2017
DOI: 10.1103/physrevd.96.115034
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Lepton-flavored electroweak baryogenesis

Abstract: We explore lepton-flavored electroweak baryogenesis, driven by CP-violation in leptonic Yukawa sector, using the τ − μ system in the two Higgs doublet model as an example. This setup generically yields, together with the flavor-changing decay h → τμ, a tree-level Jarlskog invariant that can drive dynamical generation of baryon asymmetry during a first-order electroweak phase transition and results in CP-violating effects in the decay h → ττ. We find that the observed baryon asymmetry can be generated in parame… Show more

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Cited by 56 publications
(71 citation statements)
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“…• v w and Hydrodynamics -A stronger GW production usually requires a larger v w , while a successful EWBG needs a small, generally subsonic v w (for EWBG calculations, see e.g., [26][27][28][29][30]). Hence, a large v w , which can source detectable GW signals, is detrimental to the process of generating the observed baryon asymmetry of the universe.…”
Section: Gravitational Wavesmentioning
confidence: 99%
“…• v w and Hydrodynamics -A stronger GW production usually requires a larger v w , while a successful EWBG needs a small, generally subsonic v w (for EWBG calculations, see e.g., [26][27][28][29][30]). Hence, a large v w , which can source detectable GW signals, is detrimental to the process of generating the observed baryon asymmetry of the universe.…”
Section: Gravitational Wavesmentioning
confidence: 99%
“…This was studied in relation to the LFV decay h → τ µ in [9,19,34,47,53,70,76,130], and very recently in [134,135]. It could also be linked to the popular b → s [31,48] or b → c [42] anomalies observed in B-meson decays or be a crucial ingredient for lepton-flavored electroweak baryogenesis [80]. In fact, the type-III 2HDM with generic Yukawa couplings has a very rich flavor phenomenology, see [130].…”
Section: Hlfv Phenomenologymentioning
confidence: 99%
“…Since ρ is measured to be nearly one [183], we conclude that Thus, enlarging the SM with a scalar doublet is a natural framework, which is known as Two Higgs Doublet Model (2HDM) [322]. The 2HDM has a rich phenomenology and possesses several nice features such as links to Supersymmetry [283], axion models [323][324][325][326], baryogenesis [327][328][329][330][331][332][333][334][335][336][337][338] and even furnishes an environment for dark matter [339][340][341][342][343], among others [344,345]. In what follows, we will be restricted to the non-supersymmetric 2HDM, see [346] for an extensive discussion.…”
Section: Two Higgs Doublet Modelmentioning
confidence: 99%