References
M. Gell-Mann andA. Pais:Proceedings of the Glasgow Conference (1954).
G. Wentzel:Phys. Rev.,101, 1214 (1956);G. Takeda:Phys. Rev.,101, 1547 (1956);R. Gatto:Nuovo Cimento,3, 318 (1956).
M. Gell-Mann:Proceedings of the Rochester Conference (1956).
N. Dallaporta:Nuovo Cimento,1, 962 (1955).
K. Iwata, S. Ogawa, H. Okonogi, B. Sakita andS. Oneda:Progr. Theor. Phys.,13, 19 (1955).
A discussion of rulesA andB is given byS. Oneda:Nuclear Physics (in press).
L. W. Alvarez, H. Bradner, P. Falk, J. D. Gow, A. H. Rosenfeld, F. Solmitz andR. D. Tripp: to be published.
T. D. Lee andC. N. Yang:Phys. Rev.,104, 254 (1956);R. L. Garwin, L. M. Lederman andM. Weinrich: to be published;C. S. Wu, E. Ambler, R. W. Hayward, D. D. Hoppes andR. P. Hudson: to be published.
M. Gell-Mann andA. Pais:Phys. Rev.,97, 1387 (1955).
One merely replaces the charge conjugation operatorC of reference (8) byCP, whereP is the parity operator. In a time-reversible theory,CP is conserved.
T. D. Lee, R. Oehme andC. N. Yang: to be published.
Proceedings of the Rochester Conference (1956), Session V.
S. Okubo andR. Marshak:Phys. Rev.,100, 1809 (1955).
Preliminary experimental results of J. Steinberger et al. seem to indicate thatf is much less than 1/3 but not zero. (Private communication from Dr.A. H. Rosenfeld).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Gell-Mann, M. Change of isotopic spin in the Kπ2 decay. Nuovo Cim 5, 758–760 (1957). https://doi.org/10.1007/BF02835607
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02835607