The inelastic scattering of elementary particles
Author:
Publisher
Springer Science and Business Media LLC
Subject
Astronomy and Astrophysics,Nuclear and High Energy Physics,Atomic and Molecular Physics, and Optics
Link
http://link.springer.com/content/pdf/10.1007/BF02732948.pdf
Reference8 articles.
1. A well known example is photo-pion production where thes-wave electric dipole scattering is ordinary scattering, while thep-wave magnetic dipole proceeds through the (3/2, 3/2) resonance.G. F. Chew andF. Low:Phys. Rev. 101, 1579 (1956).
2. G. F. Chew andF. Low:Phys. Rev.,101, 1570 (1956).
3. C. Moller:Det. Kgl. Dan. Vid. Selskab. Mat.-Fys.,23, no. 1 (1945).
4. These parameters are alternatives to the eigen-phase shifts and mixing parameters and avoid the necessity of transforming the physical states to a mixed representation which is awkward when different momenta are associated with different channels. See for exampleBlatt andBiedenharn:Rev. Mod. Phys.,24, 258 (1952).Y. Yamaguchi:Prog. Theor. Phys. (to be published).
5. G. F. Chew, M. L. Goldberger, F. E. Low andY. Nambu:Phys. Rev.,106, 1337 (1957);P. K. Roy:Phys. Rev. Letters,2, 364 (1959).
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1. Paul Taunton Matthews, 19 November 1919 - 26 February 1987;Biographical Memoirs of Fellows of the Royal Society;1988-12
2. Relativistic extension of the Le Couteur-Newton formalism;Il Nuovo Cimento A;1969-10
3. Use of Iteration Procedures to Generate Scattering Approximations;Physical Review;1968-04-25
4. Average Fluctuation Potential as Effective Interaction in Composite-System Scattering;Physical Review;1966-08-19
5. Mass splitting and unitarity;Physics Letters;1965-12
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