On the Test of Pomeron Structure (Parton Distribution Functions)

  • The contributions of the double Pomeron exchange to the J/ψ production inhigh energy p+p(p) collisions are calculated using different models for parton distribution functions inside the Pomeron(P). For the Ingelman-Schlein model in which gluons dominate in partons, the cross sections in high energy increase smoothly with as In2S or InS. The total cross section σ(S) is about 102-103nb in the TeV energies. For the Donnachie-Landshoff model in which the P are considered as something like isoscalar photons with C=+1 the cross section behavior increasing with energy is a little bit complicated. In same energy range, the cross sections are only 1-3nb which are smaller than that of the former case by 2—3 order of magnitude. So, if we assume the parameters of the above models are reliable, then these J/ψ production processes should be a good place for testing these models.
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  • [1] F.E.Low,Phys Rev,D12(1975)163;S.Nussinov,Phys.Rev.Lett,34(1975)1286;Phys.Rev,D14(1976)246;P.V.LandshoffO.Nachtmann,Z.Phys,C35(1987)405.[2]UA8,R.Bonino et al,Phys.Lett,211B(1988)239;UA1,K.Wackeretal,Phys Lett,311B(1993)317;UA8,A.Brandtyetal,Phys.Lett,297B(1992)417;ZUES,D.Allenetal,DESY93-093预印本。[3]G.Ingelman,P.E.Schlein,Phys.Lett,152B(1985)256.[4]A.Donnachie,P.V.Landshoff,Nucl.Phys,B303(1988)634.[5]彭宏安、何祯民、秦克诚,高能物理与核物理,18(1994)1078.彭宏安、秦克诚、何祯民,高能物理与核物理,19(1995)34.[6]P.V.LandshoffandO.Nachtmann,Z.Phys,C35(1987)405;O.Nachtmann,Ann.Phys,209(1991)436.[7]E.L.Berger,D.Jones,Jones,Phys.Rev.,D23(1981)1521;R.Baier,R.Ruckl,Z.Phys,C19(1983)251.[8]A.Schafer,L.Mankiewicz,O.Nachtmann,Phys.Lett.,272B(1991)419;E.Stein.A.Schafer,Phys.Let,300B(1993)403.[9]A.Donnachie,P.V.Land shoff,CERN-TH5020/88预印本。
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He Zhenmin, Lin Zhongjin, Qin Kecheng and Peng Hongan. On the Test of Pomeron Structure (Parton Distribution Functions)[J]. Chinese Physics C, 1995, 19(4): 310-319.
He Zhenmin, Lin Zhongjin, Qin Kecheng and Peng Hongan. On the Test of Pomeron Structure (Parton Distribution Functions)[J]. Chinese Physics C, 1995, 19(4): 310-319. shu
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Received: 1900-01-01
Revised: 1900-01-01
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On the Test of Pomeron Structure (Parton Distribution Functions)

    Corresponding author: He Zhenmin,
  • Department of Physics, Hebei Teacher's University, Shijiazhuang 0500162 Department of Physics, Xiamen University, Xiamen 3610053 Department of Physics, Peking University, Beijing 100871

Abstract: The contributions of the double Pomeron exchange to the J/ψ production inhigh energy p+p(p) collisions are calculated using different models for parton distribution functions inside the Pomeron(P). For the Ingelman-Schlein model in which gluons dominate in partons, the cross sections in high energy increase smoothly with as In2S or InS. The total cross section σ(S) is about 102-103nb in the TeV energies. For the Donnachie-Landshoff model in which the P are considered as something like isoscalar photons with C=+1 the cross section behavior increasing with energy is a little bit complicated. In same energy range, the cross sections are only 1-3nb which are smaller than that of the former case by 2—3 order of magnitude. So, if we assume the parameters of the above models are reliable, then these J/ψ production processes should be a good place for testing these models.

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