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Volumn 67, Issue 9, 2003, Pages

Transverse momentum in semi-inclusive polarized deep inelastic scattering and the spin-flavor structure of the proton

Author keywords

[No Author keywords available]

Indexed keywords

PROTON;

EID: 0038236348     PISSN: 15507998     EISSN: 15502368     Source Type: Journal    
DOI: 10.1103/PhysRevD.67.097502     Document Type: Article
Times cited : (15)

References (33)
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    • HERMES Collaboration, A. Miller, plenary talk at the SPIN 2002 Conference (BNL), www.c-ad.bnl.gov/SPIN2002/presentations/miller.pdf;, A. Brüll for the HERMES Collaboration, Proceedings of SPIN 2002 Conference, BNL
    • H.E. Jackson, Int. J. Mod. Phys. A 17, 3551 (2002);HERMES Collaboration, A. Miller, plenary talk at the SPIN 2002 Conference (BNL), www.c-ad.bnl.gov/SPIN2002/presentations/miller.pdf;A. Brüll for the HERMES Collaboration, Proceedings of SPIN 2002 Conference, BNL.
    • (2002) Int. J. Mod. Phys. A , vol.17 , pp. 3551
    • Jackson, H.E.1
  • 4
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    • The Spin Muon Collaboration, B. Adeva, Phys. Lett. B 420, 180 (1998).
    • (1998) Phys. Lett. B , vol.420 , pp. 180
    • Adeva, B.1
  • 14
    • 85039026232 scopus 로고    scopus 로고
    • F.E. Close, An Introduction to Quarks and Partons (Academic, New York, 1978), Chap. 13
    • F.E. Close, An Introduction to Quarks and Partons (Academic, New York, 1978), Chap. 13.
  • 18
    • 85039000216 scopus 로고    scopus 로고
    • A. Miller and N. Makins (private communications)
    • A. Miller and N. Makins (private communications).
  • 19
    • 85038979622 scopus 로고    scopus 로고
    • B. Badelek and A. Deshpande (private communications)
    • B. Badelek and A. Deshpande (private communications).
  • 20
    • 85039024770 scopus 로고    scopus 로고
    • S.D. Bass, N.N. Nikolaev, and A.W. Thomas, Adelaide University Report No. ADP-133-T80, 1990; S.D. Bass, Ph.D. thesis, University of Adelaide, 1992
    • S.D. Bass, N.N. Nikolaev, and A.W. Thomas, Adelaide University Report No. ADP-133-T80, 1990; S.D. Bass, Ph.D. thesis, University of Adelaide, 1992.
  • 28
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    • Note that there is no contribution to the first moment from the intermediate region of (Formula presented) between the soft scale set by (Formula presented) and (Formula presented) and the hard scale set by (Formula presented) because the first moment of the spin-dependent Altarelli-Parisi splitting function for (Formula presented) vanishes: (Formula presented)
    • Note that there is no contribution to the first moment from the intermediate region of (Formula presented) between the soft scale set by (Formula presented) and (Formula presented) and the hard scale set by (Formula presented) because the first moment of the spin-dependent Altarelli-Parisi splitting function for (Formula presented) vanishes: (Formula presented)
  • 29
    • 85038987099 scopus 로고    scopus 로고
    • A.V. Efremov and O.V. Teryaev, JINR Report No. E2–88–287, 1988
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  • 31
    • 85038983398 scopus 로고    scopus 로고
    • The optimal conditions for this study are high luminosity and a (Formula presented) detector for full angular acceptance. For (Formula presented) fusion the cutoff (Formula presented) is equivalent to a cutoff on the angular acceptance (Formula presented) where (Formula presented) is defined relative to the photon-gluon direction. Leading-twist negative sea polarization at (Formula presented) corresponds, in part, to final state hadrons produced at large angles
    • The optimal conditions for this study are high luminosity and a (Formula presented) detector for full angular acceptance. For (Formula presented) fusion the cutoff (Formula presented) is equivalent to a cutoff on the angular acceptance (Formula presented) where (Formula presented) is defined relative to the photon-gluon direction. Leading-twist negative sea polarization at (Formula presented) corresponds, in part, to final state hadrons produced at large angles.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.