In a two-triplet Type-II seesaw, resonant leptogenesis at the TeV scale dynamically requires small Yukawa couplings that suppress observable lepton flavor violation as a direct consequence of successful baryogenesis.
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Simulations of the positron transport system for MACE report 65.81% geometric acceptance, 88 by 102 micrometer position resolution, and 6.9 ns transit time spread enabling 10 to the minus 7 background rejection.
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Resonant Leptogenesis in a Two-Triplet Type-II Seesaw: A Dynamical Origin of Suppressed Lepton Flavor Violation
In a two-triplet Type-II seesaw, resonant leptogenesis at the TeV scale dynamically requires small Yukawa couplings that suppress observable lepton flavor violation as a direct consequence of successful baryogenesis.
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Positron Transport System for Muonium-to-Antimuonium Conversion Experiment
Simulations of the positron transport system for MACE report 65.81% geometric acceptance, 88 by 102 micrometer position resolution, and 6.9 ns transit time spread enabling 10 to the minus 7 background rejection.