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CKM Matrix

The CKM quark mixing matrix is the transformation between the strong interaction quark eigenstates
gather83
and the weak interaction quark eigenstates,
gather91
The transformation between these strong and weak mass eigenstates takes the form:
gather105

A test of the unitarity of the CKM matrix would serve to limit certain extensions to the current Standard Model of elementary particles. This test can be performed most reliably by a measure of the sum of the elements of the top row of the matrix: tex2html_wrap_inline4816. If the sum tex2html_wrap_inline4818 is equal to unity, then the matrix is unitary. Using the accepted value for tex2html_wrap_inline4820 and the limits on tex2html_wrap_inline4822, in combination with the value of tex2html_wrap_inline4824 extracted from nuclear beta decay, one finds the result tex2html_wrap_inline4826. This value includes the most reliable nuclear structure dependent corrections, and is lower than the Standard Model prediction by tex2html_wrap_inline4828.

A second evaluation of tex2html_wrap_inline4818, using the value for tex2html_wrap_inline4824 extracted from neutron beta decay, brings the value of tex2html_wrap_inline4834 up to tex2html_wrap_inline4836, which is higher than the Standard Model prediction by tex2html_wrap_inline4838 [15].

A precise extraction of tex2html_wrap_inline4824 is needed to resolve the discrepancy between these two calculations of tex2html_wrap_inline4818. This will be accomplished with the measurement of the pion beta decay rate tex2html_wrap_inline4844, as
equation138
where tex2html_wrap_inline4846 is the weak vector coupling constant.



Penny Slocum
Fri Apr 2 00:36:38 EST 1999