2014
DOI: 10.1103/physrevd.90.035008
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Nonuniversal gaugino masses and muong2

Abstract: We consider two classes of supersymmetric models with nonuniversal gaugino masses at M GUT in an attempt to resolve the apparent muon g − 2 anomaly encountered in the Standard Model. We explore two distinct scenarios, one in which all gaugino masses have the same sign at M GUT , and a second case with opposite sign gaugino masses. The sfermion masses in both cases are assumed to be universal at M GUT . We exploit the non universality among gaugino masses to realize large mass splitting between the colored and … Show more

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Cited by 59 publications
(47 citation statements)
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References 64 publications
(36 reference statements)
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“…It was shown in ref. [13] that the sleptons can be as light as 100 GeV in this model. This observation motivated us to investigate the decay rate for h → γγ and study the parameter space which yields enhancement or suppression for this process.…”
Section: H → γγ Decay and Particle Spectramentioning
confidence: 99%
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“…It was shown in ref. [13] that the sleptons can be as light as 100 GeV in this model. This observation motivated us to investigate the decay rate for h → γγ and study the parameter space which yields enhancement or suppression for this process.…”
Section: H → γγ Decay and Particle Spectramentioning
confidence: 99%
“…Thus, it is hard to simultaneously explain the observed Higgs boson mass and resolve the muon g − 2 anomaly if we consider CMSSM, NUHM1 or NUHM2, since in all these cases, the slepton masses are larger than 1 TeV. Recently, there have been several attempts to reconcile this apparent tension between muon g − 2 and the Higgs boson mass within the MSSM framework by assuming non-universal SSB mass terms for the gauginos [13,14] or the sfermions [15,16] at the GUT scale. Indeed, a simultaneous explanation of m h and muon g − 2 is possible [17] in the presence of t − b − τ Yukawa coupling unification condition [18].…”
Section: Introductionmentioning
confidence: 99%
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