46 research outputs found

    Top Down Electroweak Dipole Operators

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    We derive present constraints on, and prospective sensitivity to, the electric dipole moment (EDM) of the top quark (dtd_t) implied by searches for the EDMs of the electron and nucleons. Above the electroweak scale vv, the dtd_t arises from two gauge invariant operators generated at a scale Λv\Lambda \gg v that also mix with the light fermion EDMs under renormalization group evolution at two-loop order. Bounds on the EDMs of first generation fermion systems thus imply bounds on dt|d_t|. Working in the leading log-squared approximation, we find that the present upper bound on dt|d_t| is roughly 101910^{-19} ee cm for Λ=1\Lambda = 1 TeV, except in regions of finely tuned cancellations that allow for dt|d_t| to be up to fifty times larger. Future ded_e and dnd_n probes may yield an order of magnitude increase in dtd_t sensitivity, while inclusion of a prospective proton EDM search may lead to an additional increase in reach.Comment: 7 pages, 6 figure

    Toward verification of electroweak baryogenesis by electric dipole moments

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    We study general aspects of the CP-violating effects on the baryon asymmetry of the Universe (BAU) and electric dipole moments (EDMs) in models extended by an extra Higgs doublet and a singlet, together with electroweak-interacting fermions. In particular, the emphasis is on the structure of the CP-violating interactions and dependences of the BAU and EDMs on masses of the relevant particles. In a concrete mode, we investigate a relationship between the BAU and the electron EDM for a typical parameter set. As long as the BAU-related CP violation predominantly exists, the electron EDM has a strong power in probing electroweak baryogenesis. However, once a BAU-unrelated CP violation comes into play, the direct correlation between the BAU and electron EDM can be lost. Even in such a case, we point out that verifiability of the scenario still remains with the help of Higgs physics.Comment: 7 pages, 5 figure

    Electroweak Baryogenesis driven by Extra Top Yukawa Couplings

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    We study electroweak baryogenesis driven by the top quark in a general two Higgs doublet model with flavor-changing Yukawa couplings, keeping the Higgs potential CPCP invariant. With Higgs sector couplings and the additional top Yukawa coupling ρtt\rho_{tt} all of O\mathcal{O}(1), one naturally has sizable CPCP violation that fuels the cosmic baryon asymmetry. Even if ρtt\rho_{tt} vanishes, the favor-changing coupling ρtc\rho_{tc} can still lead to successful baryogenesis. Phenomenological consequences such as tcht\to ch, τμγ\tau \to \mu\gamma, electron electric dipole moment, hγγh\to\gamma\gamma, and hhhhhh coupling are discussed.Comment: 5 pages, 3 figures; v2: updated to match version published in PL

    ALP contributions to μe\mu\to e conversion

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    We study the μe\mu\to e conversion process in nuclear targets arising in models of axion-like particles (ALPs) with hadronic and charged lepton flavor violating (CLFV) interactions. Contributions to this process generally fall into two categories: spin-independent (SI) and spin-dependent (SD). While the SI contribution can be generated by a dipole operator through purely leptonic ALP interactions, the SD contribution can also be present through ALP-quark interactions at tree-level. It is naively anticipated that the SI contribution would be dominant due to its coherent enhancement. In this letter\textit{letter}, we show that is not generically the case; in particular, for naturally-sized ALP couplings to quarks of order  ⁣mq/fa\sim\!m_q/f_a, the SD interaction induced by ALP-π0\pi^0 mixing turns out to be the leading contribution to μe\mu\to e conversion. Intuitively, this stems from the suppressed dipole contribution by the QED one-loop factor which counters the effect of SI coherent enhancement. Our study highlights the importance of μe\mu\to e conversion searches in exploring the parameter space of generic ALP models, and demonstrates the competitiveness of these searches in probing the CLFV ALP parameter space in the heavy mass range of mamμm_a\gtrsim m_{\mu}.Comment: 6 pages, 4 figure
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