Exact NLO matching and analyticity in b → sℓℓ

Abstract Exclusive rare decays mediated by b → sℓℓ transitions receive contributions from four-quark operators that cannot be naively expressed in terms of local form factors. Instead, one needs to calculate a matrix element of a bilocal operator. In certain kinematic regions, this bilocal operator...

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Main Authors: Hrachia M. Asatrian, Christoph Greub, Javier Virto
Format: Article
Language:English
Published: SpringerOpen 2020-04-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP04(2020)012
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spelling doaj-f74b87d070e54a88a2b3366c8b56b0712020-11-25T02:06:17ZengSpringerOpenJournal of High Energy Physics1029-84792020-04-012020413510.1007/JHEP04(2020)012Exact NLO matching and analyticity in b → sℓℓHrachia M. Asatrian0Christoph Greub1Javier Virto2Yerevan Physics InstituteAlbert Einstein Center for Fundamental Physics, Institute for Theoretical Physics, University of BernDepartament de Física Quàntica i Astrofísica, Institut de Cìencies del Cosmos, Universitat de BarcelonaAbstract Exclusive rare decays mediated by b → sℓℓ transitions receive contributions from four-quark operators that cannot be naively expressed in terms of local form factors. Instead, one needs to calculate a matrix element of a bilocal operator. In certain kinematic regions, this bilocal operator obeys some type of Operator Product Expansion, with coefficients that can be calculated in perturbation theory. We review the formalism and, focusing on the dominant SM operators O 1,2, we perform an improved calculation of the NLO matching for the leading dimension-three operators. This calculation is performed completely analytically in the two relevant mass scales (charm-quark mass mc and dilepton squared mass q 2), and we pay particular attention to the analytic continuation in the complex q 2 plane. This allows for the first time to study the analytic structure of the non-local form factors at NLO, and to calculate the OPE coefficients far below q 2 = 0, say q 2 < ~ − 10 GeV 2 $$ {q}^2\underset{\sim }{<}-10{\mathrm{GeV}}^2 $$ . We also provide explicitly the contributions proportional to different charge factors, which obey separate dispersion relations.http://link.springer.com/article/10.1007/JHEP04(2020)012Beyond Standard ModelEffective Field TheoriesHeavy Quark Physics
collection DOAJ
language English
format Article
sources DOAJ
author Hrachia M. Asatrian
Christoph Greub
Javier Virto
spellingShingle Hrachia M. Asatrian
Christoph Greub
Javier Virto
Exact NLO matching and analyticity in b → sℓℓ
Journal of High Energy Physics
Beyond Standard Model
Effective Field Theories
Heavy Quark Physics
author_facet Hrachia M. Asatrian
Christoph Greub
Javier Virto
author_sort Hrachia M. Asatrian
title Exact NLO matching and analyticity in b → sℓℓ
title_short Exact NLO matching and analyticity in b → sℓℓ
title_full Exact NLO matching and analyticity in b → sℓℓ
title_fullStr Exact NLO matching and analyticity in b → sℓℓ
title_full_unstemmed Exact NLO matching and analyticity in b → sℓℓ
title_sort exact nlo matching and analyticity in b → sℓℓ
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2020-04-01
description Abstract Exclusive rare decays mediated by b → sℓℓ transitions receive contributions from four-quark operators that cannot be naively expressed in terms of local form factors. Instead, one needs to calculate a matrix element of a bilocal operator. In certain kinematic regions, this bilocal operator obeys some type of Operator Product Expansion, with coefficients that can be calculated in perturbation theory. We review the formalism and, focusing on the dominant SM operators O 1,2, we perform an improved calculation of the NLO matching for the leading dimension-three operators. This calculation is performed completely analytically in the two relevant mass scales (charm-quark mass mc and dilepton squared mass q 2), and we pay particular attention to the analytic continuation in the complex q 2 plane. This allows for the first time to study the analytic structure of the non-local form factors at NLO, and to calculate the OPE coefficients far below q 2 = 0, say q 2 < ~ − 10 GeV 2 $$ {q}^2\underset{\sim }{<}-10{\mathrm{GeV}}^2 $$ . We also provide explicitly the contributions proportional to different charge factors, which obey separate dispersion relations.
topic Beyond Standard Model
Effective Field Theories
Heavy Quark Physics
url http://link.springer.com/article/10.1007/JHEP04(2020)012
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