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1.2 Experimental motivation

According to the Standard Model (SM), the strong mass eigenstates of the quarks are different from the eigenstates for the weak force. Cabibbo parameterized this difference in 1963 in the form of a matrix that rotated the quark mass eigenstates of the strong force into the weak eigenstates [Cab 63]. Cabibo's parameterization dealt only with four quarks (u, d, s, and c) and used a single parameter known as the Cabibbo angle. In 1973, Kobayashi and Maskawa extended the idea to all six quarks (three generations) and gave an explicit parameterization for what is known as the Cabibbo-Kobayashi-Maskawa quark mixing matrix (CKM) [Kob 73]. In the CKM, only the charge -1/3e quarks (d, s, b) mix by convention as show here:

According to the SM, the CKM is a unitary matrix; thus, adding the elements of any row in quadrature should result in unity. Given the experimental precision with which each of the elements of the CKM has been determined, the top row provides the most stringent test of unitarity.

(1.5)

has been determined from Ke3 decays (e.g. K+ -> p 0 e+ n e) to be 0.2196 ± 0.0023 [PDG 96, Shr 78] . A more recent re-analysis by Barker et al. modifies the value only slightly to 0.2199 ± 0.0017 [Bar 92]. Slightly higher values of have been determined from the study of hyperon decays (e.g. [Xi] -> [Lambda] e n and [Sigma]- -> n e n ) [Gar 92] which leads to an overall average of 0.2205 ± 0.0018 [PDG 96].

The value has not yet been determined directly. Values for and however, have been measured and can be used to indicate of the magnitude of . The value can be determined from the semileptonic decay of B mesons produced on the [hammer](4S) resonance. The current value, which combines the experimental and theoretical uncertainties, is [PDG 96]:

=0.08 ± 0.02 (1.6)

The value can be obtained from B semileptonic decays to charmed mesons ( ). The current value of is :

=0.041 ± 0.003 (1.7)

Combining (1.6) and (1.7) yields a value for on the order of 10-3 (about the same order uncertainty as in ) and is therefore safe to ignore.

The dominant term in (1.5) is which can be determined from both nuclear beta-decay and neutron decay experiments. The results disagree somewhat as described below.


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