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The LHCb Collaboration at the Large Hadron Collider at CERN discovered two pentaquark states $P_c(4380)$ and $P_c(4450)$. These two hidden-charm states are interpreted as the loosely bound $\Sigma_c(2455)D^*$ and $\Sigma_c^*(2520)D^*$…

High Energy Physics - Phenomenology · Physics 2015-09-30 Rui Chen , Xiang Liu , Xue-Qian Li , Shi-Lin Zhu

The $\Xi_b(6227)$ baryon with the quantum number $J^P=1/2^{-}$ is considered as a molecular state composed of a $\Sigma_b$ baryon and $\bar{K}$ meson. The partial decay widths of the $\Sigma_b\bar{K}$ molecular state into $\Xi_b\gamma$ and…

High Energy Physics - Phenomenology · Physics 2020-08-26 HongQiang Zhu , Yin Huang

The LHCb Collaboration has recently observed two narrow baryon resonances with beauty. Their masses and decay modes look consistent with the quark model orbitally excited states Lambda_b(5912) and Lambda*_b(5920), with quantum numbers…

High Energy Physics - Phenomenology · Physics 2013-02-22 C. Garcia-Recio , J. Nieves , O. Romanets , L. L. Salcedo , L. Tolos

The three pentaquark states, $P_c(4312)$, $P_c(4440)$ and $P_c(4457)$, discovered by the LHCb Collaboration in 2019, are widely recognized as $\bar{D}^{(\ast)}\Sigma_{c}$ hadronic molecules. Together with their four…

High Energy Physics - Phenomenology · Physics 2022-12-14 Jia-Ming Xie , Xi-Zhe Ling , Ming-Zhu Liu , Li-Sheng Geng

The decay behavior of an exotic state can be used to probe its internal structure. We note that the hidden-charm pentaquark states, $P_{\psi}^{N}(4312)$, $P_{\psi}^{N}(4440)$, and $P_{\psi}^{N}(4457)$, have only been observed in the $J/\psi…

High Energy Physics - Phenomenology · Physics 2024-12-06 Ming-Zhu Liu , Ya-Wen Pan , Li-Sheng Geng

For the long standing low mass puzzle of $\Lambda_c(2940)^+$, we propose an unquenched picture. Our calculation explicitly shows that the mass of the $\Lambda_c(2P,3/2^-)$ state can be lowered down to be consistent with the experimental…

High Energy Physics - Phenomenology · Physics 2020-04-07 Si-Qiang Luo , Bing Chen , Zhan-Wei Liu , Xiang Liu

We present a theoretical study of $\Xi^*(1690)$ resonance in the $\Lambda_c^+ \to \Lambda K^+ \bar{K}^0$ decay, where the weak interaction part proceeds through the Cabibbo-favored process $c \to s + u\bar{d}$. Next, the intermediate two…

High Energy Physics - Phenomenology · Physics 2023-07-19 Si-Wei Liu , Qing-Hua Shen , Ju-Jun Xie

We discuss the structure of the narrow mesons with charm and strangeness $D_{sJ}^*(2317)$ and $D_{sJ}(2460)$, stressing the role of the radiative decay modes in shedding light on the quark content of these states. We argue that present…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Colangelo , F. De Fazio , R. Ferrandes , A. Ozpineci

It is pointed out that in the decays $X(3872) \to D {\bar D} \gamma$ the possible `molecular' component of the X(3872) should give rise essentially only to a $D^0 {\bar D}^0 \gamma$ final state with a predictable spectrum, and should yield…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. B. Voloshin

The hidden-charm decays serve as irreplaceable platforms for probing the structures of charmonium-like states, such as $X(3872)$, $Y(4260)$, $Z_c(3900)$, and their heavy-quark-symmetry partners. In the hadronic molecular scenario, these…

High Energy Physics - Phenomenology · Physics 2025-10-29 Zhao-Sai Jia , Gang Li , Zhen-Hua Zhang

The newly observed hidden-charm meson Zc(3900) with quantum numbers J(P) = 1(+) is considered as a hadronic molecule composed of DD*. We give detailed predictions for the decay modes Zc(+) -> J/psi + pi(+) + gamma and Zc(+) -> J/psi + pi(+)…

High Energy Physics - Phenomenology · Physics 2014-11-19 Thomas Gutsche , Matthias Kesenheimer , Valery E. Lyubovitskij

It is shown that, in the bound state picture, the $\Lambda_c(2593) \to\Lambda_c\gamma$ and $\Lambda_c(2625)\to\Lambda_c\gamma$ decays are severely suppressed. On the other hand, for their bottom counterparts, which are predicted to have…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chi-Keung Chow

We report on recent results in spectroscopy from BaBar. This includes the discovery of a new $\Lambda_c$ baryon, detailed studies of the $D^*_{sJ}(2317)^+$, $D_{sJ}(2460)^+$, X(3872) and Y(4260) particles and the first measurement of…

High Energy Physics - Experiment · Physics 2007-05-23 S. J. Gowdy

Recently, a charmonium $X(3960)$ in $B$ decays in the $D_s^+D_s^-$ invariant-mass spectrum is discovered by the LHCb Collaboration with the quantum number $J^{PC}=0^{++}$. Motivated by the discovery, in this work, we systematically…

High Energy Physics - Phenomenology · Physics 2025-02-18 Xiaoyun Chen , Yue Tan , Xuejie Liu , Jialun Ping

In this work, we adopt the one-boson exchange model to analyze the $D^{(*)}_{(s)}B^{(*)}_{(s)}$ interactions from a coupled-channel perspective. For the $I(J^{P})=1(1^{+})$ $DB^{*}/D^*B/D^*B^{*}$ system, employing the complex scaling…

High Energy Physics - Phenomenology · Physics 2025-07-23 Qing-Fu Song , Wei Liang , Qi-Fang Lü , Xiao-Nu Xiong

At present work, we systematically study various bottom-strange molecular pentaquarks to search for possible bound states and resonances by adopting one-boson-exchange model within complex scaling method. According to our calculations, we…

High Energy Physics - Phenomenology · Physics 2025-10-09 Qing-Fu Song , Qi-Fang Lü , Xiaonu Xiong

A search for charmed baryons decaying to $D^0 p$ reveals two states: the $\Lambda_c(2880)^+$ baryon and a previously unobserved state at a mass of [$2939.8\pm 1.3 \text{(stat.)}\pm 1.0 \text{(syst.)}$]~\mevcc and with an intrinsic width of…

High Energy Physics - Experiment · Physics 2010-03-19 The BABAR Collaboration , B. Aubert

We study the bottom $\Lambda_b(6146)^0$ baryon, newly discovered by the LHCb Collaboration. By adopting an interpolating current of $(L_{\rho}, L_{\lambda})=(0,2)$ type and $D$-wave nature with spin-parity quantum numbers…

High Energy Physics - Phenomenology · Physics 2020-04-29 K. Azizi , Y. Sarac , H. Sundu

With the one-boson-exchange model we have studied the possible existence of the very loosely bound hidden-charm molecular baryons composed of anti-charmed meson and charmed baryon. Our numerical results indicate that there exist…

High Energy Physics - Phenomenology · Physics 2011-12-21 Zhong-Cheng Yang , Zhi-Feng Sun , Jun He , Xiang Liu , Shi-Lin Zhu

The present day experimental data on the $X(3872)$ decays do not allow to make clear conclusions on the dominating structure of this state. We discuss here an alternative way to study its structure by means of the two-step $\bar D^*$ (or…

Nuclear Theory · Physics 2016-06-22 Alexei Larionov , Mark Strikman , Marcus Bleicher
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