CERN Accelerating science

002836027 001__ 2836027
002836027 003__ SzGeCERN
002836027 005__ 20240810041945.0
002836027 0247_ $$2DOI$$9Elsevier B.V.$$a10.1016/j.physletb.2022.137386$$qpublication
002836027 0248_ $$aoai:cds.cern.ch:2836027$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002836027 037__ $$9arXiv$$aarXiv:1710.02204$$chep-ph
002836027 035__ $$9arXiv$$aoai:arXiv.org:1710.02204
002836027 037__ $$9arXiv:reportnumber$$aIPMU17-0134
002836027 035__ $$9Inspire$$aoai:inspirehep.net:1628985$$d2024-08-09T08:59:40Z$$h2024-08-10T02:00:05Z$$mmarcxml$$tfalse$$uhttps://inspirehep.net/api/oai2d
002836027 037__ $$9arXiv:reportnumber$$aTU-1047
002836027 035__ $$9Inspire$$a1628985
002836027 041__ $$aeng
002836027 100__ $$aHarigaya, Keisuke$$uLBNL, Berkeley$$uUC, Berkeley$$uCERN$$vTheoretical Physics Department, CERN, Geneva, Switzerland$$vDepartment of Physics, University of California, Berkeley, CA 94720, USA$$vTheoretical Physics Group, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
002836027 245__ $$9Elsevier B.V.$$aAxion induced SUSY breaking and focus point gaugino mediation
002836027 246__ $$9arXiv$$aAxion induced SUSY breaking and focus point gaugino mediation
002836027 269__ $$c2017-10-05
002836027 260__ $$c2022-10-10
002836027 300__ $$a9 p
002836027 520__ $$9arXiv$$aWe consider a scenario where the supersymmetry breaking and its mediation, and the cancellation of the theta parameter of SU(3)c are all caused by a single chiral multiplet. The string axion multiplet is a natural candidate of such a single superfield. We show that the scenario provides a convincing basis of focus point gaugino mediation, where the electroweak scale is explained with a moderate tuning among the parameters of the theory.
002836027 540__ $$3publication$$aCC BY 4.0$$fSCOAP3$$uhttp://creativecommons.org/licenses/by/4.0/
002836027 540__ $$3preprint$$aarXiv nonexclusive-distrib 1.0$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002836027 542__ $$3publication$$dThe Author(s)$$g2022
002836027 65017 $$2INSPIRE$$ahep-ph
002836027 65017 $$2SzGeCERN$$aParticle Physics - Phenomenology
002836027 690C_ $$aARTICLE
002836027 690C_ $$aCERN
002836027 700__ $$aYanagida, Tsutomu T.$$uTsung-Dao Lee Inst., Shanghai$$uTokyo U., IPMU$$vTsung-Dao Lee Institute, Shanghai Jiao Tong University, Shanghai 200240, China$$vKavli IPMU (WPI), UTIAS, University of Tokyo, Kashiwa, Chiba 277-8583, Japan
002836027 700__ $$aYokozaki, [email protected]$$uHangzhou, Zhejiang U.$$uTohoku U.$$vZhejiang Institute of Modern Physics and Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China$$vDepartment of Physics, Tohoku University, Sendai, Miyagi 980-8578, Japan
002836027 773__ $$c137386$$mpublication$$pPhys. Lett. B$$v833$$y2022
002836027 8564_ $$82399316$$s9236$$uhttps://cds.cern.ch/record/2836027/files/fig621.png$$y00001 The contours of $\Delta$ (black solid line) and $m_h$ (red dashed line). In the left (right) panel, $M_1=M_2=M_3$ $(M_1:M_2:M_3=6:2:1)$. On the green dotted lines, $B_\mu$-term vanishes at $M_{\rm in}$. Here, $\alpha_s(m_Z)=0.1181$ and $m_t = 173.34$\,GeV.
002836027 8564_ $$82399317$$s6983$$uhttps://cds.cern.ch/record/2836027/files/DD.png$$y00002 The spin-independent LSP-nucleon scattering cross section as a function of $0.6 M_{1}({\rm TeV}) = M_{2}({\rm TeV})$ for $\mu = 800$ GeV.
002836027 8564_ $$82399318$$s6972$$uhttps://cds.cern.ch/record/2836027/files/fig111.png$$y00000 The contours of $\Delta$ (black solid line) and $m_h$ (red dashed line). In the left (right) panel, $M_1=M_2=M_3$ $(M_1:M_2:M_3=6:2:1)$. On the green dotted lines, $B_\mu$-term vanishes at $M_{\rm in}$. Here, $\alpha_s(m_Z)=0.1181$ and $m_t = 173.34$\,GeV.
002836027 8564_ $$82399319$$s399501$$uhttps://cds.cern.ch/record/2836027/files/Publication.pdf$$yFulltext
002836027 8564_ $$82399320$$s426430$$uhttps://cds.cern.ch/record/2836027/files/1710.02204.pdf$$yFulltext
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