Determinations of the form factors of semileptonic $$D\rightarrow K$$ D→K decays and leptoquark constraints

Abstract By analyzing all existing measurements for $$ D\rightarrow K \ell ^+ \nu _{\ell } $$ D→Kℓ+νℓ ($$\ell =e,\ \mu $$ ℓ=e,μ ) decays, we find that the determinations of both the vector form factor $$f_+^K(q^2)$$ f+K(q2) and scalar form factor $$f_0^K(q^2)$$ f0K(q2) for semileptonic $$D\rightarro...

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Main Authors: Jian Zhang, Chong-Xing Yue, Chun-Hua Li
Format: Article
Language:English
Published: SpringerOpen 2018-08-01
Series:European Physical Journal C: Particles and Fields
Subjects:
.
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-018-6184-3
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author Jian Zhang
Chong-Xing Yue
Chun-Hua Li
author_facet Jian Zhang
Chong-Xing Yue
Chun-Hua Li
author_sort Jian Zhang
collection DOAJ
description Abstract By analyzing all existing measurements for $$ D\rightarrow K \ell ^+ \nu _{\ell } $$ D→Kℓ+νℓ ($$\ell =e,\ \mu $$ ℓ=e,μ ) decays, we find that the determinations of both the vector form factor $$f_+^K(q^2)$$ f+K(q2) and scalar form factor $$f_0^K(q^2)$$ f0K(q2) for semileptonic $$D\rightarrow K$$ D→K decays from these measurements are feasible. By taking the parameterization of the one order series expansion of the $$f_+^K(q^2)$$ f+K(q2) and $$f_0^K(q^2)$$ f0K(q2) , $$f_+^K(0)|V_{cs}|$$ f+K(0)|Vcs| is determined to be $$0.7182\pm 0.0029$$ 0.7182±0.0029 , and the shape parameters of $$f_+^K(q^2)$$ f+K(q2) and $$f_0^K(q^2)$$ f0K(q2) are $$r_{+1}=-2.16\pm 0.007$$ r+1=-2.16±0.007 and $$r_{01}=0.89\pm 3.27$$ r01=0.89±3.27 , respectively. Combining with the average $$f_+^K(0)$$ f+K(0) of $$N_f=2+1$$ Nf=2+1 and $$N_f=2+1+1$$ Nf=2+1+1 lattice calculaltion, the $$|V_{cs}|$$ |Vcs| is extracted to be $$0.964\pm 0.004\pm 0.019$$ 0.964±0.004±0.019 where the first error is experimental and the second theoretical. Alternatively, the $$f_+^K(0)$$ f+K(0) is extracted to be $$0.7377\pm 0.003\pm 0.000$$ 0.7377±0.003±0.000 by taking the $$|V_{cs}|$$ |Vcs| as the value from the global fit with the unitarity constraint of the CKM matrix. Moreover, using the obtained form factors by $$N_f=2+1+1$$ Nf=2+1+1 lattice QCD, we re-analyze these measurements in the context of new physics. Constraints on scalar leptoquarks are obtained for different final states of semileptonic $$D \rightarrow K$$ D→K decays.
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spelling doaj.art-0d73f52a12b04f3c9d9332c445c531f12022-12-21T17:57:16ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522018-08-0178911310.1140/epjc/s10052-018-6184-3Determinations of the form factors of semileptonic $$D\rightarrow K$$ D→K decays and leptoquark constraintsJian Zhang0Chong-Xing Yue1Chun-Hua Li2School of Physics and Electronic Technology, Liaoning Normal UniversitySchool of Physics and Electronic Technology, Liaoning Normal UniversitySchool of Physics and Electronic Technology, Liaoning Normal UniversityAbstract By analyzing all existing measurements for $$ D\rightarrow K \ell ^+ \nu _{\ell } $$ D→Kℓ+νℓ ($$\ell =e,\ \mu $$ ℓ=e,μ ) decays, we find that the determinations of both the vector form factor $$f_+^K(q^2)$$ f+K(q2) and scalar form factor $$f_0^K(q^2)$$ f0K(q2) for semileptonic $$D\rightarrow K$$ D→K decays from these measurements are feasible. By taking the parameterization of the one order series expansion of the $$f_+^K(q^2)$$ f+K(q2) and $$f_0^K(q^2)$$ f0K(q2) , $$f_+^K(0)|V_{cs}|$$ f+K(0)|Vcs| is determined to be $$0.7182\pm 0.0029$$ 0.7182±0.0029 , and the shape parameters of $$f_+^K(q^2)$$ f+K(q2) and $$f_0^K(q^2)$$ f0K(q2) are $$r_{+1}=-2.16\pm 0.007$$ r+1=-2.16±0.007 and $$r_{01}=0.89\pm 3.27$$ r01=0.89±3.27 , respectively. Combining with the average $$f_+^K(0)$$ f+K(0) of $$N_f=2+1$$ Nf=2+1 and $$N_f=2+1+1$$ Nf=2+1+1 lattice calculaltion, the $$|V_{cs}|$$ |Vcs| is extracted to be $$0.964\pm 0.004\pm 0.019$$ 0.964±0.004±0.019 where the first error is experimental and the second theoretical. Alternatively, the $$f_+^K(0)$$ f+K(0) is extracted to be $$0.7377\pm 0.003\pm 0.000$$ 0.7377±0.003±0.000 by taking the $$|V_{cs}|$$ |Vcs| as the value from the global fit with the unitarity constraint of the CKM matrix. Moreover, using the obtained form factors by $$N_f=2+1+1$$ Nf=2+1+1 lattice QCD, we re-analyze these measurements in the context of new physics. Constraints on scalar leptoquarks are obtained for different final states of semileptonic $$D \rightarrow K$$ D→K decays.http://link.springer.com/article/10.1140/epjc/s10052-018-6184-3.
spellingShingle Jian Zhang
Chong-Xing Yue
Chun-Hua Li
Determinations of the form factors of semileptonic $$D\rightarrow K$$ D→K decays and leptoquark constraints
European Physical Journal C: Particles and Fields
.
title Determinations of the form factors of semileptonic $$D\rightarrow K$$ D→K decays and leptoquark constraints
title_full Determinations of the form factors of semileptonic $$D\rightarrow K$$ D→K decays and leptoquark constraints
title_fullStr Determinations of the form factors of semileptonic $$D\rightarrow K$$ D→K decays and leptoquark constraints
title_full_unstemmed Determinations of the form factors of semileptonic $$D\rightarrow K$$ D→K decays and leptoquark constraints
title_short Determinations of the form factors of semileptonic $$D\rightarrow K$$ D→K decays and leptoquark constraints
title_sort determinations of the form factors of semileptonic d rightarrow k d k decays and leptoquark constraints
topic .
url http://link.springer.com/article/10.1140/epjc/s10052-018-6184-3
work_keys_str_mv AT jianzhang determinationsoftheformfactorsofsemileptonicdrightarrowkdkdecaysandleptoquarkconstraints
AT chongxingyue determinationsoftheformfactorsofsemileptonicdrightarrowkdkdecaysandleptoquarkconstraints
AT chunhuali determinationsoftheformfactorsofsemileptonicdrightarrowkdkdecaysandleptoquarkconstraints