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Related papers: A Refined Analysis on the $X(3872)$ Resonance

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The X(3872) is studied as an axial-vector charmonium state in the multichannel framework of the Resonance-Spectrum-Expansion quark-meson model, previously applied to a variety of other puzzling mesonic resonances. Included are the…

High Energy Physics - Phenomenology · Physics 2015-03-17 S. Coito , G. Rupp , E. van Beveren

We propose a simple explanation for the increase of approximately 3 MeV/c^2 in the mass value of the X(3872) obtained from D^{*0} {D^0}bar decay relative to that obtained from decay to J/psi pi+ pi-. If the total width of the X(3872) is 2-3…

High Energy Physics - Experiment · Physics 2008-11-26 W. Dunwoodie , V. Ziegler

It is pointed out that the internal structure of the narrow resonance X(3872) at the D^0 {\bar D}^{*0} threshold can be studied in some detail by measuring the rate and the spectra in the decays X(3872) \to D^0 {\bar D}^0 \pi^0 and X(3872)…

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

We report the first observation of $B^0 \to X(3872) (K^{+}\pi^{-})$ and evidence for $B^+ \to X(3872) (K^{0}\pi^{+})$. We measure the product of branching fractions for the former to be ${\cal B}(B^0 \to X(3872) (K^+ \pi^-)) \times {\cal…

High Energy Physics - Experiment · Physics 2015-09-14 A. Bala , V. Bhardwaj , K. Trabelsi , J. B. Singh , A. Abdesselam , I. Adachi , H. Aihara , K. Arinstein , D. M. Asner , V. Aulchenko , T. Aushev , R. Ayad , T. Aziz , S. Bahinipati , A. M. Bakich , V. Bansal , E. Barberio , B. Bhuyan , A. Bobrov , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , D. Červenkov , A. Chen , B. G. Cheon , R. Chistov , K. Cho , V. Chobanova , S. -K. Choi , Y. Choi , D. Cinabro , J. Dalseno , J. Dingfelder , Z. Doležal , A. Drutskoy , D. Dutta , S. Eidelman , D. Epifanov , H. Farhat , J. E. Fast , T. Ferber , O. Frost , V. Gaur , N. Gabyshev , A. Garmash , D. Getzkow , Y. M. Goh , B. Golob , O. Grzymkowska , J. Haba , T. Hara , H. Hayashii , X. H. He , A. Heller , T. Horiguchi , W. -S. Hou , M. Huschle , T. Iijima , A. Ishikawa , R. Itoh , Y. Iwasaki , I. Jaegle , D. Joffe , K. H. Kang , E. Kato , T. Kawasaki , C. Kiesling , D. Y. Kim , J. B. Kim , J. H. Kim , K. T. Kim , M. J. Kim , S. H. Kim , Y. J. Kim , K. Kinoshita , B. R. Ko , P. Kodyš , S. Korpar , P. Križan , P. Krokovny , T. Kuhr , R. Kumar , A. Kuzmin , Y. -J. Kwon , J. S. Lange , I. S. Lee , Y. Li , L. Li Gioi , J. Libby , D. Liventsev , P. Lukin , D. Matvienko , K. Miyabayashi , H. Miyake , H. Miyata , R. Mizuk , G. B. Mohanty , S. Mohanty , A. Moll , H. K. Moon , R. Mussa , E. Nakano , M. Nakao , Z. Natkaniec , M. Nayak , N. K. Nisar , S. Nishida , S. Ogawa , S. Okuno , S. L. Olsen , P. Pakhlov , G. Pakhlova , C. W. Park , H. Park , R. Pestotnik , M. Petrič , L. E. Piilonen , E. Ribežl , M. Ritter , Y. Sakai , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , C. Schwanda , K. Senyo , O. Seon , M. E. Sevior , V. Shebalin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , Y. -S. Sohn , A. Sokolov , E. Solovieva , M. Starič , M. Steder , M. Sumihama , T. Sumiyoshi , K. Tanida , G. Tatishvili , Y. Teramoto , F. Thorne , V. Trusov , M. Uchida , S. Uehara , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Usov , P. Vanhoefer , G. Varner , A. Vinokurova , V. Vorobyev , M. N. Wagner , C. H. Wang , X. L. Wang , Y. Watanabe , K. M. Williams , E. Won , H. Yamamoto , Y. Yamashita , S. Yashchenko , C. Z. Yuan , Z. P. Zhang , V. Zhilich , V. Zhulanov , M. Ziegler , A. Zupanc

We construct line shapes for the X(3872) that generalize the Flatte and zero-range line shapes that have been considered previously. These line shapes are associated with scattering amplitudes that are exactly unitary for real values of the…

High Energy Physics - Phenomenology · Physics 2015-03-17 Pierre Artoisenet , Eric Braaten , Daekyoung Kang

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

We re-examine the re-scattering mechanism for the X(3872), as a candidate for the 2P charmonium state $\chi_{c1}(2P)$, decaying to $J/\psi\rho(\omega)$ through exchanging $D^{(*)}$ mesons between intermediate states $D(\bar{D})$ and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ce Meng , Kuang-Ta Chao

We consider the $X(3872)$ resonance as a $J^{PC}=1^{++}$ $D\bar D^*$ hadronic molecule. According to heavy quark spin symmetry, there will exist a partner with quantum numbers $2^{++}$, $X_{2}$, which would be a $D^*\bar D^*$ loosely bound…

High Energy Physics - Phenomenology · Physics 2016-01-20 M. Albaladejo , F. -K. Guo , C. Hidalgo-Duque , J. Nieves , M. Pavon Valderrama

We discuss the possibility that the X(3872) can be a $D\bar{D}^*$ molecular bound state in the Bethe-Salpeter equation approach in the ladder and instantaneous approximations. We show that the $D\bar{D}^*$ bound state with quantum numbers…

High Energy Physics - Phenomenology · Physics 2018-07-02 Zhen-Yang Wang , Jing-Juan Qi , Chao Wang , Xin-Heng Guo

We study the decays $B_{c,u,d}\to X(3872)P$ in the perturbative QCD (PQCD) approach, where the puzzling resonance $X(3872)$ is involved and $P$ represents a light pseudoscalar meson $K$ and $\pi$. Assuming the $X(3872)$ as a $1^{++}$…

High Energy Physics - Phenomenology · Physics 2022-12-21 Zhi-Qing Zhang , Zhi-Lin Guan , Yan-Chao Zhao , Zi-Yu Zhang , Zhi-Jie Sun , Na Wang , Xiao-Dong Ren

We analyze recent data from the Babar and Belle Collaborations on the X(3872) resonance in the J/psi pi+ pi- and D0 D0-bar pi0 decay channels, taking careful account of the universal features of an S-wave threshold resonance. Because the…

High Energy Physics - Phenomenology · Physics 2013-05-29 Eric Braaten James Stapleton

We study the decay B- --> J/psi K- pi+ pi- using 117 million BBbar events collected at the Y(4S) resonance with the BaBar detector at the PEP-II e+ e- asymmetric-energy storage ring. We measure the branching fractions Br(B- --> J/psi K- pi+…

High Energy Physics - Experiment · Physics 2008-11-26 B. Aubert , BaBar Collaboration

The isospin-breaking decay $X(3872)\to(D^*\bar D+ \bar D^*D) \to\pi^0D\bar D\to\pi^0\pi^+\pi^-$ is discussed. In its amplitude there is a triangle logarithmic singularity, due to which the dominant contribution to…

High Energy Physics - Phenomenology · Physics 2019-07-03 N. N. Achasov , G. N. Shestakov

We investigate heavy quark symmetries for heavy meson hadronic molecules, and explore the consequences of assuming the X(3872) and $Z_b(10610)$ as an isoscalar $D\bar D^*$ and an isovector $B\bar B^*$ hadronic molecules, respectively. The…

High Energy Physics - Phenomenology · Physics 2014-09-16 F. -K. Guo , C. Hidalgo-Duque , J. Nieves , A. Ozpineci , M. Pavon Valderrama

We report recent results on the properties of the X(3872) produced via the B+ --> K+ X(3872) decay process. We observe X -->pi+pi-pi0 J/psi decays where the 3pi invariant masses cluster near the upper kinematic boundary suggesting that they…

High Energy Physics - Experiment · Physics 2019-08-14 K. Abe

We search for a charged partner of the X(3872) in the decay B --> X- K, X- --> J/psi pi- pi0, using 234 million BBbar events collected at the Y(4S) resonance with the BaBar detector at the PEP-II e+e- asymmetric-energy storage ring. The…

High Energy Physics - Experiment · Physics 2008-11-26 B. Aubert , BaBar Collaboration

The decay channel J/\psi --> \gamma \pi^+ \pi^- \eta^{\prime} is analyzed using a sample of 5.8\times 10^7 J\psi events collected with the BESII detector. A resonance, the X(1835), is observed in the \pi^+ \pi^- \eta^{\prime} invariant mass…

High Energy Physics - Experiment · Physics 2008-11-26 BES Collaboration , M. Ablikim

The BABAR Collaboration performed a search for xi(2220) production in the initial-state radiation process e^+e^- --> gamma J/psi, J/psi --> gamma K^+K^- or J/psi --> gamma K^0_SK^0_S. No evidence for the xi(2220) resonance has been found.…

High Energy Physics - Experiment · Physics 2011-09-08 Arafat Gabareen Mokhtar

The charmless decay processes of $X(3872)$ provide us a good platform to study the nature and the decay mechanism of $X(3872)$. Based on a molecular nature of $X(3872)$ as a $\bar{D}D^*$ bound state, we have investigated the charmless…

High Energy Physics - Phenomenology · Physics 2022-09-27 Yan Wang , Qi Wu , Gang Li , Wen-Hua Qin , Xiao-Hai Liu , Chun-Sheng An , Ju-Jun Xie

We present a search for the decay $X(3872) \to \pi^+\pi^-\pi^0$ in the $(772\pm11)\times10^6$ $\Upsilon(4S)\to B \bar B$ data sample collected at the Belle detector, where the $X(3872)$ is produced in $B^{\pm}\to K^{\pm}X(3872)$ and…

High Energy Physics - Experiment · Physics 2023-02-21 Belle Collaboration , J. H. Yin , E. Won , I. Adachi , H. Aihara , S. Al Said , D. M. Asner , H. Atmacan , V. Aulchenko , T. Aushev , R. Ayad , V. Babu , S. Bahinipati , P. Behera , K. Belous , J. Bennett , M. Bessner , V. Bhardwaj , B. Bhuyan , T. Bilka , D. Bodrov , G. Bonvicini , J. Borah , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , D. Červenkov , M. -C. Chang , P. Chang , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Das , G. De Pietro , R. Dhamija , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , T. Ferber , D. Ferlewicz , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Garmash , A. Giri , P. Goldenzweig , E. Graziani , K. Gudkova , C. Hadjivasiliou , K. Hayasaka , H. Hayashii , 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 , K. K. Joo , H. Kakuno , K. H. Kang , G. Karyan , T. Kawasaki , 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 , M. Kumar , R. Kumar , K. Kumara , T. Lam , J. S. Lange , S. C. Lee , C. H. Li , J. Li , L. K. Li , Y. Li , Y. B. Li , L. Li Gioi , J. Libby , K. Lieret , M. Masuda , T. Matsuda , D. Matvienko , S. K. Maurya , F. Meier , M. Merola , K. Miyabayashi , R. Mizuk , G. B. Mohanty , H. K. Moon , M. Mrvar , R. Mussa , M. Nakao , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , S. Ogawa , H. Ono , Y. Onuki , P. Oskin , P. Pakhlov , G. Pakhlova , S. Pardi , H. Park , S. -H. Park , S. Patra , S. Paul , R. Pestotnik , L. E. Piilonen , T. Podobnik , E. Prencipe , M. T. Prim , N. Rout , G. Russo , Y. Sakai , S. Sandilya , A. Sangal , L. Santelj , T. Sanuki , V. Savinov , G. Schnell , J. Schueler , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , M. Shapkin , C. Sharma , C. P. Shen , J. -G. Shiu , J. B. Singh , A. Sokolov , E. Solovieva , M. Starič , Z. S. Stottler , J. F. Strube , M. Sumihama , K. Sumisawa , T. Sumiyoshi , M. Takizawa , U. Tamponi , K. Tanida , M. Uchida , T. Uglov , Y. Unno , K. Uno , S. Uno , R. van Tonder , G. Varner , A. Vinokurova , E. Waheed , E. Wang , M. -Z. Wang , M. Watanabe , S. Watanuki , B. D. Yabsley , W. Yan , S. B. Yang , C. Z. Yuan , Y. Yusa , Y. Zhai , Z. P. Zhang , V. Zhilich , V. Zhukova , V. Zhulanov