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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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 |
work_keys_str_mv |
AT hrachiamasatrian exactnlomatchingandanalyticityinbsll AT christophgreub exactnlomatchingandanalyticityinbsll AT javiervirto exactnlomatchingandanalyticityinbsll |
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1724934723501817856 |