Heavy quarkonium production through the top quark rare decays via the channels involving flavor changing neutral currents

Abstract In the paper, we discuss the possibility of observation of heavy quarkoniums via the processes involving flavor changing neutral currents (FCNC). More explicitly, we systematically calculate the production of heavy charmonium and $$(c{\bar{b}})$$ (cb¯) -quarkonium through the top quark semi...

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Main Authors: Juan-Juan Niu, Lei Guo, Hong-Hao Ma, Shao-Ming Wang
Format: Article
Language:English
Published: SpringerOpen 2018-08-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-018-6126-0
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spelling doaj-d1c14b15eed34f13ba9b633f0c53301a2020-11-25T02:07:42ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522018-08-017881910.1140/epjc/s10052-018-6126-0Heavy quarkonium production through the top quark rare decays via the channels involving flavor changing neutral currentsJuan-Juan Niu0Lei Guo1Hong-Hao Ma2Shao-Ming Wang3Department of Physics, Chongqing UniversityDepartment of Physics, Chongqing UniversityFaculdade de Engenharia de Guaratinguetá, Universidade Estadual PaulistaDepartment of Physics, Chongqing UniversityAbstract In the paper, we discuss the possibility of observation of heavy quarkoniums via the processes involving flavor changing neutral currents (FCNC). More explicitly, we systematically calculate the production of heavy charmonium and $$(c{\bar{b}})$$ (cb¯) -quarkonium through the top quark semi-exclusive rare FCNC decays in the framework of the non-relativistic QCD (NRQCD) factorization theory. Our results show that the total decay widths $$\Gamma _{t\rightarrow \eta _c} =1.20^{+1.04+1.14}_{-0.51-0.45}\times 10^{-16}$$ Γt→ηc=1.20-0.51-0.45+1.04+1.14×10-16 GeV, $$\Gamma _{t\rightarrow J/\psi } =1.37^{+1.03+1.30}_{-0.51-0.51}\times 10^{-16}$$ Γt→J/ψ=1.37-0.51-0.51+1.03+1.30×10-16 GeV, $$\Gamma _{t\rightarrow B_c}=2.06^{+0.17+0.91}_{-0.17-0.54}\times 10^{-18}$$ Γt→Bc=2.06-0.17-0.54+0.17+0.91×10-18 GeV, and $$\Gamma _{t\rightarrow B^*_c}=6.27^{+0.63+2.78}_{-0.62-1.64}\times 10^{-18}$$ Γt→Bc∗=6.27-0.62-1.64+0.63+2.78×10-18 GeV, where the uncertainties are from variation of quark masses and renormalization scales. Even though the decay widths are small, it is important to make a systematic study on the production of charmonium and $$(c{\bar{b}})$$ (cb¯) -quarkonium through the top-quark decays via FCNC in the Standard Model, which will provide useful guidance for future new physics research from the heavy quarkonium involved processes.http://link.springer.com/article/10.1140/epjc/s10052-018-6126-0
collection DOAJ
language English
format Article
sources DOAJ
author Juan-Juan Niu
Lei Guo
Hong-Hao Ma
Shao-Ming Wang
spellingShingle Juan-Juan Niu
Lei Guo
Hong-Hao Ma
Shao-Ming Wang
Heavy quarkonium production through the top quark rare decays via the channels involving flavor changing neutral currents
European Physical Journal C: Particles and Fields
author_facet Juan-Juan Niu
Lei Guo
Hong-Hao Ma
Shao-Ming Wang
author_sort Juan-Juan Niu
title Heavy quarkonium production through the top quark rare decays via the channels involving flavor changing neutral currents
title_short Heavy quarkonium production through the top quark rare decays via the channels involving flavor changing neutral currents
title_full Heavy quarkonium production through the top quark rare decays via the channels involving flavor changing neutral currents
title_fullStr Heavy quarkonium production through the top quark rare decays via the channels involving flavor changing neutral currents
title_full_unstemmed Heavy quarkonium production through the top quark rare decays via the channels involving flavor changing neutral currents
title_sort heavy quarkonium production through the top quark rare decays via the channels involving flavor changing neutral currents
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2018-08-01
description Abstract In the paper, we discuss the possibility of observation of heavy quarkoniums via the processes involving flavor changing neutral currents (FCNC). More explicitly, we systematically calculate the production of heavy charmonium and $$(c{\bar{b}})$$ (cb¯) -quarkonium through the top quark semi-exclusive rare FCNC decays in the framework of the non-relativistic QCD (NRQCD) factorization theory. Our results show that the total decay widths $$\Gamma _{t\rightarrow \eta _c} =1.20^{+1.04+1.14}_{-0.51-0.45}\times 10^{-16}$$ Γt→ηc=1.20-0.51-0.45+1.04+1.14×10-16 GeV, $$\Gamma _{t\rightarrow J/\psi } =1.37^{+1.03+1.30}_{-0.51-0.51}\times 10^{-16}$$ Γt→J/ψ=1.37-0.51-0.51+1.03+1.30×10-16 GeV, $$\Gamma _{t\rightarrow B_c}=2.06^{+0.17+0.91}_{-0.17-0.54}\times 10^{-18}$$ Γt→Bc=2.06-0.17-0.54+0.17+0.91×10-18 GeV, and $$\Gamma _{t\rightarrow B^*_c}=6.27^{+0.63+2.78}_{-0.62-1.64}\times 10^{-18}$$ Γt→Bc∗=6.27-0.62-1.64+0.63+2.78×10-18 GeV, where the uncertainties are from variation of quark masses and renormalization scales. Even though the decay widths are small, it is important to make a systematic study on the production of charmonium and $$(c{\bar{b}})$$ (cb¯) -quarkonium through the top-quark decays via FCNC in the Standard Model, which will provide useful guidance for future new physics research from the heavy quarkonium involved processes.
url http://link.springer.com/article/10.1140/epjc/s10052-018-6126-0
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