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Trimaximal mixing : ウィキペディア英語版
Trimaximal mixing
Trimaximal mixing〔
〕 (also known as threefold maximal mixing〔
〕) refers to the highly symmetric, maximally CP-violating, 3 \times 3 fermion mixing configuration, characterised by a unitary matrix (U) having all its elements equal in modulus
( |U_|=1/\sqrt, a,i=1,2,3) as may be written, e.g.:
:
U=
\begin
\frac}}
\Rightarrow (|U_|^2)=
\begin
\frac & \frac & \frac \\
\frac & \frac & \frac \\
\frac & \frac & \frac
\end

where \omega=\exp(i2\pi/3) and \bar=\exp(-i2\pi/3)
are the complex cube roots of unity. In the standard PDG〔
〕 convention, trimaximal mixing corresponds to: \theta_=\theta_=\pi/4, \theta_=\sin^(1/\sqrt) and \delta=\pi/2. The Jarlskog CP-violating parameter J
〕 takes its extremal value |J|=1/(6\sqrt).
Originally proposed as a candidate lepton mixing matrix,〔
〕〔
〕 and actively studied〔〔〔
〕〔
〕 as such (and even as a candidate quark mixing matrix〔
〕), trimaximal mixing is now definitively ruled-out as a phenomenologically viable lepton mixing scheme by neutrino oscillation experiments, especially the CHOOZ reactor experiment,〔
〕 in favour of the no longer tenable (related) tribimaximal mixing
〕 scheme.
==References==


抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Trimaximal mixing」の詳細全文を読む



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