STATISTICAL CHARACTERISTIC OF THE INITIAL EXCITON NUMBER n0 AND IT'S INFLUENCE ON THE RESULTS IN THE EXCITON MODEL

  • It is assumed that the initial exciton number n0 is statistical. The expression of the probability h(n0) for any probable n0 is given. The theoretical calculation results, including the energy spectra and the double differential cross sections, are obtained by weighted summation of the contributions coming from various probable n0. The agreement between experimental data and the theoretical results is quite well.
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  • [1] C. K. Cline and M. Blann, Nucl. Phys., A172(1971) 225-259.[2] J. J. Griffin, Phys. Lett., Vol. 24B (1967), No. 1.[3] C. K. Cline. Nucl. Phys, A193 (1972), 417-437.[4] M. Blann, Nukleonika, Vol. 21, No. 4/76.[5] G. Mantzouranis, H. A. Weidenmuller and D. Agassi, Z. Physik, A276(1976), 145-154.[6] C. Kalbach-Cline, Nucl. Phys., A210(1973), 59G-604.[7] P. Oblozinsky, I. Ribansky and E. Betak, Nucl. Phys., A226 (1974), 347.[8] J. J. Griffin, Phys. Rev. Lett., 17(1966), 478481.[9] J. M. Akkermens, H. Gruppelaar and G. Reffo, Phys. Rev., C22 (1980), 73.[10] 缪容之, 吴国华, 刘建业, 余超凡, 中国科学院近代物理研究所内部资料.[11] 缪容少, 昊国华, 余超凡、刘建业, 中国科学院内部资料.[12] J. M. Akkermans, Z. Physik, A292 (1979), 57-59.[13] A. Chevarier et al., Phys. Rev., C11 (1975), 11.[14] I. Ribansky and P. Obalozinsky, Phys. Lett. 45B (1973), 22-24.
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MIAO Rong-Zhi, WU Guo-Hua, ZHENG Wei-Han, LIU Jian-Ye, YU Chao-Fan and YU Xian. STATISTICAL CHARACTERISTIC OF THE INITIAL EXCITON NUMBER n0 AND IT'S INFLUENCE ON THE RESULTS IN THE EXCITON MODEL[J]. Chinese Physics C, 1984, 8(6): 740-747.
MIAO Rong-Zhi, WU Guo-Hua, ZHENG Wei-Han, LIU Jian-Ye, YU Chao-Fan and YU Xian. STATISTICAL CHARACTERISTIC OF THE INITIAL EXCITON NUMBER n0 AND IT'S INFLUENCE ON THE RESULTS IN THE EXCITON MODEL[J]. Chinese Physics C, 1984, 8(6): 740-747. shu
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Received: 1900-01-01
Revised: 1900-01-01
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STATISTICAL CHARACTERISTIC OF THE INITIAL EXCITON NUMBER n0 AND IT'S INFLUENCE ON THE RESULTS IN THE EXCITON MODEL

    Corresponding author: MIAO Rong-Zhi,

Abstract: It is assumed that the initial exciton number n0 is statistical. The expression of the probability h(n0) for any probable n0 is given. The theoretical calculation results, including the energy spectra and the double differential cross sections, are obtained by weighted summation of the contributions coming from various probable n0. The agreement between experimental data and the theoretical results is quite well.

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