K0-K¯0 Mixing in the Minimal Flavor-Violating Two-Higgs-Doublet Models

The two-Higgs-doublet model (2HDM), as one of the simplest extensions of the Standard Model (SM), is obtained by adding another scalar doublet to the SM and is featured by a pair of charged Higgs, which could affect many low-energy processes. In the “Higgs basis” for a generic 2HDM, only one scalar...

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Main Authors: Natthawin Cho, Xin-Qiang Li, Fang Su, Xin Zhang
Format: Article
Language:English
Published: Wiley 2017-01-01
Series:Advances in High Energy Physics
Online Access:http://dx.doi.org/10.1155/2017/2863647
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author Natthawin Cho
Xin-Qiang Li
Fang Su
Xin Zhang
author_facet Natthawin Cho
Xin-Qiang Li
Fang Su
Xin Zhang
author_sort Natthawin Cho
collection DOAJ
description The two-Higgs-doublet model (2HDM), as one of the simplest extensions of the Standard Model (SM), is obtained by adding another scalar doublet to the SM and is featured by a pair of charged Higgs, which could affect many low-energy processes. In the “Higgs basis” for a generic 2HDM, only one scalar doublet gets a nonzero vacuum expectation value and, under the criterion of minimal flavor violation, the other one is fixed to be either color-singlet or color-octet, which are named as type III and type C 2HDM, respectively. In this paper, we study the charged-Higgs effects of these two models on the K0-K¯0 mixing, an ideal process to probe New Physics (NP) beyond the SM. Firstly, we perform a complete one-loop computation of the box diagrams relevant to the K0-K¯0 mixing, keeping the mass and momentum of the external strange quark up to the second order. Together with the up-to-date theoretical inputs, we then give a detailed phenomenological analysis, in the cases of both real and complex Yukawa couplings of the charged Higgs to quarks. The parameter spaces allowed by the current experimental data on the mass difference ΔmK and the CP-violating parameter ϵK are obtained and the differences between these two 2HDMs are investigated, which are helpful to distinguish them from each other from a phenomenological point of view.
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spelling doaj-art-4cbb10b6883f4122b0e0c0398b1e799d2025-08-20T02:38:39ZengWileyAdvances in High Energy Physics1687-73571687-73652017-01-01201710.1155/2017/28636472863647K0-K¯0 Mixing in the Minimal Flavor-Violating Two-Higgs-Doublet ModelsNatthawin Cho0Xin-Qiang Li1Fang Su2Xin Zhang3Institute of Particle Physics and Key Laboratory of Quark and Lepton Physics (MOE), Central China Normal University, Wuhan, Hubei 430079, ChinaInstitute of Particle Physics and Key Laboratory of Quark and Lepton Physics (MOE), Central China Normal University, Wuhan, Hubei 430079, ChinaInstitute of Particle Physics and Key Laboratory of Quark and Lepton Physics (MOE), Central China Normal University, Wuhan, Hubei 430079, ChinaInstitute of Particle Physics and Key Laboratory of Quark and Lepton Physics (MOE), Central China Normal University, Wuhan, Hubei 430079, ChinaThe two-Higgs-doublet model (2HDM), as one of the simplest extensions of the Standard Model (SM), is obtained by adding another scalar doublet to the SM and is featured by a pair of charged Higgs, which could affect many low-energy processes. In the “Higgs basis” for a generic 2HDM, only one scalar doublet gets a nonzero vacuum expectation value and, under the criterion of minimal flavor violation, the other one is fixed to be either color-singlet or color-octet, which are named as type III and type C 2HDM, respectively. In this paper, we study the charged-Higgs effects of these two models on the K0-K¯0 mixing, an ideal process to probe New Physics (NP) beyond the SM. Firstly, we perform a complete one-loop computation of the box diagrams relevant to the K0-K¯0 mixing, keeping the mass and momentum of the external strange quark up to the second order. Together with the up-to-date theoretical inputs, we then give a detailed phenomenological analysis, in the cases of both real and complex Yukawa couplings of the charged Higgs to quarks. The parameter spaces allowed by the current experimental data on the mass difference ΔmK and the CP-violating parameter ϵK are obtained and the differences between these two 2HDMs are investigated, which are helpful to distinguish them from each other from a phenomenological point of view.http://dx.doi.org/10.1155/2017/2863647
spellingShingle Natthawin Cho
Xin-Qiang Li
Fang Su
Xin Zhang
K0-K¯0 Mixing in the Minimal Flavor-Violating Two-Higgs-Doublet Models
Advances in High Energy Physics
title K0-K¯0 Mixing in the Minimal Flavor-Violating Two-Higgs-Doublet Models
title_full K0-K¯0 Mixing in the Minimal Flavor-Violating Two-Higgs-Doublet Models
title_fullStr K0-K¯0 Mixing in the Minimal Flavor-Violating Two-Higgs-Doublet Models
title_full_unstemmed K0-K¯0 Mixing in the Minimal Flavor-Violating Two-Higgs-Doublet Models
title_short K0-K¯0 Mixing in the Minimal Flavor-Violating Two-Higgs-Doublet Models
title_sort k0 k¯0 mixing in the minimal flavor violating two higgs doublet models
url http://dx.doi.org/10.1155/2017/2863647
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