1975);
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Oliver, L.2
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Raynal, J.C.4
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