Determination of |Vcb| using N3LO perturbative corrections to Γ(B → Xcℓν) and 1S masses

We determine |Vcb| using the third-order perturbative series for the inclusive semileptonic B decay width and for the masses of the bottomonium 1S states. We use the masses of ηb(1S) and ϒ(1S) as short-distance masses and point out that there is a sizable difference of |Vcb| between the two 1S mass...

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Main Authors: Yuuki Hayashi, Yukinari Sumino, Hiromasa Takaura
Format: Article
Language:English
Published: Elsevier 2022-06-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269322002027
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author Yuuki Hayashi
Yukinari Sumino
Hiromasa Takaura
author_facet Yuuki Hayashi
Yukinari Sumino
Hiromasa Takaura
author_sort Yuuki Hayashi
collection DOAJ
description We determine |Vcb| using the third-order perturbative series for the inclusive semileptonic B decay width and for the masses of the bottomonium 1S states. We use the masses of ηb(1S) and ϒ(1S) as short-distance masses and point out that there is a sizable difference of |Vcb| between the two 1S mass schemes. This is the dominant error of our determination and stems from insufficiency to describe theoretically the observed mass splitting of the bottomonium 1S states. We also study the significance of the O(ΛMS‾2) non-perturbative effects in HQET with respect to the current perturbative accuracy. Our result |Vcb|=0.0425(11) is consistent with the PDG value determined from the inclusive decays and has a slightly larger error.
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spelling doaj.art-11fdce1d94454bc8b7ba506bedf66d7a2022-12-22T02:11:37ZengElsevierPhysics Letters B0370-26932022-06-01829137068Determination of |Vcb| using N3LO perturbative corrections to Γ(B → Xcℓν) and 1S massesYuuki Hayashi0Yukinari Sumino1Hiromasa Takaura2Department of Physics, Tohoku University, Sendai, 980–8578, JapanDepartment of Physics, Tohoku University, Sendai, 980–8578, JapanTheory Center, KEK, Tsukuba, Ibaraki 305-0801, Japan; Corresponding author.We determine |Vcb| using the third-order perturbative series for the inclusive semileptonic B decay width and for the masses of the bottomonium 1S states. We use the masses of ηb(1S) and ϒ(1S) as short-distance masses and point out that there is a sizable difference of |Vcb| between the two 1S mass schemes. This is the dominant error of our determination and stems from insufficiency to describe theoretically the observed mass splitting of the bottomonium 1S states. We also study the significance of the O(ΛMS‾2) non-perturbative effects in HQET with respect to the current perturbative accuracy. Our result |Vcb|=0.0425(11) is consistent with the PDG value determined from the inclusive decays and has a slightly larger error.http://www.sciencedirect.com/science/article/pii/S0370269322002027
spellingShingle Yuuki Hayashi
Yukinari Sumino
Hiromasa Takaura
Determination of |Vcb| using N3LO perturbative corrections to Γ(B → Xcℓν) and 1S masses
Physics Letters B
title Determination of |Vcb| using N3LO perturbative corrections to Γ(B → Xcℓν) and 1S masses
title_full Determination of |Vcb| using N3LO perturbative corrections to Γ(B → Xcℓν) and 1S masses
title_fullStr Determination of |Vcb| using N3LO perturbative corrections to Γ(B → Xcℓν) and 1S masses
title_full_unstemmed Determination of |Vcb| using N3LO perturbative corrections to Γ(B → Xcℓν) and 1S masses
title_short Determination of |Vcb| using N3LO perturbative corrections to Γ(B → Xcℓν) and 1S masses
title_sort determination of vcb using n3lo perturbative corrections to γ b   xclν and 1s masses
url http://www.sciencedirect.com/science/article/pii/S0370269322002027
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