Branching fractions of semileptonic D and $$D_s$$ D s decays from the covariant light-front quark model
Abstract Based on the predictions of the relevant form factors from the covariant light-front quark model, we show the branching fractions for the $$D (D_s) \rightarrow (P,\,S,\,V,\,A)\,\ell \nu _\ell $$ D ( D s ) → ( P , S , V , A ) ℓ ν ℓ ( $$\ell =e$$ ℓ = e or $$\mu $$ μ ) decays, where P denotes...
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Online Access: | http://link.springer.com/article/10.1140/epjc/s10052-017-5170-5 |
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doaj-fa80ad34aff54f14b373b3d0f72cdab92020-11-24T20:56:25ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522017-09-017791910.1140/epjc/s10052-017-5170-5Branching fractions of semileptonic D and $$D_s$$ D s decays from the covariant light-front quark modelHai-Yang Cheng0Xian-Wei Kang1Institute of Physics, Academia SinicaInstitute of Physics, Academia SinicaAbstract Based on the predictions of the relevant form factors from the covariant light-front quark model, we show the branching fractions for the $$D (D_s) \rightarrow (P,\,S,\,V,\,A)\,\ell \nu _\ell $$ D ( D s ) → ( P , S , V , A ) ℓ ν ℓ ( $$\ell =e$$ ℓ = e or $$\mu $$ μ ) decays, where P denotes the pseudoscalar meson, S the scalar meson with a mass above 1 GeV, V the vector meson and A the axial-vector one. Comparison with the available experimental results are made, and we find an excellent agreement. The predictions for other decay modes can be tested in a charm factory, e.g., the BESIII detector. The future measurements will definitely further enrich our knowledge of the hadronic transition form factors as well as the inner structure of the even-parity mesons (S and A).http://link.springer.com/article/10.1140/epjc/s10052-017-5170-5 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Hai-Yang Cheng Xian-Wei Kang |
spellingShingle |
Hai-Yang Cheng Xian-Wei Kang Branching fractions of semileptonic D and $$D_s$$ D s decays from the covariant light-front quark model European Physical Journal C: Particles and Fields |
author_facet |
Hai-Yang Cheng Xian-Wei Kang |
author_sort |
Hai-Yang Cheng |
title |
Branching fractions of semileptonic D and $$D_s$$ D s decays from the covariant light-front quark model |
title_short |
Branching fractions of semileptonic D and $$D_s$$ D s decays from the covariant light-front quark model |
title_full |
Branching fractions of semileptonic D and $$D_s$$ D s decays from the covariant light-front quark model |
title_fullStr |
Branching fractions of semileptonic D and $$D_s$$ D s decays from the covariant light-front quark model |
title_full_unstemmed |
Branching fractions of semileptonic D and $$D_s$$ D s decays from the covariant light-front quark model |
title_sort |
branching fractions of semileptonic d and $$d_s$$ d s decays from the covariant light-front quark model |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2017-09-01 |
description |
Abstract Based on the predictions of the relevant form factors from the covariant light-front quark model, we show the branching fractions for the $$D (D_s) \rightarrow (P,\,S,\,V,\,A)\,\ell \nu _\ell $$ D ( D s ) → ( P , S , V , A ) ℓ ν ℓ ( $$\ell =e$$ ℓ = e or $$\mu $$ μ ) decays, where P denotes the pseudoscalar meson, S the scalar meson with a mass above 1 GeV, V the vector meson and A the axial-vector one. Comparison with the available experimental results are made, and we find an excellent agreement. The predictions for other decay modes can be tested in a charm factory, e.g., the BESIII detector. The future measurements will definitely further enrich our knowledge of the hadronic transition form factors as well as the inner structure of the even-parity mesons (S and A). |
url |
http://link.springer.com/article/10.1140/epjc/s10052-017-5170-5 |
work_keys_str_mv |
AT haiyangcheng branchingfractionsofsemileptonicdanddsdsdecaysfromthecovariantlightfrontquarkmodel AT xianweikang branchingfractionsofsemileptonicdanddsdsdecaysfromthecovariantlightfrontquarkmodel |
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1716789717376172032 |