Abstract
Computation of the correction rate has shown that:
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-- in double tagging experiments, the radiative corrections are rather small. The inelastic corrections are limited by the resolution of the tagging system and, thus,we have a very small contribution of the hard photons. Moreover, the use of the double equivalent photon approximation is completely justified in that case.
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-- in no tagging experiments, the radiative corrections are extremely small and even negligible. They cannot practically affect the cross section.
However, there are other types of γγ experiments, namely single-tagging experiments and measurements at finite angle, and the next work is to compute the corresponding radiative corrections to obtain their order of magnitude.
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References
G. COCHARD & S.ONG, Phys. Rev. D19, 810 (1979).
S.Ong, Thése de Troisième Cycle, Univ. of Paris VI (1976), unpublished.
A. COURAU et al., Phys. Lett. 84 B, 145 (1979).
M.DEFRISE, S.ONG end J.SILVA, submitted for publication to Phys. Rev. D. (1980). Numerical results relative to the radiative corrections in the no tagging case published in “ A double equivalent-photon approximation including radiative corrections for photon-photon collision experiments without electron tagging” (LPTP 80/l, S.ONG et al.) and in “Update on photon-photon collisions” (LPC 80/06, N.ARTEAGA-ROMERO et al.) are wrong.
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© 1980 Springer-Verlag
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Cochard, G., Ong, S. (1980). Radiative corrections to γ γ processes in e+e− ,e− e+e+collision rings. In: Cochard, G., Kessler, P. (eds) γγ Collisions. Lecture Notes in Physics, vol 134. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-10262-0_13
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DOI: https://doi.org/10.1007/3-540-10262-0_13
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