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Related papers: Exploring $X(5568)$ as a meson molecule

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In this work we study the production of $K^*(4307)$ in $B$ decays by determining the $J/\psi\pi^{+(0)}K^{0}$ and $J/\psi \pi^- K^+$ invariant mass distributions of the processes $B^+\to J/\psi \pi^+\pi^0 K^0$ and $B^+\to J/\psi \pi^+\pi^-…

High Energy Physics - Phenomenology · Physics 2020-07-15 Xiu-Lei Ren , K. P. Khemchandani , A. Martinez Torres

We study the molecular probability of the $X(3872)$ in the $D^0 \bar D^{*0}$ and $D^+ D^{*-}$ channels in several scenarios. One of them assumes that the state is purely due to a genuine nonmolecular component. However, it gets unavoidably…

High Energy Physics - Phenomenology · Physics 2023-07-13 Jing Song , L. R. Dai , E. Oset

We provide a comprehensive, up-to-date analysis of possible New Physics contributions to the mass difference $\Delta M_D$ in $D^0$-${\bar D}^0$ mixing. We consider the most general low energy effective Hamiltonian and include leading order…

High Energy Physics - Phenomenology · Physics 2008-11-26 Eugene Golowich , JoAnne Hewett , Sandip Pakvasa , Alexey A. Petrov

We present lattice results for the a_0(980) state using a variational approach with a variety of creation operators: quark-antiquark, mesonic molecule, diquark-antidiquark as well as two-meson type. Focus is put on recent technical…

We present a study of the $X(3872)$ lineshape in the decay $B \to X(3872)K\to D^0\overline{D}{}^{*0}K$ using a data sample of $772\times 10^6$ $B\overline{B}$ pairs collected at the $\Upsilon(4S)$ resonance with the Belle detector at the…

High Energy Physics - Experiment · Physics 2023-07-14 Belle Collaboration , H. Hirata , T. Iijima , Y. Kato , K. Tanida , I. Adachi , J. K. Ahn , H. Aihara , S. Al Said , D. M. Asner , H. Atmacan , T. Aushev , R. Ayad , V. Babu , Sw. Banerjee , P. Behera , K. Belous , J. Bennett , M. Bessner , V. Bhardwaj , B. Bhuyan , T. Bilka , D. Biswas , A. Bobrov , D. Bodrov , J. Borah , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , D. Červenkov , M. -C. Chang , P. Chang , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , S. Das , G. de Marino , G. De Nardo , G. De Pietro , R. Dhamija , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , D. Epifanov , T. Ferber , D. Ferlewicz , B. G. Fulsom , V. Gaur , A. Garmash , A. Giri , P. Goldenzweig , E. Graziani , K. Gudkova , C. Hadjivasiliou , S. Halder , T. Hara , K. Hayasaka , H. Hayashii , M. T. Hedges , D. Herrmann , W. -S. Hou , C. -L. Hsu , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , E. -J. Jang , S. Jia , Y. Jin , D. Kalita , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , T. Konno , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , P. Krokovny , T. Kuhr , R. Kumar , K. Kumara , A. Kuzmin , Y. -J. Kwon , T. Lam , J. S. Lange , M. Laurenza , K. Lautenbach , S. C. Lee , L. K. Li , Y. Li , J. Libby , K. Lieret , Y. -R. Lin , D. Liventsev , T. Luo , Y. Ma , A. Martini , M. Masuda , T. Matsuda , D. Matvienko , S. K. Maurya , F. Meier , M. Merola , F. Metzner , K. Miyabayashi , G. B. Mohanty , M. Mrvar , R. Mussa , I. Nakamura , M. Nakao , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , K. Ogawa , S. Ogawa , H. Ono , P. Oskin , P. Pakhlov , G. Pakhlova , T. Pang , S. Pardi , H. Park , J. Park , S. -H. Park , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , E. Prencipe , M. T. Prim , N. Rout , G. Russo , S. Sandilya , A. Sangal , L. Santelj , V. Savinov , G. Schnell , C. Schwanda , A. J. Schwartz , Y. Seino , K. Senyo , M. E. Sevior , W. Shan , M. Shapkin , C. Sharma , J. -G. Shiu , B. Shwartz , A. Sokolov , E. Solovieva , M. Starič , Z. S. Stottler , M. Sumihama , W. Sutcliffe , M. Takizawa , U. Tamponi , S. Tanaka , F. Tenchini , R. Tiwary , K. Trabelsi , M. Uchida , T. Uglov , Y. Unno , K. Uno , S. Uno , P. Urquijo , Y. Usov , S. E. Vahsen , G. Varner , A. Vinokurova , A. Vossen , D. Wang , E. Wang , M. -Z. Wang , S. Watanuki , O. Werbycka , E. Won , X. Xu , B. D. Yabsley , W. Yan , S. B. Yang , J. Yelton , J. H. Yin , Y. Yook , C. Z. Yuan , L. Yuan , Y. Yusa , Z. P. Zhang , V. Zhilich , V. Zhukova

We assign $X(4500)$ as a D-wave tetraquark state and study the decay of $X(4500)$ $\to$ $J/\psi \phi$. The mass and the decay constant of $X(4500)$ are calculated by using the SVZ sum rules. For the decay width of $X(4500)$ $\to$ $J/\psi…

High Energy Physics - Phenomenology · Physics 2023-12-05 Yiling Xie , Hao Sun

We propose that the search of the $B\to D^{*}_{sJ}M$ decays, $M=D$, $\pi$ and $K$, can discriminate the different theoretical postulations for the nature of the recently observed $D^{*}_{sJ}$ mesons. The ratio of the branching ratios…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chuan-Hung Chen , Hsiang-nan Li

We study the X(3872)-->D^0 \bar D^0 \pi^0 decay within a D \bar D^* molecular picture for the X(3872) state. This decay mode is more sensitive to the long-distance structure of the X(3872) resonance than its J/\psi\pi\pi and J/\psi3\pi…

High Energy Physics - Phenomenology · Physics 2014-06-02 Feng-Kun Guo , Carlos Hidalgo-Duque , Juan Nieves , Altug Ozpineci , Manuel Pavon Valderrama

We interpret the $B_{s1}(5778)$ as an $S$-wave $B^\ast\bar{K}$ molecular state in the Bethe-Salpeter equation approach. In the ladder and instantaneous approximations, and with the kernel containing one-particle-exchange diagrams and…

High Energy Physics - Phenomenology · Physics 2019-11-20 Zhen-Yang Wang , Jing-Juan Qi , Qi-Xin Yu , Xin-Heng Guo

Two iso-singlet hadron states $X_0(2900)$ and $X_1(2900)$ with $J=0$ and 1 respectively, discovered by the LHCb collaboration in 2020, were identified as molecular bound states of $\bar D^*K^*$. Recently two structures $T^a_{cs0}(2900)^0$…

High Energy Physics - Phenomenology · Physics 2023-01-02 Hong-Wei Ke , Yi-Fan Shi , Xiao-Hai Liu , Xue-Qian Li

The structure, spectroscopic parameters and width of the resonance with quantum numbers $J^{PC}=1^{++}$ discovered by the COMPASS Collaboration and classified as the $a_1(1420)$ meson are examined in the context of QCD sum rule method. In…

High Energy Physics - Phenomenology · Physics 2018-03-14 H. Sundu , S. S. Agaev , K. Azizi

The strong $D_{2}^{*}(2460)^{0}\rightarrow D^+ \pi^- $ and $D_{s2}^{*}(2573)^{+}\rightarrow D^{+} K^{0}$ transitions are analyzed via three point QCD sum rules. First, we calculate the corresponding strong coupling constants $g_{D_2^*D\pi}$…

High Energy Physics - Phenomenology · Physics 2014-09-29 K. Azizi , Y. Sarac , H. Sundu

We investigate the newly observed $X(4500)$ and $X(4700)$ based on the diquark-antidiquark configuration within the framework of QCD sum rules. Both of them may be interpreted as the $D$-wave $cs\bar{c}\bar{s}$ tetraquark states of $J^P =…

High Energy Physics - Phenomenology · Physics 2017-03-17 Hua-Xing Chen , Er-Liang Cui , Wei Chen , Xiang Liu , Shi-Lin Zhu

Heavy quark symmetry can help us identify the internal structure of hadrons and predict new particles. In this study, we examine the strong decay modes of the observed $\Lambda_b^0(6146)$ and $\Lambda_b^0(6152)$, assuming these two states…

High Energy Physics - Phenomenology · Physics 2024-06-18 Jing-wen Feng , Cai Cheng , Yin Huang

In this work, we investigate the exotic doubly charmed molecular state $T_{cc}^{+}(3875)$ with quantum numbers $J^{P} = 1^{+}$ using the Thermal QCD Sum Rules framework. Employing a molecular interpolating current, we evaluate the two-point…

High Energy Physics - Phenomenology · Physics 2026-03-17 S. Damen , J. Y. Süngü , E. Veli Veliev

Using the QCD sum rule approach we study the X(4260) state assuming that it can be described by a mixed charmonium-tetraquark current with $J^{PC}=1^{--}$ quantum numbers. For the mixing angle around $\theta=(53.0 \pm 0.5)^0$, we obtain a…

High Energy Physics - Phenomenology · Physics 2013-12-02 R. M. Albuquerque , J. M. Dias , M. Nielsen , C. M. Zanetti

We observe evidence for $D^0 - \bar{D}^0$ mixing by measuring the difference in apparent lifetime when a $D^0$ meson decays to the CP eigenstates $K^+K^-$ and $\pi^+\pi^-$, and when it decays to the final state $K^-\pi^+$. We find…

High Energy Physics - Experiment · Physics 2008-11-26 Belle Collaboration , M. Staric

The LHCb Collaboration recently observed new structures in the invariant mass spectrum of $J/\psi J/\psi$ meson pairs produced in proton-proton collisions, including a narrow peak around $6.2$ GeV. This study investigates the thermal…

High Energy Physics - Phenomenology · Physics 2025-06-11 Ö. E. Demircan , H. Dağ , H. Sundu , J. Y. Süngü , E. V. Veliev

In this feature article we summarise and highlight aspects of the treatment of four-quark states with functional methods. Model approaches to those exotic mesons almost inevitably have to assume certain internal structures, e.g. by grouping…

High Energy Physics - Phenomenology · Physics 2021-09-02 Gernot Eichmann , Christian S. Fischer , Walter Heupel , Nico Santowsky , Paul C. Wallbott

Very recently, three new structures $\Xi_c(2923)^0$, $\Xi(2938)^0$, and $\Xi(2964)^0$ at the invariant mass spectrum of $\Lambda_c^{+}K^{-}$ observed by the LHCb Collaboration triggers a hot discussion about their inner structure. In this…

High Energy Physics - Phenomenology · Physics 2021-02-03 HongQiang Zhu , NaNa Ma , Yin Huang
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