Analytic expression for the proton structure function in deep inelastic scattering

  • The analytic expression of proton in deep inelastic scattering is studied by using the color glass condensate model and the dipole picture. We get a better description of the HERA DIS data than the GBW model which was inspired by the Glauber model. We find that our model satisfies the unitarity limit and Froissart
    Bound which refers to an energy dependence of the total cross-section rising no more rapidly than ln2 s.

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  • [1] . Golec-Biernat K J, Wustho M. Phys. Rev. D, 1999, 59:0140172. Golec-Biernat K J, Wustho M. Phys. Rev. D, 1999, 60:1140233. Berger E L, Block M M, Chung-I Tan. Phys. Rev. Lett.,2007, 98: 2420014. Block M M, Berger E L, Chung-I Tan. Phys. Rev. Lett.,2006, 97: 2520035. Froissart M. Phys. Rev., 1961, 123: 10536. Breitweg J et al. (ZEUS Collaboration). Phys. Lett. B,2000, 487: 537. Chekanov S et al. (ZEUS Collaboration). Eur. Phys. J. C,2001, 21: 4438. Adlo C et al. (H1 Collaboration). Eur. Phys. J. C, 2001,21: 339. Kozlov M, Shoshi A, XIANG W. JHEP, 2007, 10: 20
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XIANG Wen-Chang, ZHOU Dai-Cui, WAN Ren-Zhuo and YUAN Xian-Bao. Analytic expression for the proton structure function in deep inelastic scattering[J]. Chinese Physics C, 2009, 33(2): 98-102. doi: 10.1088/1674-1137/33/2/004
XIANG Wen-Chang, ZHOU Dai-Cui, WAN Ren-Zhuo and YUAN Xian-Bao. Analytic expression for the proton structure function in deep inelastic scattering[J]. Chinese Physics C, 2009, 33(2): 98-102.  doi: 10.1088/1674-1137/33/2/004 shu
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Received: 2008-04-22
Revised: 2008-07-28
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Analytic expression for the proton structure function in deep inelastic scattering

    Corresponding author: XIANG Wen-Chang,

Abstract: 

The analytic expression of proton in deep inelastic scattering is studied by using the color glass condensate model and the dipole picture. We get a better description of the HERA DIS data than the GBW model which was inspired by the Glauber model. We find that our model satisfies the unitarity limit and Froissart
Bound which refers to an energy dependence of the total cross-section rising no more rapidly than ln2 s.

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