SUSY breaking mediation mechanisms and (g-2)mu, B -> X-s gamma, B -> X(s)l(+)l(-) and B-s -> mu(+)mu(-)

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dc.contributor.authorBaek, Seungwonko
dc.contributor.authorKo, PyungWonko
dc.contributor.authorSong, Wan Youngko
dc.date.accessioned2013-03-04T01:03:30Z-
dc.date.available2013-03-04T01:03:30Z-
dc.date.created2012-02-06-
dc.date.created2012-02-06-
dc.date.issued2003-03-
dc.identifier.citationJOURNAL OF HIGH ENERGY PHYSICS, no.3, pp.3417 - 3428-
dc.identifier.issn1126-6708-
dc.identifier.urihttp://hdl.handle.net/10203/81194-
dc.description.abstractWe show that there are qualitative differences in correlations among (g - 2)(mu), B --> X-s gamma, B --> X(s)l(+)l(-) and B-s --> mu(+)mu(-) in various SUSY breaking mediation mechanisms: minimal supergravity (mSUGRA), gauge mediation (GMSB), anomaly mediation (AMSB), gaugino mediation ((g) over tilde MSB), weakly and strongly interacting string theories, and D brane models. After imposing the direct search limits on the Higgs boson and SUSY particle search limits and B --> X(s)gamma branching ratio, we find all the scenarios can accommodate the a(mu) = (g - 2)(mu)/2 in the range of (a few tens) x 10(-10), and predict that the branching ratio for B --> X(s)l(+)l(-) can differ from the standard model (SM) prediction by +/-20% but no more. On the other hand, the B-s --> mu(+)mu(-) is sensitive to the SUSY breaking mediation mechanisms through the pseudoscalar and stop masses (m(A) and m((t) over tilde1)), and the stop mixing angle. In the GMSB with a small messenger number, the AMSB, the (g) over tilde MSB and the noscale scenarios, one finds that B(B-s --> mu(+)mu(-)) less than or similar to 2 x 10(-8), which is below the search limit at the Tevatron Run II. Only the mSUGRA or string inspired models can generate a large branching ratio for this decay.-
dc.languageEnglish-
dc.publisherINT SCHOOL ADVANCED STUDIES-
dc.subjectANOMALOUS MAGNETIC-MOMENT-
dc.subjectDYNAMICAL SUPERSYMMETRY BREAKING-
dc.subjectLARGE TAN-BETA-
dc.subjectMUON G-2-
dc.subjectSTANDARD MODEL-
dc.subjectDARK-MATTER-
dc.subjectLEADING LOGARITHMS-
dc.subjectPARAMETER SPACE-
dc.subjectCOLOR BREAKING-
dc.subjectQUARK MASS-
dc.titleSUSY breaking mediation mechanisms and (g-2)mu, B -> X-s gamma, B -> X(s)l(+)l(-) and B-s -> mu(+)mu(-)-
dc.typeArticle-
dc.identifier.wosid000182939300054-
dc.type.rimsART-
dc.citation.issue3-
dc.citation.beginningpage3417-
dc.citation.endingpage3428-
dc.citation.publicationnameJOURNAL OF HIGH ENERGY PHYSICS-
dc.identifier.doi10.1088/1126-6708/2003/03/054-
dc.contributor.nonIdAuthorBaek, Seungwon-
dc.contributor.nonIdAuthorSong, Wan Young-
dc.type.journalArticleReview-
dc.subject.keywordAuthorsupersymmetry breaking-
dc.subject.keywordAuthorsupersymmetry phenomenology-
dc.subject.keywordAuthorsupersymmetric standard model-
dc.subject.keywordAuthorB-physics-
dc.subject.keywordPlusANOMALOUS MAGNETIC-MOMENT-
dc.subject.keywordPlusDYNAMICAL SUPERSYMMETRY BREAKING-
dc.subject.keywordPlusLARGE TAN-BETA-
dc.subject.keywordPlusMUON G-2-
dc.subject.keywordPlusSTANDARD MODEL-
dc.subject.keywordPlusDARK-MATTER-
dc.subject.keywordPlusLEADING LOGARITHMS-
dc.subject.keywordPlusPARAMETER SPACE-
dc.subject.keywordPlusCOLOR BREAKING-
dc.subject.keywordPlusQUARK MASS-
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