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Related papers: The study of Ds1(2460) and Ds1(2536) mixing

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The mixing mechanism of axial-vectors $D_{s1}(2460)$ and $D_{s1}(2536)$ is studied via intermediate hadron loops, e.g. $D^* K$, to which both states have strong couplings. By constructing the two-state mixing propagator matrix that respects…

High Energy Physics - Phenomenology · Physics 2015-06-03 Xiao-Gang Wu , Qiang Zhao

In charmed $D$ and $D_s$ mesons sector, the matrix of a Hamiltonian in a quark potential model is computed in the $2^3S_1$ and $1^3D_1$ subspace. The masses of four mixed states of $2^3S_1$ and $1^3D_1$ denoted with $D^*_1(2635)$,…

High Energy Physics - Phenomenology · Physics 2020-09-23 Hao Yu , Ze Zhao , Ailin Zhang

The hadron loop effect is conjectured to be important in understanding discrepancies between the observed states in experiments and the theoretical expectations of non-relativistic potential model. We present that, in an easily operable…

High Energy Physics - Phenomenology · Physics 2011-09-08 Zhi-Yong Zhou , Zhiguang Xiao

The recently discovered $D_{s0}(2590)$ state by the LHCb collaboration was regarded as the first excited state of $^1S_{0}$ charmed-strange meson. Its mass is, however, lower than the Godfrey-Isgur quark model prediction by about 80 MeV. In…

High Energy Physics - Phenomenology · Physics 2021-12-15 Jia-Ming Xie , Ming-Zhu Liu , Li-Sheng Geng

Motivated by the recently observed $D_{s0}(2590)$ state by LHCb, we investigate the mass spectrum and the strong decay properties of the charmed-strange mesons within Godfrey-Isgur model considering the coupled-channel effects. Our results…

High Energy Physics - Phenomenology · Physics 2023-12-06 Jing-Jing Yang , Wei Hao , Xiaoyu Wang , De-Min Li , Yu-Xiao Li , En Wang

Recently LHCb predicted spin 1 and spin 3 states D* s1(2860) and D* s3(2860) which are studied through their strong decays, and are assigned to fit the 13D1and 13D3 states in the charm spectroscopy. In this paper,using the heavy quark…

High Energy Physics - Phenomenology · Physics 2016-11-07 Pallavi Gupta , Alka Upadhyay

We study the interaction of the $n \bar {D}_{s1}(2460)$ and $n \bar {D}_{s1}(2536)$ systems from the perspective that the $D_{s1}(2460)$ and $D_{s1}(2536)$ states are molecular states of $K D^*$ and $K^*D$, respectively. We use an improved…

High Energy Physics - Phenomenology · Physics 2025-08-11 Breno Agatão , Pedro Brandão , A. Martinez Torres , K. P. Khemchandani , Luciano M. Abreu , E. Oset

The mass spectra and wave functions of both $1S$ and $2S$ state heavy pseudoscalar ($P$) and vector ($V$) mesons are analyzed within the light-front quark model. Important empirical constraints employed in our analysis of the mass spectra…

High Energy Physics - Phenomenology · Physics 2022-09-13 Ahmad Jafar Arifi , Ho-Meoyng Choi , Chueng-Ryong ji , Yongseok Oh

We calculate the mass shifts of heavy-light scalar mesons due to hadronic loops under the assumption that these vanish for the groundstate heavy-light mesons. The results show that the masses calculated in quark models can be reduced…

High Energy Physics - Phenomenology · Physics 2008-11-26 Feng-Kun Guo , Siegfried Krewald , Ulf-G. Meissner

In this paper we develop a formalism for incorporating hadron loops in the quark model. We derive expressions for mass shifts, continuum components and mixing amplitudes of "quenched" quark model states due to hadron loops, as perturbation…

High Energy Physics - Phenomenology · Physics 2009-03-05 T. Barnes , E. S. Swanson

Using the variational principle, we systematically investigate the mass spectra and wave functions of both $1S$ and $2S$ state heavy pseudoscalar $(P)$ and vector $(V)$ mesons within the light-front quark model. This approach incorporates a…

High Energy Physics - Phenomenology · Physics 2024-07-03 Bhoomika Pandya , Bheemsehan Gurjar , Dipankar Chakrabarti , Ho-Meoyng Choi , Chueng-Ryong Ji

In this study, we calculate the mixing angles between the axial-vector mesons $D_{1(s1)} - D_{1(s1)}^\prime$ and $B_{1(s1)} - B_{1(s1)}^\prime$ using the QCD sum rules approach. Our results are $\theta_1 = 28.2 \pm 0.6^\circ$, $\theta_2 =…

High Energy Physics - Phenomenology · Physics 2024-12-31 T. M. Aliev , S. Bilmis , M. Savci

The $T_{c\bar{s}}$ state observed in the decay $D_{s1}(2460)^+ \to D_s^+\pi^+\pi^-$ provides direct evidence for an isovector open-charm tetraquark state with strangeness. We develop a unified theoretical framework that consistently…

High Energy Physics - Phenomenology · Physics 2025-10-03 Zhi Yang , Guang-Juan Wang , Jia-Jun Wu , Makoto Oka

We make a systematic calculation of the spectra and hadronic decays of the $D_s$ system in a coupled channel framework, where the unquenched effects are induced by the $^3P_0$ model. In the calculation, the wave functions are obtained by…

High Energy Physics - Phenomenology · Physics 2022-08-24 Wei Hao , Yu Lu , Bing-Song Zou

We examine charmed-strange mesons within the framework of the constituent quark model, focusing on the states with L=1. We are particularly interested in the mixing of two spin-states that are involved in $D_{s1}(2536)$ and the recently…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yukiko Yamada , Akira Suzuki , Masashi Kazuyama , Masahiro Kimura

Different experiments have confirmed that the $D_{s0}^{\ast}(2317)$ and $D_{s1}(2460)$ mesons are very narrow states located, respectively, below the $DK$ and $D^{\ast}K$ thresholds. This is markedly in contrast with the expectations of…

High Energy Physics - Phenomenology · Physics 2016-09-08 Pablo G. Ortega , Jorge Segovia , David R. Entem , Francisco Fernández

We carry out a systematic study of the heavy-light meson strong decays in a chiral quark model. For the $S$-wave vectors ($D^*(2007)$, $D^{*\pm}(2010)$), $P$-wave scalars ($D^*_0(2400)$, $B^*_0(5730)$) and tensors ($D^*_2(2460)$,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Xian-hui Zhong , Qiang Zhao

Heavy-light hadrons are studied in a mass loaded flux tube model. The study indicates that the dynamics of mesons and baryons containing a $c$ quark is well described by the mass loaded flux tube. The hypothesis of good diquark-antiquark…

High Energy Physics - Phenomenology · Physics 2015-05-13 Hong-Yun Shan , Ailin Zhang

Charmonium states can decay into pairs of $D$ and $\overline{D}$ mesons if their masses are above the allowed decay thresholds. In general $c\bar{c}$ states near threshold will also undergo mixing with $D\overline{D}$ molecular (or…

High Energy Physics - Lattice · Physics 2010-11-05 Gunnar Bali , Christian Ehmann

We re-examine the hadronic loop effects to the masses of $D^*_0$ and $D^*_{s0}$ calculated in quark models in the framework of heavy meson chiral perturbation theory (HMCHPT). The inaccuracy in the choice of the argument of the chiral loop…

High Energy Physics - Phenomenology · Physics 2023-03-22 Mohammad H. Alhakami , Numa A. Althubiti , Nwuyer A. Al-shammari
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