1966
DOI: 10.1146/annurev.ns.16.120166.002455
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Weak Interactions (Second section) Chapter 9: Decays of Neutral K Mesons

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Cited by 201 publications
(91 citation statements)
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“…the two phenomenological quantities ε and ε signal CP and CP T -violating effects that occur directly in the decay amplitudes and are used to parametrize the following constant amplitude ratios [16][17][18] …”
Section: The Neutral Kaon Systemmentioning
confidence: 99%
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“…the two phenomenological quantities ε and ε signal CP and CP T -violating effects that occur directly in the decay amplitudes and are used to parametrize the following constant amplitude ratios [16][17][18] …”
Section: The Neutral Kaon Systemmentioning
confidence: 99%
“…Nevertheless, one usually takes the approximation of neglecting the lepton mass; [16] in this case, one can show that O is constant so that a state |K can be defined and the corresponding probabilities | K|K | 2 can be related to measurable quantities, as explained before. However, this approximation is not necessary if one assumes, as we will do, the validity of the socalled ∆S = ∆Q rule; [16,17] in this case only K 0 and not K 0 can decay into + π − ν. This allows us to associate to the final state + π − ν the constant projector…”
Section: The Neutral Kaon Systemmentioning
confidence: 99%
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“…Lee and Wolfenstein (1965) and Lee and Wu (1966a) instance, the super-weak interaction postulated by Wolfenstein (1964) has recently been shown to be invalidated by measurements of the relative decay rates of the ~ meson into neutral and charged pions (Gaillard, et al, 1967).…”
Section: Disclaimermentioning
confidence: 99%
“…This is certainly not the case for other meson systems, like the B 0B0 , D 0D0 and B 0 sB 0 s systems (see below). Inserting now the quantum mechanical expectation value (58) into inequality (54) we arrive at Ghirardi, Grassi and Weber's result [56] …”
Section: Bell Inequality For Time Variationmentioning
confidence: 99%