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@@ -250,7 +250,7 @@ flavour was experimentally verified in the Nobel Prize-winning experiment of
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Danby et al. at Brookhaven National Laboratory
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(BNL)~\cite{DanbyGaillard.etal.1962}. Then the concepts of generations of
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particles was developed~\cite{MakiNakagawa.etal.1962}, and integrated into the
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SM, in which the lepton flavour conservation is guaranteed by and exact
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SM, in which the lepton flavour conservation is guaranteed by an exact
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symmetry, owing to massless neutrinos.
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Following the above LFV searches with muons, searches with various particles,
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@@ -267,11 +267,11 @@ must be modified to accommodate the massive neutrinos.
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With the massive neutrinos charged lepton flavour violation (CLFV) must occur
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through oscillations in loops. But, CLFV processes are highly suppressed in the
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SM.
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For example, Marciano and Mori ~\cite{MarcianoMori.etal.2008} calculated the
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%\hl{TODO: Feynman diagram}
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For example, Marciano and Mori~\cite{MarcianoMori.etal.2008} calculated the
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branching ratio of the process \mueg to be \brmeg$<10^{-54}$. Other
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CLFV processes with muons are also suppressed to similar practically
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unmeasurable levels.%\hl{TODO: Feynman diagram}
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Therefore, any experimental
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unmeasurable levels. Therefore, any experimental
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observation of CLFV would be an unambiguous signal of the physics beyond the
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SM. Many theoretical models for physics beyond the SM, including supersymmetric
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(SUSY) models, extra dimensional models, little Higgs models, predict
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@@ -308,7 +308,7 @@ significantly larger CLFV
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%It is calculated that there are two CLFV processes that would
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%occur at large rates by many new physics models,
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Among the CLFV processes, the \mueg and
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the \muec are expected to have large effect by many models. The current
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the \muec are expected to have large effect in many models. The current
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experimental limits on these two decay modes are set respectively by the MEG
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experiment~\cite{Adam.etal.2013} and the SINDRUM-II
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experiment~\cite{Bertl.etal.2006}:
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