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The quark mixing matrix (Kobayashi-Maskawa matrix) is expanded in powers of a small parameter λ equal to sinθc=0.22. The term of order λ² is determined from the recently measured B lifetime. Two remaining parameters, including the CP-nonconservation effects, enter only the term of order λ³ and are poorly constrained. A significant reduction in the limit on ε^'ε possible in an ongoing experiment would tightly constrain the CP-nonconservation parameter and could rule out the hypothesis that the only source of CP nonconservation is the Kobayashi-Maskawa mechanism.
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L. Wolfenstein (1983) studied this question.
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