Flavor physics in an SO(10) grand unified model
In supersymmetric grand-unified models, the lepton mixing matrix can possibly affect flavor-changing transitions in the quark sector. We present a detailed analysis of a model proposed by Chang, Masiero and Murayama, in which the near-maximal atmospheric neutrino mixing angle governs large new b → ...
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creator | Girrbach, Jennifer Jäger, Sebastian Knopf, Markus Martens, Waldemar Nierste, Ulrich Scherrer, Christian Wiesenfeldt, Sören |
description | In supersymmetric grand-unified models, the lepton mixing matrix can possibly affect flavor-changing transitions in the quark sector. We present a detailed analysis of a model proposed by Chang, Masiero and Murayama, in which the near-maximal atmospheric neutrino mixing angle governs large new
b
→
s
transitions. Relating the supersymmetric low-energy parameters to seven new parameters of this SO(10) GUT model, we perform a correlated study of several flavor-changing neutral current (FCNC) processes. We find the current bound on
more constraining than
. The LEP limit on the lightest Higgs boson mass implies an important lower bound on tan β, which in turn limits the size of the new FCNC transitions. Remarkably, the combined analysis does not rule out large effects in mixing and we can easily accomodate the large CP phase in the
system which has recently been inferred from a global analysis of CDF and DØ data. The model predicts a particle spectrum which is different from the popular Constrained Minimal Supersymmetric Standard Model (CMSSM).
enforces heavy masses, typicallyabove1TeV,forthesfermionsofthedegeneratefirsttwogenerations. However, the ratio of the third-generation and first-generation sfermion masses is smaller than in the CMSSM and a (dominantly right-handed) stop with massbelow500GeV is possible. |
doi_str_mv | 10.1007/JHEP06(2011)044 |
format | Article |
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b
→
s
transitions. Relating the supersymmetric low-energy parameters to seven new parameters of this SO(10) GUT model, we perform a correlated study of several flavor-changing neutral current (FCNC) processes. We find the current bound on
more constraining than
. The LEP limit on the lightest Higgs boson mass implies an important lower bound on tan β, which in turn limits the size of the new FCNC transitions. Remarkably, the combined analysis does not rule out large effects in mixing and we can easily accomodate the large CP phase in the
system which has recently been inferred from a global analysis of CDF and DØ data. The model predicts a particle spectrum which is different from the popular Constrained Minimal Supersymmetric Standard Model (CMSSM).
enforces heavy masses, typicallyabove1TeV,forthesfermionsofthedegeneratefirsttwogenerations. However, the ratio of the third-generation and first-generation sfermion masses is smaller than in the CMSSM and a (dominantly right-handed) stop with massbelow500GeV is possible.</description><identifier>ISSN: 1029-8479</identifier><identifier>EISSN: 1029-8479</identifier><identifier>DOI: 10.1007/JHEP06(2011)044</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer-Verlag</publisher><subject>Atmospheric models ; Classical and Quantum Gravitation ; Correlation analysis ; Elementary Particles ; Flavor (particle physics) ; Higgs bosons ; High energy physics ; Leptons ; Lower bounds ; Mathematical models ; Neutral currents ; Neutrinos ; Parameters ; Physics ; Physics and Astronomy ; Quantum Field Theories ; Quantum Field Theory ; Quantum Physics ; Quarks ; Relativity Theory ; Standard model (particle physics) ; String Theory ; Supersymmetry</subject><ispartof>The journal of high energy physics, 2011-06, Vol.2011 (6), Article 44</ispartof><rights>SISSA, Trieste, Italy 2011</rights><rights>SISSA, Trieste, Italy 2011.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c376t-348128208e9988deb78bfe0121f6d688312debe917207cd3178833decdadcd2b3</citedby><cites>FETCH-LOGICAL-c376t-348128208e9988deb78bfe0121f6d688312debe917207cd3178833decdadcd2b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/JHEP06(2011)044$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://doi.org/10.1007/JHEP06(2011)044$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27903,27904,41099,41467,42168,42536,51297,51554</link.rule.ids><linktorsrc>$$Uhttps://doi.org/10.1007/JHEP06(2011)044$$EView_record_in_Springer_Nature$$FView_record_in_$$GSpringer_Nature</linktorsrc></links><search><creatorcontrib>Girrbach, Jennifer</creatorcontrib><creatorcontrib>Jäger, Sebastian</creatorcontrib><creatorcontrib>Knopf, Markus</creatorcontrib><creatorcontrib>Martens, Waldemar</creatorcontrib><creatorcontrib>Nierste, Ulrich</creatorcontrib><creatorcontrib>Scherrer, Christian</creatorcontrib><creatorcontrib>Wiesenfeldt, Sören</creatorcontrib><title>Flavor physics in an SO(10) grand unified model</title><title>The journal of high energy physics</title><addtitle>J. High Energ. Phys</addtitle><description>In supersymmetric grand-unified models, the lepton mixing matrix can possibly affect flavor-changing transitions in the quark sector. We present a detailed analysis of a model proposed by Chang, Masiero and Murayama, in which the near-maximal atmospheric neutrino mixing angle governs large new
b
→
s
transitions. Relating the supersymmetric low-energy parameters to seven new parameters of this SO(10) GUT model, we perform a correlated study of several flavor-changing neutral current (FCNC) processes. We find the current bound on
more constraining than
. The LEP limit on the lightest Higgs boson mass implies an important lower bound on tan β, which in turn limits the size of the new FCNC transitions. Remarkably, the combined analysis does not rule out large effects in mixing and we can easily accomodate the large CP phase in the
system which has recently been inferred from a global analysis of CDF and DØ data. The model predicts a particle spectrum which is different from the popular Constrained Minimal Supersymmetric Standard Model (CMSSM).
enforces heavy masses, typicallyabove1TeV,forthesfermionsofthedegeneratefirsttwogenerations. However, the ratio of the third-generation and first-generation sfermion masses is smaller than in the CMSSM and a (dominantly right-handed) stop with massbelow500GeV is possible.</description><subject>Atmospheric models</subject><subject>Classical and Quantum Gravitation</subject><subject>Correlation analysis</subject><subject>Elementary Particles</subject><subject>Flavor (particle physics)</subject><subject>Higgs bosons</subject><subject>High energy physics</subject><subject>Leptons</subject><subject>Lower bounds</subject><subject>Mathematical models</subject><subject>Neutral currents</subject><subject>Neutrinos</subject><subject>Parameters</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Field Theories</subject><subject>Quantum Field Theory</subject><subject>Quantum Physics</subject><subject>Quarks</subject><subject>Relativity Theory</subject><subject>Standard model (particle physics)</subject><subject>String Theory</subject><subject>Supersymmetry</subject><issn>1029-8479</issn><issn>1029-8479</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNp1kMFLwzAYxYMoOKdnrwEv26H2-5LaJEcZm1MGE9RzaJt0dnRtTdbB_nszKujF0_d4vPc--BFyi3CPACJ-Wc5fIZ0wQJxCkpyREQJTkUyEOv-jL8mV91sAfEAFIxIv6uzQOtp9Hn1VeFo1NGvo23qCMKUblzWG9k1VVtbQXWtsfU0uyqz29ubnjsnHYv4-W0ar9dPz7HEVFVyk-4gnEplkIK1SUhqbC5mXFpBhmZpUSo4smFahYCAKw1EEjxtbmMwUhuV8TO6G3c61X731e71te9eEl5pxJVkiVZqEVDykCtd672ypO1ftMnfUCPpERQ9U9ImKDlRCA4aGD8lmY93v7n-Vb8ENYUE</recordid><startdate>20110601</startdate><enddate>20110601</enddate><creator>Girrbach, Jennifer</creator><creator>Jäger, Sebastian</creator><creator>Knopf, Markus</creator><creator>Martens, Waldemar</creator><creator>Nierste, Ulrich</creator><creator>Scherrer, Christian</creator><creator>Wiesenfeldt, Sören</creator><general>Springer-Verlag</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope></search><sort><creationdate>20110601</creationdate><title>Flavor physics in an SO(10) grand unified model</title><author>Girrbach, Jennifer ; 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b
→
s
transitions. Relating the supersymmetric low-energy parameters to seven new parameters of this SO(10) GUT model, we perform a correlated study of several flavor-changing neutral current (FCNC) processes. We find the current bound on
more constraining than
. The LEP limit on the lightest Higgs boson mass implies an important lower bound on tan β, which in turn limits the size of the new FCNC transitions. Remarkably, the combined analysis does not rule out large effects in mixing and we can easily accomodate the large CP phase in the
system which has recently been inferred from a global analysis of CDF and DØ data. The model predicts a particle spectrum which is different from the popular Constrained Minimal Supersymmetric Standard Model (CMSSM).
enforces heavy masses, typicallyabove1TeV,forthesfermionsofthedegeneratefirsttwogenerations. However, the ratio of the third-generation and first-generation sfermion masses is smaller than in the CMSSM and a (dominantly right-handed) stop with massbelow500GeV is possible.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer-Verlag</pub><doi>10.1007/JHEP06(2011)044</doi><oa>free_for_read</oa></addata></record> |
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subjects | Atmospheric models Classical and Quantum Gravitation Correlation analysis Elementary Particles Flavor (particle physics) Higgs bosons High energy physics Leptons Lower bounds Mathematical models Neutral currents Neutrinos Parameters Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum Physics Quarks Relativity Theory Standard model (particle physics) String Theory Supersymmetry |
title | Flavor physics in an SO(10) grand unified model |
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