|o
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).
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.
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.
H. K. Lee andH. McManus:Phys. Rev.,161, 1087 (1967);A. Dar: preprint, Technion, Haifa (1970).
N. V. Giai andJ. Sawicki:Phys. Rev.,156, 1077 (1967).
R. H. Bassel andC. Wilkin:Phys. Rev.,174, 1179 (1968).
R. J. Glauber: inLectures in Theoretical Physics, Vol.1 (New York, 1959).
E. Kujawski andT. J. Krieger:Phys. Lett.,27 B, 132 (1968).
F. R. Kroll andN. S. Wall:Phys. Rev. C,1, 138 (1970).
The importance of considering the reaction mechanism and the structure problem as mutually interacting has also been discussed byG. R. Satchler, G. R. Satchler:Comm. Nucl. Part. Phys.,4, 6 (1970).
Author information
Authors and Affiliations
Additional information
Work supported by the National Science Foundation under Contract GU 2061.
Rights and permissions
About this article
Cite this article
Kujawski, E. Coupled-channel formulation for high-energy inelastic nuclear scattering. Lett. Nuovo Cimento 1, 734–738 (1971). https://doi.org/10.1007/BF02770117
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02770117