The Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil in HQET

Abstract In this paper we discuss the Standard Model and new physics sensitivity of the Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil, where ℓ ± are massive leptons and N K ¯ = pK −...

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Main Authors: Diganta Das, Jaydeb Das
Format: Article
Language:English
Published: SpringerOpen 2020-07-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP07(2020)002
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spelling doaj-0823f543be2e493d87d6bd129394fbc82020-11-25T03:07:24ZengSpringerOpenJournal of High Energy Physics1029-84792020-07-012020712910.1007/JHEP07(2020)002The Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil in HQETDiganta Das0Jaydeb Das1Department of Physics and Astrophysics, University of DelhiDepartment of Physics and Astrophysics, University of DelhiAbstract In this paper we discuss the Standard Model and new physics sensitivity of the Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil, where ℓ ± are massive leptons and N K ¯ = pK − n K ¯ 0 $$ N\overline{K}=\left\{{pK}^{-},n{\overline{K}}^0\right\} $$ . We provide a full angular distribution with a set of operators that includes the Standard Model operators and their chirality flipped counterparts, and new scalar and pseudo-scalar operators. The resulting angular distribution allows us to construct observables that we study in the Standard Model and in model-independent new physics scenarios. To reduce the hadronic effects emanating from the Λ b → Λ* (1520) transition form factors, we exploit the Heavy Quark Effective theory framework valid at low Λ ∗ (1520) recoil, i.e., large dilepton invariant mass squared q 2 ∼ O m b 2 $$ {q}^2\sim \mathcal{O}\left({m}_b^2\right) $$ . Working to the leading order in 1/m b and including O α s $$ \mathcal{O}\left({\alpha}_s\right) $$ corrections, we compute the ‘improved Isgur-Wise relations’ between the form factors. The relations correlate the form factors and thereby allow the description of this decay at the low-recoil region with a smaller number of independent form factors.http://link.springer.com/article/10.1007/JHEP07(2020)002Beyond Standard ModelHeavy Quark Physics
collection DOAJ
language English
format Article
sources DOAJ
author Diganta Das
Jaydeb Das
spellingShingle Diganta Das
Jaydeb Das
The Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil in HQET
Journal of High Energy Physics
Beyond Standard Model
Heavy Quark Physics
author_facet Diganta Das
Jaydeb Das
author_sort Diganta Das
title The Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil in HQET
title_short The Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil in HQET
title_full The Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil in HQET
title_fullStr The Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil in HQET
title_full_unstemmed The Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil in HQET
title_sort λ b → λ ∗ 1520 → n k ¯ ℓ + ℓ − $$ {\lambda}_b\to {\lambda}^{\ast }(1520)\left(\to n\overline{k}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil in hqet
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2020-07-01
description Abstract In this paper we discuss the Standard Model and new physics sensitivity of the Λ b → Λ ∗ 1520 → N K ¯ ℓ + ℓ − $$ {\Lambda}_b\to {\Lambda}^{\ast }(1520)\left(\to N\overline{K}\right){\mathrm{\ell}}^{+}{\mathrm{\ell}}^{-} $$ decay at low-recoil, where ℓ ± are massive leptons and N K ¯ = pK − n K ¯ 0 $$ N\overline{K}=\left\{{pK}^{-},n{\overline{K}}^0\right\} $$ . We provide a full angular distribution with a set of operators that includes the Standard Model operators and their chirality flipped counterparts, and new scalar and pseudo-scalar operators. The resulting angular distribution allows us to construct observables that we study in the Standard Model and in model-independent new physics scenarios. To reduce the hadronic effects emanating from the Λ b → Λ* (1520) transition form factors, we exploit the Heavy Quark Effective theory framework valid at low Λ ∗ (1520) recoil, i.e., large dilepton invariant mass squared q 2 ∼ O m b 2 $$ {q}^2\sim \mathcal{O}\left({m}_b^2\right) $$ . Working to the leading order in 1/m b and including O α s $$ \mathcal{O}\left({\alpha}_s\right) $$ corrections, we compute the ‘improved Isgur-Wise relations’ between the form factors. The relations correlate the form factors and thereby allow the description of this decay at the low-recoil region with a smaller number of independent form factors.
topic Beyond Standard Model
Heavy Quark Physics
url http://link.springer.com/article/10.1007/JHEP07(2020)002
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