메뉴 건너뛰기




Volumn 59, Issue 3, 1999, Pages

Valence quark spin distribution functions

Author keywords

[No Author keywords available]

Indexed keywords


EID: 17044401690     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.59.034013     Document Type: Article
Times cited : (123)

References (46)
  • 10
    • 85038335166 scopus 로고    scopus 로고
    • See, for example, the pedagogical review by B. L. Ioffe, in The Spin Structure of the Nucleon
    • See, for example, the pedagogical review by B. L. Ioffe, in The Spin Structure of the Nucleon 1, p. 215.
  • 13
    • 0000763762 scopus 로고
    • E143 Collaboration, K. Abe, Phys. Rev. Lett. 74, 346 (1995);
    • (1995) Phys. Rev. Lett. , vol.74 , pp. 346
    • Abe, K.1
  • 15
  • 16
    • 33745278175 scopus 로고
    • EMC Collaboration, J. Ashman, Nucl. Phys. B328, 1 (1989);
    • (1989) Nucl. Phys. , vol.B328 , pp. 1
    • Ashman, J.1
  • 17
    • 17044415779 scopus 로고
    • SMC Collaboration, D. Adams, Phys. Lett. B 329, 199 (1994);
    • (1994) Phys. Lett. B , vol.329 , pp. 199
    • Adams, D.1
  • 20
    • 17044439924 scopus 로고
    • V. Hughes, C. Cavata
    • 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;
    • (1995) Internal Spin Structure of the Nucleon , pp. 91
    • Mueller, A.H.1
  • 22
    • 30944433125 scopus 로고
    • 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).
    • (1979) Phys. Rev. D , vol.19 , pp. 2653
    • Isgur, N.1    Karl, G.2
  • 26
    • 0037851554 scopus 로고
    • 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.
    • (1977) Acta Phys. Pol. B , vol.8 , pp. 1081
    • Isgur, N.1
  • 27
    • 4243757394 scopus 로고
    • 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);
    • (1975) Phys. Rev. Lett. , vol.35 , pp. 1416
    • Farrar, G.1    Jackson, D.2
  • 28
    • 0000518551 scopus 로고
    • 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.
    • (1995) Nucl. Phys. , vol.B441 , pp. 197
    • Brodsky, S.J.1    Burkardt, M.2    Schmidt, I.3
  • 29
    • 0000143812 scopus 로고
    • See, e.g., the analysis of S. Liuti and F. Gross, Phys. Lett. B 356, 157 (1995) which supports (Formula presented) and that of
    • (1995) Phys. Lett. B , vol.356 , pp. 157
    • Liuti, S.1    Gross, F.2
  • 33
    • 17044404839 scopus 로고
    • see also F. E. Close, Introduction to Quarks and Partons (Academic, New York, 1979), p. 197
    • F. E. CloseNucl. Phys. B80, 269 (1974);see also F. E. Close, Introduction to Quarks and Partons (Academic, New York, 1979), p. 197.
    • (1974) Nucl. Phys. , vol.B80 , pp. 269
    • Close, F.E.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.