Looking for new physics via semi-leptonic and leptonic rare decays of D and Ds
It is well recognized that looking for new physics at lower energy colliders is a path wnmn is complemen- tary to high energy machines such as the LHC. Using the large volume of data collected by BESIII, we may have a unique opportunity to tackle this. In this paper we calculate the branching ratios...
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Published in | 中国物理C:英文版 Vol. 41; no. 9; pp. 59 - 69 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
01.09.2017
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Subjects | |
Online Access | Get full text |
ISSN | 1674-1137 0254-3052 |
DOI | 10.1088/1674-1137/41/9/093107 |
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Summary: | It is well recognized that looking for new physics at lower energy colliders is a path wnmn is complemen- tary to high energy machines such as the LHC. Using the large volume of data collected by BESIII, we may have a unique opportunity to tackle this. In this paper we calculate the branching ratios of the semi-leptonic processes D+ → K+e-e+ and D+ → K+e-P-+, and the leptonic processes D0→ e-e+ and D0→ e-μ+, in the frameworks of the U(1) model, 2HDM and unparticle model. It is found that both the U(1) model and 2HDM may influence the semi-leptonic decay rates, but only the U(1) model offers substantial contributions to the pure leptonic decays, and the resultant branching ratio of DO → e- μ+ can be as large as 10-7 - 10-8. This might be observed at the future super τ-charm factory. |
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Bibliography: | rare decay, D meson, LFV 11-5641/O4 It is well recognized that looking for new physics at lower energy colliders is a path wnmn is complemen- tary to high energy machines such as the LHC. Using the large volume of data collected by BESIII, we may have a unique opportunity to tackle this. In this paper we calculate the branching ratios of the semi-leptonic processes D+ → K+e-e+ and D+ → K+e-P-+, and the leptonic processes D0→ e-e+ and D0→ e-μ+, in the frameworks of the U(1) model, 2HDM and unparticle model. It is found that both the U(1) model and 2HDM may influence the semi-leptonic decay rates, but only the U(1) model offers substantial contributions to the pure leptonic decays, and the resultant branching ratio of DO → e- μ+ can be as large as 10-7 - 10-8. This might be observed at the future super τ-charm factory. Xing-Dao Guo1,4 Xi-Qing Hao2 Hong-Wei Ke3) Ming-Gang Zhao,Xue-Qian L4( 1 School of Physics and Math, Xuzhou University of Technology, Xuzhou 221111, China 2 Physics Department, Henan Normal University, Xinxiang 453007, China 3 School of Science, Tianjin University, Tianjin 300072, China 4 Department of Physics, Nankai University, Tianjin 300071, China |
ISSN: | 1674-1137 0254-3052 |
DOI: | 10.1088/1674-1137/41/9/093107 |