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Related papers: Molecular components in P-wave charmed-strange mes…

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We study the positive parity charmed strange mesons using lattice QCD, the only reliable ab initio method to study QCD at low energies. Especially the experimentally observed $D_{s0}^*(2317)$ and $D_{s1}(2460)$ have challenged theory for…

High Energy Physics - Lattice · Physics 2016-01-06 Luka Leskovec , C. B. Lang , Daniel Mohler , Sasa Prelovsek , R. M. Woloshyn

Using a constituent quark model we study the mass and decay channels of meson meson and meson baryon structures in the charm sector. We show that the $X(3872)$ and $X(3940)$ resonances can be described as mixed charmonium-molecular states…

High Energy Physics - Phenomenology · Physics 2013-12-03 F. Fernandez , D. R. Entem , P. G. Ortega

We propose an explanation of the new resonances observed in $D_s^{(*)+} \pi^0$ decays. We suggest that the data can be explained by the mixing of conventional p-wave excited $D_s^+$ mesons with 4-quark states. The narrow states observed in…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas E. Browder , Sandip Pakvasa , Alexey A. Petrov

We study the decay widths of the narrow resonances $D_{sj}^*(2317)$ and $D_{sj}(2460)$ in the chiral quark model, together with the well-known $D^\ast$ and $D_s^*$ mesons. All the parameters in our calculation are taken from Godfrey and…

High Energy Physics - Phenomenology · Physics 2010-11-15 Feng-Lin Wang , Xiao-Lin Chen , Da-Hai Lu , Shi-Lin Zhu , Wei-Zhen Deng

Inspired by that Belle\uppercase\expandafter{\romannumeral2} Collaboration recently reported $T_{cc}$, which can be interpreted as a molecular $DD^{*}$, we investigated the trihadron system of $T_{cc}$ partner with $IJ^{P}$=$01^{-}$ in the…

High Energy Physics - Phenomenology · Physics 2024-04-03 Yue Tan , Xuejie Liu , Xiaoyun Chen , Youchang Yang , Hongxia Huang , Jialun Ping

Motivated by the recently reported resonant structure $X(2300)$, a strong candidate for a fully strange tetraquark with positive parity, we perform a systematic study of fully strange tetra- and penta-quark systems within a chiral quark…

High Energy Physics - Phenomenology · Physics 2026-02-03 Gang Yang , Jialun Ping , Jorge Segovia

Masses of the ground and excited (1P, 2S, 1D, 2P, 3S) states of the fully-heavy tetraquarks, composed of charm ($c$) and bottom ($b$) quarks and antiquarks, are calculated in the diquark-antidiquark picture within the relativistic quark…

High Energy Physics - Phenomenology · Physics 2022-12-14 R. N. Faustov , V. O. Galkin , E. M. Savchenko

Stimulated by the measurement of the $J\psi\phi$ decay model of $Y(4274)$ by the LHCb Collaboration, we consider a possible interpretation of this state as a hadron molecular-a bound state of $D_s$ and $\bar{D}_{s0}(2317)$ mesons. Using…

High Energy Physics - Phenomenology · Physics 2022-03-23 Hong Qiang Zhu , Yin Huang

The charmed meson pair $(\frac{3}{2})^+$ and anti-$(\frac{1}{2})^-$, i.e. $D_1(2420)\bar D+c.c.$, $D_1(2420)\bar D^*+c.c.$, $D_2(2460)\bar D^*+c.c.$, can couple to states with vector quantum number $J^{PC}=1^{--}$ and exotic quantum number…

High Energy Physics - Phenomenology · Physics 2014-06-16 Qian Wang

We have studied the meson-baryon $S-$wave interaction, using coupled channels, in the isoscalar hidden-charm strange sector and $J^P = 1/2^-,3/2^-$ and $5/2^-$. We impose constraints of heavy quark spin symmetry in the interaction and…

High Energy Physics - Phenomenology · Physics 2020-01-09 C. W. Xiao , J. Nieves , E. Oset

The mass spectrum of S and P-wave mesons containing a single heavy quark is computed in the quenched approximation, using NRQCD up to third order in the inverse heavy quark mass expansion. Previous results found third order contributions…

High Energy Physics - Lattice · Physics 2009-10-31 Randy Lewis , R. M. Woloshyn

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

In this letter we discuss the masses and the splittings of 1(2S+1)P_J states in the spectrum of D and B mesons, as they appear in the approach of the QCD string with quarks at the ends. We find good agreement of our predictions with those…

High Energy Physics - Phenomenology · Physics 2011-03-23 Yu. S. Kalashnikova , A. V. Nefediev

The masses of low-lying S-wave mesons are evaluated in a constituent quark model (CQM) where the Cornell-like potential and one-gluon exchange spin-spin interaction are employed. To make the model applicable to both the light and heavy…

High Energy Physics - Phenomenology · Physics 2023-04-14 Zheng Zhao , Kai Xu , Attaphon Kaewsnod , Xuyang Liu , Ayut Limphirat , Yupeng Yan

Searching for exotic multiquark states and elucidating their nature remains a central topic in understanding quantum chromodynamics--the underlying theory of the strong interaction. Two of the most studied such states are the charm-strange…

High Energy Physics - Phenomenology · Physics 2023-07-26 Tian-Chen Wu , Li-Sheng Geng

The scalar meson $D_{s0}^*(2317)$ is found 37(17)MeV below DK threshold in a lattice simulation of the $J^P=0^+$ channel using, for the first time, both DK as well as $\bar sc$ interpolating fields. The simulation is done on $N_f=2+1$ gauge…

High Energy Physics - Lattice · Physics 2013-12-04 Daniel Mohler , C. B. Lang , Luka Leskovec , Sasa Prelovsek , R. M. Woloshyn

The BaBar Collaboration has recently reported branching fractions for semileptonic decays of the $B$ meson into final states with charged and neutral $D_{1}(2420)$ and $D_{2}^{\ast}(2460)$, two narrow orbitally excited charmed mesons. We…

High Energy Physics - Phenomenology · Physics 2020-05-19 J. Segovia , C. Albertus , D. R. Entem , F. Fernández , E. Hernández , M. A. Pérez-García

In the framework of the chiral quark model along with complex scaling range, we perform a dynamical study on the low-lying $S$-wave doubly-heavy tetraquark states ($QQ\bar{q}\bar{q}$, $Q=c, b$ and $q=u, d$) with an accurate computing…

High Energy Physics - Phenomenology · Physics 2020-01-08 Gang Yang , Jialun Ping , Jorge Segovia

Hidden-charm pentaquark-like $P_{\psi s}^\Lambda(4459)^0$ and $P_{\psi s}^\Lambda(4338)$ resonances are studied in a constituent quark model as molecular meson-baryon structures. Such states are found in the $J^P(I)=\frac{1}{2}^-(0)$…

High Energy Physics - Phenomenology · Physics 2023-02-22 Pablo G. Ortega , David R. Entem , Francisco Fernandez

We have calculated the mass spectra for the $\bar{D}_s^{(*)}D^{(*)}$ molecular states and $sc\bar q\bar c$ tetraquark states with $J^P=0^+, 1^+, 2^+$. The masses of the axial-vector $\bar{D}_sD^{*}$, $\bar{D}_s^{*}D$ molecular states and…

High Energy Physics - Phenomenology · Physics 2021-09-02 Qi-Nan Wang , Wei Chen , Hua-Xing Chen