Top-quark flavor-changing tqZ couplings and rare $$\Delta F=1$$ ΔF=1 processes
Abstract We study the impacts of anomalous tqZ couplings ($$q=u,c$$ q=u,c ), which lead to the $$t\rightarrow q Z$$ t→qZ decays, on low energy flavor physics. It is found that the tuZ-coupling effect can significantly affect the rare K and B decays, whereas the tcZ-coupling effect is small. Using th...
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doaj-41559531b9c34a92ab3e8051927366db2020-11-25T03:17:38ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-08-017981910.1140/epjc/s10052-019-7133-5Top-quark flavor-changing tqZ couplings and rare $$\Delta F=1$$ ΔF=1 processesChuan-Hung Chen0Takaaki Nomura1Department of Physics, National Cheng-Kung UniversitySchool of Physics, KIASAbstract We study the impacts of anomalous tqZ couplings ($$q=u,c$$ q=u,c ), which lead to the $$t\rightarrow q Z$$ t→qZ decays, on low energy flavor physics. It is found that the tuZ-coupling effect can significantly affect the rare K and B decays, whereas the tcZ-coupling effect is small. Using the ATLAS’s branching ratio (BR) upper bound of $$BR(t\rightarrow uZ) < 1.7\times 10^{-4}$$ BR(t→uZ)<1.7×10-4 , the influence of the anomalous tuZ-coupling on the rare decays can be found as follows: (a) The contribution to the Kaon direct CP violation can be up to $$Re(\epsilon '/\epsilon ) \lesssim 0.8 \times 10^{-3}$$ Re(ϵ′/ϵ)≲0.8×10-3 ; (b) $$BR(K^+\rightarrow \pi ^+ \nu {\bar{\nu }}) \lesssim 12 \times 10^{-11}$$ BR(K+→π+νν¯)≲12×10-11 and $$BR(K_L \rightarrow \pi ^0 \nu {\bar{\nu }})\lesssim 7.9 \times 10^{-11}$$ BR(KL→π0νν¯)≲7.9×10-11 ; (c) the BR for $$K_S \rightarrow \mu ^+ \mu ^-$$ KS→μ+μ- including the long-distance effect can be enhanced by $$11\%$$ 11% with respect to the standard model result, and (d) $$BR(B_d \rightarrow \mu ^+ \mu ^-) \lesssim 1.97 \times 10^{-10}$$ BR(Bd→μ+μ-)≲1.97×10-10 . In addition, although $$Re(\epsilon '/\epsilon )$$ Re(ϵ′/ϵ) cannot be synchronously enhanced with $$BR(K_L\rightarrow \pi ^0 \nu {\bar{\nu }})$$ BR(KL→π0νν¯) and $$BR(K_S\rightarrow \mu ^+ \mu ^-)$$ BR(KS→μ+μ-) in the same region of the CP-violating phase, the values of $$Re(\epsilon '/\epsilon )$$ Re(ϵ′/ϵ) , $$BR(K^+ \rightarrow \pi ^+ \nu {\bar{\nu }})$$ BR(K+→π+νν¯) , and $$BR(B_d \rightarrow \mu ^+ \mu ^-)$$ BR(Bd→μ+μ-) can be simultaneously increased.http://link.springer.com/article/10.1140/epjc/s10052-019-7133-5 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Chuan-Hung Chen Takaaki Nomura |
spellingShingle |
Chuan-Hung Chen Takaaki Nomura Top-quark flavor-changing tqZ couplings and rare $$\Delta F=1$$ ΔF=1 processes European Physical Journal C: Particles and Fields |
author_facet |
Chuan-Hung Chen Takaaki Nomura |
author_sort |
Chuan-Hung Chen |
title |
Top-quark flavor-changing tqZ couplings and rare $$\Delta F=1$$ ΔF=1 processes |
title_short |
Top-quark flavor-changing tqZ couplings and rare $$\Delta F=1$$ ΔF=1 processes |
title_full |
Top-quark flavor-changing tqZ couplings and rare $$\Delta F=1$$ ΔF=1 processes |
title_fullStr |
Top-quark flavor-changing tqZ couplings and rare $$\Delta F=1$$ ΔF=1 processes |
title_full_unstemmed |
Top-quark flavor-changing tqZ couplings and rare $$\Delta F=1$$ ΔF=1 processes |
title_sort |
top-quark flavor-changing tqz couplings and rare $$\delta f=1$$ δf=1 processes |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2019-08-01 |
description |
Abstract We study the impacts of anomalous tqZ couplings ($$q=u,c$$ q=u,c ), which lead to the $$t\rightarrow q Z$$ t→qZ decays, on low energy flavor physics. It is found that the tuZ-coupling effect can significantly affect the rare K and B decays, whereas the tcZ-coupling effect is small. Using the ATLAS’s branching ratio (BR) upper bound of $$BR(t\rightarrow uZ) < 1.7\times 10^{-4}$$ BR(t→uZ)<1.7×10-4 , the influence of the anomalous tuZ-coupling on the rare decays can be found as follows: (a) The contribution to the Kaon direct CP violation can be up to $$Re(\epsilon '/\epsilon ) \lesssim 0.8 \times 10^{-3}$$ Re(ϵ′/ϵ)≲0.8×10-3 ; (b) $$BR(K^+\rightarrow \pi ^+ \nu {\bar{\nu }}) \lesssim 12 \times 10^{-11}$$ BR(K+→π+νν¯)≲12×10-11 and $$BR(K_L \rightarrow \pi ^0 \nu {\bar{\nu }})\lesssim 7.9 \times 10^{-11}$$ BR(KL→π0νν¯)≲7.9×10-11 ; (c) the BR for $$K_S \rightarrow \mu ^+ \mu ^-$$ KS→μ+μ- including the long-distance effect can be enhanced by $$11\%$$ 11% with respect to the standard model result, and (d) $$BR(B_d \rightarrow \mu ^+ \mu ^-) \lesssim 1.97 \times 10^{-10}$$ BR(Bd→μ+μ-)≲1.97×10-10 . In addition, although $$Re(\epsilon '/\epsilon )$$ Re(ϵ′/ϵ) cannot be synchronously enhanced with $$BR(K_L\rightarrow \pi ^0 \nu {\bar{\nu }})$$ BR(KL→π0νν¯) and $$BR(K_S\rightarrow \mu ^+ \mu ^-)$$ BR(KS→μ+μ-) in the same region of the CP-violating phase, the values of $$Re(\epsilon '/\epsilon )$$ Re(ϵ′/ϵ) , $$BR(K^+ \rightarrow \pi ^+ \nu {\bar{\nu }})$$ BR(K+→π+νν¯) , and $$BR(B_d \rightarrow \mu ^+ \mu ^-)$$ BR(Bd→μ+μ-) can be simultaneously increased. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-019-7133-5 |
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