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  • Access by Xinjiang University

Diffraction Scattering for Inelastic Processes

Hung Cheng*

Tai Tsun Wu

  • Department of Mathematics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139

  • Gordon McKay Laboratory, Harvard University, Cambridge, Massachusetts 02138

  • *Work supported in part by the National Science Foundation.

Phys. Rev. D 1, 459 – Published 15 January, 1970

DOI: https://doi.org/10.1103/PhysRevD.1.459

Abstract

Previous treatments on high-energy scattering in quantum electrodynamics are extended to diffractive inelastic processes. We explore the model in which the diffractive excitation proceeds through the exchange of vector mesons. Six inelastic impact factors are explicitly calculated in the lowest order: (1) scalar to scalar, (2) pseudoscalar to pseudoscalar, (3) vector to vector, (4) axial vector to axial vector, (5) scalar to axial vector, and (6) pseudoscalar to axial vector. For all six of these impact factors, the masses of the incoming and outgoing particles may be different; and for the last two impact factors, the spins and the parities of the incoming and outgoing particles may be different. The nonvanishing of the impact factors demonstrates that mass, spin, and parity can change during a diffractive process. We also conclude that C (charge conjugation quantum number), S (strangeness), I (isotopic spin), B (baryon number), and G parity, etc., must remain the same during a diffractive process. Some general properties of the impact factor are also discussed.

References (9)

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  4. Omitted endnote

  5. H. Cheng and T. T. Wu, Phys. Rev. Letters 23, 670 (1969) (to be published)
  6. P. Roman, Theory of Elementary Particles (North-Holland Publishing Co., Amsterdam, 1960), p. 285
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  8. T. T. Chou and C. N. Yang, Phys. Rev. 175, 1832 (1968)
  9. N. Byers and S. Frautschi, in Proceedings of the Fourteenth International Conference on High-Energy Physics, Vienna, 1968 (CERN, Geneva, 1968)

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