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CP violation

Journal Article · · AIP Conf. Proc.; (United States)
DOI:https://doi.org/10.1063/1.33015· OSTI ID:6149474
Talks on CP violation have a tendency to seem the same every year. The subject is one on which the progress is somewhat limited. The first table has been the first table for a long time. It says that, from a phenomenological point of view, one can discuss three kinds of CP violation. It think this table first appeared in the paper T. D. Lee and I wrote in 1965. We can classify the different kinds of CP violation according to their different selection rules with respect to strangeness change, 0, 1 or 2. In particular we will emphasize the one and two, one being called milliweak of strength of order 10/sup -3/ weak, and two being superweak which is very weak, because it allows at tree level ..delta..S = 2. The experimental consequences of superweak are well known; so far, they have turned out to be in agreement with what has been found. The best chances to find effects that are contrary to superweak in experiments now going on are: (1) the electric dipole moment of the neutron, for which the limit now is something like 10/sup -24/ e-cm, and for which an experiment now in progress hopes to get down to 10/sup -26/ and perhaps lower; (2) the famous eta/sub 00//eta/sub +/- parameter (really magnitude), which is the ratio of the CP forbidden ..pi../sup 0/..pi../sup 0/ mode to the forbidden ..pi../sup +/..pi../sup -/ mode. The deviation of Vertical Bareta/sub 00//eta/sub +/-Vertical Bar from unity is now known to be less than 6%. Two experiments, one by Cronin and collaborators and one by Adair and his collaborators, hope to see this at a level of 1%, if it exists.
Research Organization:
Carnegie-Mellon Univ., Pittsburgh, Pennsylvania
OSTI ID:
6149474
Report Number(s):
CONF-801244-
Journal Information:
AIP Conf. Proc.; (United States), Journal Name: AIP Conf. Proc.; (United States) Vol. 72:1; ISSN APCPC
Country of Publication:
United States
Language:
English