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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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 |
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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 |
work_keys_str_mv |
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