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- W3020443139 abstract "We study anomalous magnetic moments and flavor violating processes of $e$, $ensuremath{mu}$, and $ensuremath{tau}$ leptons. We use a data driven approach to investigate the implications of the present data on the parameters of a class of models, which has spin-0 scalar and spin-$1/2$ fermion fields. We compare two different cases, which has or does not have a built-in cancelation mechanism. Our findings are as following. Chiral interactions are unable to generate large enough $mathrm{ensuremath{Delta}}{a}_{e}$ and $mathrm{ensuremath{Delta}}{a}_{ensuremath{mu}}$ to accommodate the experimental results. Although sizable $mathrm{ensuremath{Delta}}{a}_{e}$ and $mathrm{ensuremath{Delta}}{a}_{ensuremath{mu}}$ can be generated from nonchiral interactions, they are not contributed from the same source. Presently, the upper limit of $ensuremath{mu}ensuremath{rightarrow}eensuremath{gamma}$ decay gives the most severe constraints on photonic penguin contributions in $ensuremath{mu}ensuremath{rightarrow}e$ transitions, but the situation may change in considering future experimental sensitivities. The $Z$-penguin diagrams can constrain chiral interaction better than photonic penguin diagrams in $ensuremath{mu}ensuremath{rightarrow}e$ transitions. In most of the parameter space, box contributions to $ensuremath{mu}ensuremath{rightarrow}3e$ decay are subleading. The present bounds on $mathrm{ensuremath{Delta}}{a}_{ensuremath{tau}}$ and ${d}_{ensuremath{tau}}$ are unable to give useful constraints on parameters. In $ensuremath{tau}ensuremath{rightarrow}e$ ($ensuremath{mu}$) transitions, the present $ensuremath{tau}ensuremath{rightarrow}eensuremath{gamma}(ensuremath{mu}ensuremath{gamma})$ upper limit constrains the photonic penguin contribution better than the $ensuremath{tau}ensuremath{rightarrow}3e$ $(3ensuremath{mu})$ upper limit, and $Z$-penguin amplitudes constrain chiral interaction better than photonic penguin amplitudes. Box contributions to $ensuremath{tau}ensuremath{rightarrow}3e$ and $ensuremath{tau}ensuremath{rightarrow}3ensuremath{mu}$ decays can sometime be comparable to $Z$-penguin contributions. The ${ensuremath{tau}}^{ensuremath{-}}ensuremath{rightarrow}{e}^{ensuremath{-}}{ensuremath{mu}}^{+}{e}^{ensuremath{-}}$ and ${ensuremath{tau}}^{ensuremath{-}}ensuremath{rightarrow}{ensuremath{mu}}^{ensuremath{-}}{e}^{+}{ensuremath{mu}}^{ensuremath{-}}$ rates are highly constrained by $ensuremath{tau}ensuremath{rightarrow}eensuremath{gamma}$, $ensuremath{mu}ensuremath{rightarrow}eensuremath{gamma}$ and $ensuremath{tau}ensuremath{rightarrow}ensuremath{mu}ensuremath{gamma}$, $ensuremath{mu}ensuremath{rightarrow}eensuremath{gamma}$ upper limits, respectively. We compare the current experimental upper limits, future sensitivities and bounds from consistency on various muon and tau LFV processes." @default.
- W3020443139 created "2020-05-01" @default.
- W3020443139 creator A5001987363 @default.
- W3020443139 date "2020-09-30" @default.
- W3020443139 modified "2023-09-29" @default.
- W3020443139 title "Data-driven study of the implications of anomalous magnetic moments and lepton flavor violating processes of <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi>e</mml:mi></mml:math> , <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi>μ</mml:mi></mml:math> , and <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi>τ</mml:mi></mml:math>" @default.
- W3020443139 cites W1793985650 @default.
- W3020443139 cites W1969561958 @default.
- W3020443139 cites W1975211291 @default.
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- W3020443139 cites W2048660896 @default.
- W3020443139 cites W2050811660 @default.
- W3020443139 cites W2054596921 @default.
- W3020443139 cites W2057899718 @default.
- W3020443139 cites W2089779820 @default.
- W3020443139 cites W2091605720 @default.
- W3020443139 cites W2096107376 @default.
- W3020443139 cites W2116109970 @default.
- W3020443139 cites W2130030623 @default.
- W3020443139 cites W2163389141 @default.
- W3020443139 cites W2165714791 @default.
- W3020443139 cites W2488978209 @default.
- W3020443139 cites W2543917711 @default.
- W3020443139 cites W2785694820 @default.
- W3020443139 cites W2810184318 @default.
- W3020443139 cites W2811101936 @default.
- W3020443139 cites W2885926324 @default.
- W3020443139 cites W2899140785 @default.
- W3020443139 cites W2900781455 @default.
- W3020443139 cites W2902620861 @default.
- W3020443139 cites W2905689665 @default.
- W3020443139 cites W2914471440 @default.
- W3020443139 cites W2923610092 @default.
- W3020443139 cites W2940963246 @default.
- W3020443139 cites W2949740337 @default.
- W3020443139 cites W2951501321 @default.
- W3020443139 cites W2952927646 @default.
- W3020443139 cites W2954200225 @default.
- W3020443139 cites W2961862332 @default.
- W3020443139 cites W2962789046 @default.
- W3020443139 cites W2964897915 @default.
- W3020443139 cites W2964904286 @default.
- W3020443139 cites W2981922023 @default.
- W3020443139 cites W2983995865 @default.
- W3020443139 cites W2984418101 @default.
- W3020443139 cites W2989872841 @default.
- W3020443139 cites W2995868688 @default.
- W3020443139 cites W2998566775 @default.
- W3020443139 cites W3007210348 @default.
- W3020443139 cites W3007976827 @default.
- W3020443139 cites W3015222942 @default.
- W3020443139 cites W3030386577 @default.
- W3020443139 cites W3033428719 @default.
- W3020443139 cites W3035911197 @default.
- W3020443139 cites W3040104600 @default.
- W3020443139 cites W3084107682 @default.
- W3020443139 cites W3098496183 @default.
- W3020443139 cites W3100093382 @default.
- W3020443139 cites W3100492318 @default.
- W3020443139 cites W3100673245 @default.
- W3020443139 cites W3100752619 @default.
- W3020443139 cites W3100992213 @default.
- W3020443139 cites W3101659824 @default.
- W3020443139 cites W3102582290 @default.
- W3020443139 cites W3103517076 @default.
- W3020443139 cites W3104066897 @default.
- W3020443139 cites W3104153388 @default.
- W3020443139 cites W3104168600 @default.
- W3020443139 cites W3104200363 @default.
- W3020443139 cites W3104771801 @default.
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- W3020443139 cites W3105664008 @default.
- W3020443139 cites W3106266322 @default.
- W3020443139 cites W3121284658 @default.
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- W3020443139 doi "https://doi.org/10.1103/physrevd.102.055022" @default.
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