Abstract
Experimental consequences of milliweak gauge models of CP violation that may distinguish them from superweak are discussed. Included are η00 in K0→2π decay, η+−0 in K0→3π decay, and the electric dipole moment of the neutron. Emphasis is on the six‐quark SU(2)×U(1) model (Kobayashi–Maskawa CP violation).
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
