Coupled-channel formulation for high-energy inelastic nuclear scattering
Author:
Publisher
Springer Science and Business Media LLC
Subject
General Physics and Astronomy
Link
http://link.springer.com/content/pdf/10.1007/BF02770117.pdf
Reference10 articles.
1. K. M. Watson:Phys. Rev.,89, 575 (1953);N. Francis andK. M. Watson:Phys. Rev.,92, 291 (1953);W. B. Riesenfeld andK. M. Watson:Phys. Rev.,102, 1157 (1956);M. L. Goldberger andK. M. Watson:Collision Theory, Chap.11 (New York, 1964).
2. A. K. Kerman, H. McManus andR. M. Thaler:Ann. of Phys.,8, 551 (1959) (referred to as KMT);E. Kujawski:Phys. Rev. C,1, 1651 (1970). KMT provide a slightly different multiple-scattering expansion thanWatson. Their second-order term, which contains the effective interaction in the propagator, includes all of Watson's higher-order terms with elastic scattering in intermediate states.
3. H. Feshbach andJ. Hüfner:Ann. of Phys.,56, 268 (1970);H. Feshbach, A. Gal andJ. Hüfner: M.I.T. preprint CTP 150 (Sept. 1970);W. Brown andE. Kujawski: University of Maryland Technical Report No. 71-010 (July 1970), to appear inAnn. of Phys.
4. H. K. Lee andH. McManus:Phys. Rev.,161, 1087 (1967);A. Dar: preprint, Technion, Haifa (1970).
5. N. V. Giai andJ. Sawicki:Phys. Rev.,156, 1077 (1967).
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1. Multi-step processes in high-energy elastic and inelastic nuclear scattering;Nuclear Physics A;1974-12
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