Updated NNLO QCD predictions for the weak radiative B-meson decays
Weak radiative decays of the B mesons belong to the most important flavor changing processes that provide constraints on physics at the TeV scale. In the derivation of such constraints, accurate standard model predictions for the inclusive branching ratios play a crucial role. In the current Letter...
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creator | Misiak, M Asatrian, H M Boughezal, R Czakon, M Ewerth, T Ferroglia, A Fiedler, P Gambino, P Greub, C Haisch, U Huber, T Kaminski, M Ossola, G Poradzinski, M Rehman, A Schutzmeier, T Steinhauser, M Virto, J |
description | Weak radiative decays of the B mesons belong to the most important flavor changing processes that provide constraints on physics at the TeV scale. In the derivation of such constraints, accurate standard model predictions for the inclusive branching ratios play a crucial role. In the current Letter we present an update of these predictions, incorporating all our results for the O(alpha_s^2) and lower-order perturbative corrections that have been calculated after 2006. New estimates of nonperturbative effects are taken into account, too. For the CP- and isospin-averaged branching ratios, we find B_{s gamma} = (3.36 +_ 0.23) * 10^-4 and B_{d gamma} = 1.73^{+0.12}_{-0.22} * 10^-5, for E_gamma > 1.6GeV. Both results remain in agreement with the current experimental averages. Normalizing their sum to the inclusive semileptonic branching ratio, we obtain R_gamma = ( B_{s gamma} + B_{d gamma})/B_{c l nu} = (3.31 +_ 0.22) * 10^-3. A new bound from B_{s gamma} on the charged Higgs boson mass in the two-Higgs-doublet-model II reads M_{H^+} > 480 GeV at 95%C.L. |
doi_str_mv | 10.48550/arxiv.1503.01789 |
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In the derivation of such constraints, accurate standard model predictions for the inclusive branching ratios play a crucial role. In the current Letter we present an update of these predictions, incorporating all our results for the O(alpha_s^2) and lower-order perturbative corrections that have been calculated after 2006. New estimates of nonperturbative effects are taken into account, too. For the CP- and isospin-averaged branching ratios, we find B_{s gamma} = (3.36 +_ 0.23) * 10^-4 and B_{d gamma} = 1.73^{+0.12}_{-0.22} * 10^-5, for E_gamma > 1.6GeV. Both results remain in agreement with the current experimental averages. Normalizing their sum to the inclusive semileptonic branching ratio, we obtain R_gamma = ( B_{s gamma} + B_{d gamma})/B_{c l nu} = (3.31 +_ 0.22) * 10^-3. A new bound from B_{s gamma} on the charged Higgs boson mass in the two-Higgs-doublet-model II reads M_{H^+} > 480 GeV at 95%C.L.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1503.01789</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Constraint modelling ; Higgs bosons ; Mesons ; Normalizing ; Physics - High Energy Physics - Experiment ; Physics - High Energy Physics - Phenomenology ; Quantum chromodynamics ; Quarks ; Standard model (particle physics)</subject><ispartof>arXiv.org, 2015-06</ispartof><rights>2015. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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In the derivation of such constraints, accurate standard model predictions for the inclusive branching ratios play a crucial role. In the current Letter we present an update of these predictions, incorporating all our results for the O(alpha_s^2) and lower-order perturbative corrections that have been calculated after 2006. New estimates of nonperturbative effects are taken into account, too. For the CP- and isospin-averaged branching ratios, we find B_{s gamma} = (3.36 +_ 0.23) * 10^-4 and B_{d gamma} = 1.73^{+0.12}_{-0.22} * 10^-5, for E_gamma > 1.6GeV. Both results remain in agreement with the current experimental averages. Normalizing their sum to the inclusive semileptonic branching ratio, we obtain R_gamma = ( B_{s gamma} + B_{d gamma})/B_{c l nu} = (3.31 +_ 0.22) * 10^-3. A new bound from B_{s gamma} on the charged Higgs boson mass in the two-Higgs-doublet-model II reads M_{H^+} > 480 GeV at 95%C.L.</description><subject>Constraint modelling</subject><subject>Higgs bosons</subject><subject>Mesons</subject><subject>Normalizing</subject><subject>Physics - High Energy Physics - Experiment</subject><subject>Physics - High Energy Physics - Phenomenology</subject><subject>Quantum chromodynamics</subject><subject>Quarks</subject><subject>Standard model (particle physics)</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotj9FLwzAYxIMgOOb-AJ8M-NyaL2nS5NFVnULZEOZz-WxSzHRtTbrp_nvr5tPdwXHcj5ArYGmmpWS3GH78PgXJRMog1-aMTLgQkOiM8wsyi3HDGOMq51KKCZm_9hYHZ-lyWa7oS3FP--CsrwfftZE2XaDDu6PfDj9oQOtx8HtH58nWxa6l1tV4iJfkvMHP6Gb_OiXrx4d18ZSUq8VzcVcmKDkkEhxXSnFZg5P6DTOdOaGE5Y02aDQDpXQOVhrbSKGYAZ2JMXGNozOAYkquT7NHwKoPfovhUP2BVkfQsXFzavSh-9q5OFSbbhfa8VPFmRYMxlUQvw8wUpc</recordid><startdate>20150609</startdate><enddate>20150609</enddate><creator>Misiak, M</creator><creator>Asatrian, H M</creator><creator>Boughezal, R</creator><creator>Czakon, M</creator><creator>Ewerth, T</creator><creator>Ferroglia, A</creator><creator>Fiedler, P</creator><creator>Gambino, P</creator><creator>Greub, C</creator><creator>Haisch, U</creator><creator>Huber, T</creator><creator>Kaminski, M</creator><creator>Ossola, G</creator><creator>Poradzinski, M</creator><creator>Rehman, A</creator><creator>Schutzmeier, T</creator><creator>Steinhauser, M</creator><creator>Virto, J</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20150609</creationdate><title>Updated NNLO QCD predictions for the weak radiative B-meson decays</title><author>Misiak, M ; Asatrian, H M ; Boughezal, R ; Czakon, M ; Ewerth, T ; Ferroglia, A ; Fiedler, P ; Gambino, P ; Greub, C ; Haisch, U ; Huber, T ; Kaminski, M ; Ossola, G ; Poradzinski, M ; Rehman, A ; Schutzmeier, T ; Steinhauser, M ; Virto, J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a521-51e266625c1e58ba484e363d2f89a980166871d59df536091843d5928a18491a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Constraint modelling</topic><topic>Higgs bosons</topic><topic>Mesons</topic><topic>Normalizing</topic><topic>Physics - High Energy Physics - Experiment</topic><topic>Physics - High Energy Physics - Phenomenology</topic><topic>Quantum chromodynamics</topic><topic>Quarks</topic><topic>Standard model (particle physics)</topic><toplevel>online_resources</toplevel><creatorcontrib>Misiak, M</creatorcontrib><creatorcontrib>Asatrian, H M</creatorcontrib><creatorcontrib>Boughezal, R</creatorcontrib><creatorcontrib>Czakon, M</creatorcontrib><creatorcontrib>Ewerth, T</creatorcontrib><creatorcontrib>Ferroglia, A</creatorcontrib><creatorcontrib>Fiedler, P</creatorcontrib><creatorcontrib>Gambino, P</creatorcontrib><creatorcontrib>Greub, C</creatorcontrib><creatorcontrib>Haisch, U</creatorcontrib><creatorcontrib>Huber, T</creatorcontrib><creatorcontrib>Kaminski, M</creatorcontrib><creatorcontrib>Ossola, G</creatorcontrib><creatorcontrib>Poradzinski, M</creatorcontrib><creatorcontrib>Rehman, A</creatorcontrib><creatorcontrib>Schutzmeier, T</creatorcontrib><creatorcontrib>Steinhauser, M</creatorcontrib><creatorcontrib>Virto, J</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Misiak, M</au><au>Asatrian, H M</au><au>Boughezal, R</au><au>Czakon, M</au><au>Ewerth, T</au><au>Ferroglia, A</au><au>Fiedler, P</au><au>Gambino, P</au><au>Greub, C</au><au>Haisch, U</au><au>Huber, T</au><au>Kaminski, M</au><au>Ossola, G</au><au>Poradzinski, M</au><au>Rehman, A</au><au>Schutzmeier, T</au><au>Steinhauser, M</au><au>Virto, J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Updated NNLO QCD predictions for the weak radiative B-meson decays</atitle><jtitle>arXiv.org</jtitle><date>2015-06-09</date><risdate>2015</risdate><eissn>2331-8422</eissn><abstract>Weak radiative decays of the B mesons belong to the most important flavor changing processes that provide constraints on physics at the TeV scale. In the derivation of such constraints, accurate standard model predictions for the inclusive branching ratios play a crucial role. In the current Letter we present an update of these predictions, incorporating all our results for the O(alpha_s^2) and lower-order perturbative corrections that have been calculated after 2006. New estimates of nonperturbative effects are taken into account, too. For the CP- and isospin-averaged branching ratios, we find B_{s gamma} = (3.36 +_ 0.23) * 10^-4 and B_{d gamma} = 1.73^{+0.12}_{-0.22} * 10^-5, for E_gamma > 1.6GeV. Both results remain in agreement with the current experimental averages. Normalizing their sum to the inclusive semileptonic branching ratio, we obtain R_gamma = ( B_{s gamma} + B_{d gamma})/B_{c l nu} = (3.31 +_ 0.22) * 10^-3. A new bound from B_{s gamma} on the charged Higgs boson mass in the two-Higgs-doublet-model II reads M_{H^+} > 480 GeV at 95%C.L.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1503.01789</doi><oa>free_for_read</oa></addata></record> |
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subjects | Constraint modelling Higgs bosons Mesons Normalizing Physics - High Energy Physics - Experiment Physics - High Energy Physics - Phenomenology Quantum chromodynamics Quarks Standard model (particle physics) |
title | Updated NNLO QCD predictions for the weak radiative B-meson decays |
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