QCD PREDICTION FOR THE REACTION γ+p→2γ+X

  • In the framework of the perturbative QCD, the two-fold differential cross section d2σ/dxTdxL of the reaction γ+p→2γ+X and its two backgrounds (γ+p→γ++X, γ+p→γ++X) are calculated in c.m.s.. The results show that, in a large range of (xT, xL), the calculated reaction cross section can be measured in current laboratory condition. And due to the properties of this reaction, i.e., large pT photoproduction and direct photon pair emission, all of the backgrounds can be greatly suppressed.

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  • [1] E. Amaldi et al., Phys. Lett., 77B (1978), 240;84B (1979) 360; Phys. Lett., B150 (1979), 326;J. H. Cobb et al., Phys. Lett., 78B (1978), 519;R. M. Baltrusaitis et al., Phys. Lett., 88B (1979), 372;M. Diakonon et al., Phys. Lett., 87B ( 1979), 292;Phys. Lett., 91B (1980), 296.[2] C. Carimalo et al.,Phys. Lett., 98B (1981), 105.[3] J. F. Owens, Phys. Rev., D21 (1980), 54.[4] D. Treille and P. Weilhammer, Private Communication With T. S. Tu[5] H. Feitesch and P. Minkowski, Phys. Lett., 69B (19771, 316.[6] Tung-Sheng TU and Chi-min WU, Nucl. Phys., B156 (1979), 493.[7] A. J. Buras and K. J. P. Gaemers, Nucl. Phys., B132 (1978), 249.[8] C. H. Llewellyn Smith, Phys. Lett., 79B ( 1978), 83.[9] W. A. Bardeen and A. J. Buras, Ferrnilab PUB 79-91 (1978).[10] R. D. Field and R. P. Feynman, Nucl. Phys., B136 (1978), 1[11] Katsuji JGUCHI and Akira NIEGAWA, Prog Tlzeor. Phys., Vol. 64 No. 3 (1980), 1093.
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LUO Ma. QCD PREDICTION FOR THE REACTION γ+p→2γ+X[J]. Chinese Physics C, 1984, 8(5): 539-547.
LUO Ma. QCD PREDICTION FOR THE REACTION γ+p→2γ+X[J]. Chinese Physics C, 1984, 8(5): 539-547. shu
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Received: 1900-01-01
Revised: 1900-01-01
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QCD PREDICTION FOR THE REACTION γ+p→2γ+X

    Corresponding author: LUO Ma,
  • Nankai University

Abstract: 

In the framework of the perturbative QCD, the two-fold differential cross section d2σ/dxTdxL of the reaction γ+p→2γ+X and its two backgrounds (γ+p→γ++X, γ+p→γ++X) are calculated in c.m.s.. The results show that, in a large range of (xT, xL), the calculated reaction cross section can be measured in current laboratory condition. And due to the properties of this reaction, i.e., large pT photoproduction and direct photon pair emission, all of the backgrounds can be greatly suppressed.

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