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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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 |
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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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