Parity conservation and compositeness
Author:
Publisher
Springer Science and Business Media LLC
Subject
General Medicine
Link
http://link.springer.com/content/pdf/10.1007/BF02721058.pdf
Reference5 articles.
1. F. Zachariasen andC. Zemach:Phys. Rev.,138, B 441 (1965). Referred to as ZZ.
2. A. Salam:Nuovo Cimento,25, 224 (1962); the connection with theN/D method has been discussed byR. M. Rockmore:Phys. Rev.,132, 878 (1963).
3. Cf.R. Delbourgo:Nuovo Cimento,32, 1380 (1965), where a term of the formiy·py sis likewise removed from the renormalized to the bare propagator.
4. M. Baker andS. Glashow:Phys. Rev.,128, 2462 (1962). In Sect.5, they discuss massless fermious interacting through aT-invariant coupling with a spin-1 boson, and show that, in lowest order,Z 1=0 forces either conservation or maximal violation ofP andC.
5. Cf.L. S. Liu:Phys. Rev.,125, 761 (1962), Sect.5.
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1. A Vector Meson Exchange Model for the Electromagnetic Mass Difference of Pseudoscalar Mesons;Progress of Theoretical Physics;1967-12
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