- #1
arivero
Gold Member
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Three little known equalities:
From Smirnov:
[tex] \theta_{\mbox{sun}} + \theta_{\mbox{cabibbo}} = {\pi \over 4} [/tex]
From De Vries:
[tex] \ln {m_\tau \over m_\mu} = \pi - {1 \over \pi} [/tex]
From Smirnov again:
[tex] \sqrt {m_\mu \over m_\tau} \sim \sin \theta_{\mbox{Cab.} } [/tex]
Can anyone predict them?
de Vries has a secondary formula for the electron-muon relationship, namely
ln(mu/me) / (2pi-3/pi) = 1.000627.
In principle one could recast them in terms of hyperbolic cosines and sines, for instance 1pi-1/pi= 2 sinh(ln(pi)) but it does not clarify the situation.
See also:
https://www.physicsforums.com/showthread.php?t=36624
http://arxiv.org/abs/hep-ph/0405088
http://www.chip-architect.com/news/2004_07_27_The_Electron.html
From Smirnov:
[tex] \theta_{\mbox{sun}} + \theta_{\mbox{cabibbo}} = {\pi \over 4} [/tex]
From De Vries:
[tex] \ln {m_\tau \over m_\mu} = \pi - {1 \over \pi} [/tex]
From Smirnov again:
[tex] \sqrt {m_\mu \over m_\tau} \sim \sin \theta_{\mbox{Cab.} } [/tex]
Can anyone predict them?
de Vries has a secondary formula for the electron-muon relationship, namely
ln(mu/me) / (2pi-3/pi) = 1.000627.
In principle one could recast them in terms of hyperbolic cosines and sines, for instance 1pi-1/pi= 2 sinh(ln(pi)) but it does not clarify the situation.
See also:
https://www.physicsforums.com/showthread.php?t=36624
http://arxiv.org/abs/hep-ph/0405088
http://www.chip-architect.com/news/2004_07_27_The_Electron.html
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