Abstract
The observable consequences of particle symmetry or charge symmetry in reactions of the type b(a,c)c’ are well known. Here, the final-state particles c and c’ are the charge-symmetric members of an isospin doublet or are identical particles, c = c’. The symmetries imposed on the angular distributions of the cross section and the analyzing powers have been given by Barshay and Temmerl) and Simonius2):
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References
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Conzett, H.E. (1976). Polarization Symmetries in Direct Reactions: \( ^3He{\left( {\vec t,d} \right)^4}He \) and \( ^2H{\left( {\vec d,p} \right)^3}H \) . In: Grüebler, W., König, V. (eds) Proceedings of the Fourth International Symposium on Polarization Phenomena in Nuclear Reactions. Experientia Supplementum, vol 25. Birkhäuser, Basel. https://doi.org/10.1007/978-3-0348-5506-8_10
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DOI: https://doi.org/10.1007/978-3-0348-5506-8_10
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