Muon g - 2 in Higgs-anomaly mediation

被引:14
|
作者
Yanagida, Tsutomu T. [1 ,2 ,3 ]
Yin, Wen [4 ]
Yokozaki, Norimi [5 ]
机构
[1] Shanghai Jiao Tong Univ, TD Lee Inst, Shanghai 200240, Peoples R China
[2] Shanghai Jiao Tong Univ, Sch Phys & Astron, Shanghai 200240, Peoples R China
[3] Univ Tokyo, UTIAS, Kavli IPMU WPI, Kashiwa, Chiba 2778583, Japan
[4] Korea Adv Inst Sci & Technol KAIST, Dept Phys, Daejeon 34141, South Korea
[5] Tohoku Univ, Dept Phys, Sendai, Miyagi 9808578, Japan
关键词
Supersymmetry Phenomenology; DYNAMICAL SUPERSYMMETRY BREAKING; RADIATIVE-CORRECTIONS; BOSON MASS; G-2; UNIFICATION; MSSM;
D O I
10.1007/JHEP06(2020)154
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
A simple model for the explanation of the muon anomalous magnetic moment was proposed by the present authors within the context of the minimal supersymmetric standard model [1, 2]: Higgs-anomaly mediation. In the setup, squarks, sleptons, and gauginos are massless at tree-level, but the Higgs doublets get large negative soft supersymmetry (SUSY) breaking masses squared m(Hu)(2)similar or equal to m(Hd)(2) < 0 at a certain energy scale, M-inp. The sfermion masses are radiatively generated by anomaly mediation and Higgs-loop effects, and gaugino masses are solely determined by anomaly mediation. Consequently, the smuons and bino are light enough to explain the muon g - 2 anomaly while the third generation sfermions are heavy enough to explain the observed Higgs boson mass. The scenario avoids the SUSY flavor problem as well as various cosmological problems, and is consistent with the radiative electroweak symmetry breaking. In this paper, we show that, although the muon g - 2 explanation in originally proposed Higgs-anomaly mediation with M-inp similar to 10(16) GeV is slightly disfavored by the latest LHC data, the muon g - 2 can still be explained at 1 sigma level when Higgs mediation becomes important at the intermediate scale, M-inp similar to 10(12) GeV. The scenario predicts light SUSY particles that can be fully covered by the LHC and future collider experiments. We also provide a simple realization of m(Hu)(2)similar or equal to m(Hd)(2)<0 at the intermediate scale.
引用
收藏
页数:17
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