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Related papers: $X(3872)$, $X_b$, and the $\chi_{b1}(3P)$ state

200 papers

Many new states in the charmonium and bottomonium mass region were recently discovered by the BaBar, Belle and CDF Collaborations. We use the QCD Sum Rule approach to study the possible structure of some of these states. In particular we…

High Energy Physics - Phenomenology · Physics 2015-05-30 F. S. Navarra , M. Nielsen , J. -M. Richard

Assuming the newly observed structure $Z_{b}(10610)$ as a bottomonium-like molecular state $B^{*}\bar{B}$, we calculate its mass in the framework of QCD sum rules. The numerical result is $10.54\pm0.22 GeV$ for $B^{*}\bar{B}$, which…

High Energy Physics - Phenomenology · Physics 2011-10-11 Jian-Rong Zhang , Ming Zhong , Ming-Qiu Huang

The photoproduction of bottomonium-like states $Z_{b}(10610)$ and $Z_{b}(10650)$ via $\gamma p$ scattering is studied within an effectiv Lagrangian approach and the vector-meson-dominance model. The Regge model is employed to calculate the…

High Energy Physics - Phenomenology · Physics 2021-08-06 Xiao-Yun Wang , Wei Kou , Qing-Yong Lin , Ya-Ping Xie , Xurong Chen , Alexey Guskov

We report a search for $X(3872)$ and $X(3915)$ in $B^+ \to \chi_{c1} \pi^0 K^+$ decays. We set an upper limit of $\mathcal{B}(B^+ \to X(3872) K^+) \times \mathcal{B}(X(3872) \to \chi_{c1} \pi^0)$ $ < 8.1 \times 10^{-6}$ and $\mathcal{B}(B^+…

High Energy Physics - Experiment · Physics 2019-06-19 V. Bhardwaj , S. Jia , I. Adachi , H. Aihara , D. M. Asner , T. Aushev , R. Ayad , V. Babu , I. Badhrees , S. Bahinipati , V. Bansal , P. Behera , C. Beleño , M. Berger , B. Bhuyan , T. Bilka , J. Biswal , A. Bobrov , A. Bondar , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , M. Campajola , L. Cao , D. Červenkov , P. Chang , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , S. Di Carlo , Z. Doležal , T. V. Dong , S. Eidelman , D. Epifanov , J. E. Fast , T. Ferber , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Garmash , A. Giri , P. Goldenzweig , D. Greenwald , O. Grzymkowska , J. Haba , T. Hara , K. Hayasaka , H. Hayashii , W. -S. Hou , C. -L. Hsu , T. Iijima , K. Inami , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , Y. Jin , D. Joffe , K. K. Joo , T. Julius , A. B. Kaliyar , G. Karyan , Y. Kato , T. Kawasaki , C. Kiesling , C. H. Kim , D. Y. Kim , S. H. Kim , K. Kinoshita , P. Kodyš , S. Korpar , D. Kotchetkov , P. Križan , R. Kroeger , P. Krokovny , T. Kuhr , R. Kulasiri , R. Kumar , Y. -J. Kwon , K. Lalwani , J. S. Lange , I. S. Lee , J. K. Lee , J. Y. Lee , S. C. Lee , L. K. Li , Y. B. Li , L. Li Gioi , J. Libby , D. Liventsev , P. -C. Lu , J. MacNaughton , C. MacQueen , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , K. Miyabayashi , R. Mizuk , G. B. Mohanty , T. Mori , R. Mussa , M. Nakao , K. J. Nath , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , K. Nishimura , S. Ogawa , H. Ono , Y. Onuki , P. Pakhlov , G. Pakhlova , B. Pal , S. Pardi , H. Park , S. -H. Park , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , V. Popov , E. Prencipe , P. K. Resmi , M. Ritter , A. Rostomyan , G. Russo , Y. Sakai , M. Salehi , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , O. Seon , M. E. Sevior , C. P. Shen , J. -G. Shiu , B. Shwartz , F. Simon , A. Sokolov , E. Solovieva , M. Starič , Z. S. Stottler , M. Sumihama , T. Sumiyoshi , W. Sutcliffe , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , K. Trabelsi , M. Uchida , S. Uehara , T. Uglov , S. Uno , P. Urquijo , R. Van Tonder , G. Varner , B. Wang , C. H. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , S. Watanuki , E. Won , S. B. Yang , H. Ye , J. Yelton , J. H. Yin , J. Zhang , Z. P. Zhang , V. Zhilich , V. Zhukova , V. Zhulanov

Motivated by the interpretation of $X(3872)$ as a $D\bar{D}^{*}$ molecular state, heavy-quark spin symmetry predicts a spin-2 partner, $X_{2}(4013)$, which can be regarded as a $D^{*}\bar{D}^{*}$ molecule with quantum numbers $J^{PC} =…

High Energy Physics - Phenomenology · Physics 2025-10-16 Min Yuan , Bo Nan Zhang , Yin Huang

We propose that the $X(3915)$ observed in the $J/\psi\,\omega$ channel is the same state as the $\chi_{c2}(3930)$, and the $X(3960)$, observed in the $D_s^+D_s^-$ channel, is an $S$-wave $D_s^+ D_s^-$ hadronic molecule. In addition, the…

High Energy Physics - Phenomenology · Physics 2023-09-14 Teng Ji , Xiang-Kun Dong , Miguel Albaladejo , Meng-Lin Du , Feng-Kun Guo , Juan Nieves , Bing-Song Zou

In this contribution, we discuss our recent unquenched quark model results for the spectrum of $b \bar b$ mesons with self energy corrections, due to the coupling to the meson-meson continuum. Our unquenched quark model predictions for the…

High Energy Physics - Phenomenology · Physics 2015-10-05 J. Ferretti

The possibility to observe new bottomonium states with $J^{PC}= 1^{--}$ in the region $10.7-11.1$ GeV is discussed. The analysis of the di-electron widths shows that the $(n+1)^3S_1$ and $n^3D_1$ states ($n\geq 3$) may be mixed with a…

High Energy Physics - Phenomenology · Physics 2009-09-11 A. M. Badalian , B. L. G. Bakker , I. V. Danilkin

Recently, the LHCb Collaboration reported a new structure $P_{cs}(4459)$ with a mass of 19 MeV below the $\Xi_c \bar{D}^{*} $ threshold. It may be a candidate of molecular state from the $\Xi_c \bar{D}^{*} $ interaction. In the current…

High Energy Physics - Phenomenology · Physics 2021-10-27 Jun-Tao Zhu , Lin-Qing Song , Jun He

As a sister work of Ref.[1], we incorporate the color-screening effect due to light quark pair creation into the heavy quark-antiquark potential, and investigate the effects of screened potential on the spectrum of bottomonium. We calculate…

High Energy Physics - Phenomenology · Physics 2009-11-30 Bai-Qing Li , Kuang-Ta Chao

We discuss the possibility and the description of bound states between $B$ and $\bar{B}^*$ mesons. We argue that the existence of such a bound state can be deduced from (i) the weakly bound X(3872) state, (ii) certain assumptions about the…

High Energy Physics - Phenomenology · Physics 2015-05-28 J. Nieves , M. Pavon Valderrama

The X(3872) and Y(4260), among a host of charmonium-like mesons, have rather unusual properties: the former has very small total width, the latter has large rate into $\pi^+\pi^-J/\psi$ channel. It would not be easy to settle between the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wei-Shu Hou

Compared to charmonium-like states, exotic hadrons associated with $b$-quark offer distinct advantages for exploring the nature of multiquark phenomena and the dynamics of the strong interaction. Due to the heavier bottom quark mass,…

High Energy Physics - Phenomenology · Physics 2026-03-11 Xinchen Dai , Sen Jia , Alexey Nefediev , Juan Nieves , Chengping Shen , Liming Zhang

We re-investigate the possibility of X(3872) as a $D\bar{D}^*$ molecule with $J^{PC}=1^{++}$ within the framework of both the one-pion-exchange (OPE) model and the one-boson-exchange (OBE) model. After careful treatment of the S-D wave…

High Energy Physics - Phenomenology · Physics 2012-10-19 Ning Li , Shi-Lin Zhu

Recent results by BELLE and BaBar point to the existence of a second X particle decaying in D^0 D^0bar pi^0, a few MeV above the X(3872). We identify the two X states with the neutral particles predicted by the 4-quark model and show that…

High Energy Physics - Phenomenology · Physics 2008-11-26 L. Maiani , A. D. Polosa , V. Riquer

The newly observed $Z^+ (4433)$ resonance by BELLE is believed to be a tetraquark bound state made up of $(cu)(\bar c \bar d)$. We propose the bottomed analog of this bound state, namely, by replacing one of the charm quarks by a bottom…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kingman Cheung , Wai-Yee Keung , Tzu-Chiang Yuan

In the framework of the one-boson-exchange model, we have studied the interaction of the $B^*\bar{B}$ and $B^*\bar{B}^{*}$ system. After considering the S-wave and D-wave mixing, we notice that both $Z_b(10610)^\pm$ and $Z_b(10650)^\pm$ can…

High Energy Physics - Phenomenology · Physics 2011-09-02 Zhi-Feng Sun , Jun He , Xiang Liu , Zhi-Gang Luo , Shi-Lin Zhu

The $X(3872)$, as the first and the most crucial member in the exotic charmoniumlike $XYZ$ family, has been studied for a long time. However, its dynamical origin, whether stemming from a $D\bar{D}^*$ hadronic molecule or the first excited…

High Energy Physics - Phenomenology · Physics 2025-06-10 Jun-Zhang Wang , Zi-Yang Lin , Yan-Ke Chen , Lu Meng , Shi-Lin Zhu

Inspired by the LHCb's newest observation of two new excited $\Xi_b^0$ states, we systematically study the strong decays of the low-lying $\lambda$- and $\rho$-modes $1D$-wave $\Xi_{b}$ and $\Xi^{'}_{b}$ baryons using the chiral quark model…

High Energy Physics - Phenomenology · Physics 2022-04-27 Wen-Jia Wang , Yu-Hui Zhou , Li-Ye Xiao , Xian-Hui Zhong

Within the framework of dispersion theory, we analyze the dipion transitions between the lightest $\Upsilon$ states, $\Upsilon(nS) \rightarrow \Upsilon(mS) \pi\pi$ with $m < n \leq 3$. In particular, we consider the possible effects of two…

High Energy Physics - Phenomenology · Physics 2016-03-07 Yun-Hua Chen , Johanna T. Daub , Feng-Kun Guo , Bastian Kubis , Ulf-G. Meißner , Bing-Song Zou