Study of 1D Strange Charmed Meson Family Using HQET

Recently LHCb predicted spin 1 and spin 3 states Ds1⁎(2860) and Ds3⁎(2860) which are studied through their strong decays and are assigned to fit the 13D1 and 13D3 states in the charm spectroscopy. In this paper, using the heavy quark effective theory, we state that assigning Ds1⁎(2860) as the mixing...

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Main Authors: Pallavi Gupta, A. Upadhyay
Format: Article
Language:English
Published: Wiley 2016-01-01
Series:Advances in High Energy Physics
Online Access:http://dx.doi.org/10.1155/2016/4957236
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author Pallavi Gupta
A. Upadhyay
author_facet Pallavi Gupta
A. Upadhyay
author_sort Pallavi Gupta
collection DOAJ
description Recently LHCb predicted spin 1 and spin 3 states Ds1⁎(2860) and Ds3⁎(2860) which are studied through their strong decays and are assigned to fit the 13D1 and 13D3 states in the charm spectroscopy. In this paper, using the heavy quark effective theory, we state that assigning Ds1⁎(2860) as the mixing of 13D1-23S1 states is rather a better justification to its observed experimental values than a pure state. We study its decay modes variation with hadronic coupling constant gxh and the mixing angle θ. We appoint spin 3 state Ds3⁎(2860) as the missing 1D  3-JP state and also study its decay channel behavior with coupling constant gyh. To appreciate the above results, we check the variation of decay modes for their spin partners states, that is, 1D2 and 1D2′, with their masses and strong coupling constant, that is, gxh and gyh. Our calculation using HQET approach gives mixing angle of the 13D1-23S1 state for Ds1⁎(2860) to lie in the range (-1.6 radians ≤θ≤-1.2 radians). Our calculation for coupling constant values gives gxh to lie within value range of 0.17–0.20 and gyh to be 0.40. We expect from experiments to observe this mixing angle to verify our results.
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spelling doaj-art-1baa60f33c914d49a9d230ccd3c70f0d2025-02-03T05:45:09ZengWileyAdvances in High Energy Physics1687-73571687-73652016-01-01201610.1155/2016/49572364957236Study of 1D Strange Charmed Meson Family Using HQETPallavi Gupta0A. Upadhyay1School of Physics and Material Science, Thapar University, Patiala, Punjab 147004, IndiaSchool of Physics and Material Science, Thapar University, Patiala, Punjab 147004, IndiaRecently LHCb predicted spin 1 and spin 3 states Ds1⁎(2860) and Ds3⁎(2860) which are studied through their strong decays and are assigned to fit the 13D1 and 13D3 states in the charm spectroscopy. In this paper, using the heavy quark effective theory, we state that assigning Ds1⁎(2860) as the mixing of 13D1-23S1 states is rather a better justification to its observed experimental values than a pure state. We study its decay modes variation with hadronic coupling constant gxh and the mixing angle θ. We appoint spin 3 state Ds3⁎(2860) as the missing 1D  3-JP state and also study its decay channel behavior with coupling constant gyh. To appreciate the above results, we check the variation of decay modes for their spin partners states, that is, 1D2 and 1D2′, with their masses and strong coupling constant, that is, gxh and gyh. Our calculation using HQET approach gives mixing angle of the 13D1-23S1 state for Ds1⁎(2860) to lie in the range (-1.6 radians ≤θ≤-1.2 radians). Our calculation for coupling constant values gives gxh to lie within value range of 0.17–0.20 and gyh to be 0.40. We expect from experiments to observe this mixing angle to verify our results.http://dx.doi.org/10.1155/2016/4957236
spellingShingle Pallavi Gupta
A. Upadhyay
Study of 1D Strange Charmed Meson Family Using HQET
Advances in High Energy Physics
title Study of 1D Strange Charmed Meson Family Using HQET
title_full Study of 1D Strange Charmed Meson Family Using HQET
title_fullStr Study of 1D Strange Charmed Meson Family Using HQET
title_full_unstemmed Study of 1D Strange Charmed Meson Family Using HQET
title_short Study of 1D Strange Charmed Meson Family Using HQET
title_sort study of 1d strange charmed meson family using hqet
url http://dx.doi.org/10.1155/2016/4957236
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AT aupadhyay studyof1dstrangecharmedmesonfamilyusinghqet