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

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We investigate the decays of $B^0 \to K^0 X(3872)$ and $B^+ \to K^+ X(3872)$ based on the picture where the $X(3872)$ resonance is strongly coupled to the $D\bar{D}^* + c.c.$ channel. In addition to the decay mechanism where the $X(3872)$…

High Energy Physics - Phenomenology · Physics 2022-11-29 Hao-Nan Wang , Li-Sheng Geng , Qian Wang , Ju-Jun Xie

We present a study of $B\to X(3872)K$ with X(3872) decaying to $D^{*0}\bar D^0$ using a sample of 657 million $B\bar B$ pairs recorded at the $\Upsilon(4S)$ resonance with the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider.…

High Energy Physics - Experiment · Physics 2019-08-13 T. Aushev , N. Zwahlen

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 investigate the enhancement in the D^0\bar{D}^0\pi^0 final state with the mass M=3875.2\pm 0.7^{+0.3}_{-1.6}\pm 0.8 MeV found recently by the Belle Collaboration in the B\to K D^0\bar{D}^0\pi^0 decay and test the possibility that this is…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Hanhart , Yu. S. Kalashnikova , A. E. Kudryavtsev , A. V. Nefediev

We construct spectra of decays of the resonance X(3872) with good analytical and unitary properties which allows to define the branching ratio of the X(3872) \to D^{*0}\bar D^0 + c.c. decay studying only one more decay, for example, the…

High Energy Physics - Phenomenology · Physics 2015-10-27 N. N. Achasov , E. V. Rogozina

We present results from a study of X(3872) --> pi+pi- J/psi decays produced via exclusive B--> K X(3872) decays. We determine the mass to be M_X(3872)= (3871.84\pm 0.27 (stat)\pm 0.19 (syst)) MeV, a 90% CL upper limit on the natural width…

High Energy Physics - Experiment · Physics 2013-05-29 S. -K. Choi , S. L. Olsen , K. Trabelsi

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

Triangle mechanisms for $B^0\to (J/\psi\pi^+\pi^-) K^+\pi^-$ are studied. Experimentally, an $X(3872)$ peak has been observed in this process. When the final $(J/\psi\pi^+\pi^-)\pi$ invariant mass is around the $D^*\bar D^*$ threshold, one…

High Energy Physics - Phenomenology · Physics 2021-07-14 Satoshi X. Nakamura

We present results on the X(3872), produced in $B^+ \to X(3872) K^+$ and $B^0 \to X(3872) K^0_S$ decays where $X(3872) \to J/\psi \pi^+ \pi^-$. We report the first statistically significant observation of $B^0 \to X(3872) K^0_S$ and measure…

High Energy Physics - Experiment · Physics 2012-08-27 Belle collaboration

We study the non-Breit-Wigner line-shape of the $\psi(3770)$ resonance, predominantly a $1\ ^{3}D_{1}$ $\bar{c}c$ state, using an unitarized effective Lagrangian approach, including the one-loop effects of the nearby thresholds $D^+D^-$ and…

High Energy Physics - Phenomenology · Physics 2019-02-26 Susana Coito , Francesco Giacosa

The X(3872) resonance is considered as a hadronic molecule, a loosely-bound state of charmed D0 and D*0 mesons, since its mass is very close to the D*0 barD0 threshold. Assuming structure and quantum numbers of X(3872) as (D0 barD*0 - D*0…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yubing Dong , Amand Faessler , Thomas Gutsche , Valery E. Lyubovitskij

We study the $e^+e^-\to\gamma\omega J/\psi$ process using $11.6 ~\rm fb^{-1}$ $e^+ e^-$ annihilation data taken at center-of-mass energies from $\sqrt{s}=4.008~\rm GeV$ to $4.600~\rm GeV$ with the BESIII detector at the BEPCII storage ring.…

High Energy Physics - Experiment · Physics 2019-06-19 M Ablikim , M N Achasov , P Adlarson , S. Ahmed , M Albrecht , M Alekseev , A Amoroso , F F An , Q An , Y Bai , O Bakina , R Baldini Ferroli , I Balossino , Y Ban , K Begzsuren , J V Bennett , N Berger , M Bertani , D Bettoni , F Bianchi , J Biernat , J Bloms , I Boyko , R A Briere , H Cai , X Cai , A Calcaterra , G F Cao , N Cao , S A Cetin , J Chai , J F Chang , W L Chang , G Chelkov , D Y Chen , G Chen , H S Chen , J C Chen , M L Chen , S J Chen , Y B Chen , W Cheng , G Cibinetto , F Cossio , X F Cui , H L Dai , J P Dai , X C Dai , A Dbeyssi , D Dedovich , Z Y Deng , A Denig , I Denysenko , M Destefanis , F De Mori , Y Ding , C Dong , J Dong , L Y Dong , M Y Dong , Z L Dou , S X Du , J Z Fan , J Fang , S S Fang , Y Fang , R Farinelli , L Fava , F Feldbauer , G Felici , C Q Feng , M Fritsch , C D Fu , Y Fu , Q Gao , X L Gao , Y Gao , Y Gao , Y G Gao , Z Gao , B. Garillon , I Garzia , E M Gersabeck , A Gilman , K Goetzen , L Gong , W X Gong , W Gradl , M Greco , L M Gu , M H Gu , S Gu , Y T Gu , A Q Guo , L B Guo , R P Guo , Y P Guo , A Guskov , S Han , X Q Hao , F A Harris , K L He , F H Heinsius , T Held , Y K Heng , Y R Hou , Z L Hou , H M Hu , J F Hu , T Hu , Y Hu , G S Huang , J S Huang , X T Huang , X Z Huang , N Huesken , T Hussain , W Ikegami Andersson , W Imoehl , M Irshad , Q Ji , Q P Ji , X B Ji , X L Ji , H L Jiang , X S Jiang , X Y Jiang , J B Jiao , Z Jiao , D P Jin , S Jin , Y Jin , T Johansson , N Kalantar-Nayestanaki , X S Kang , R Kappert , M Kavatsyuk , B C Ke , I K Keshk , A Khoukaz , P. Kiese , R Kiuchi , R Kliemt , L Koch , O B Kolcu , B Kopf , M Kuemmel , M Kuessner , A Kupsc , M Kurth , M G Kurth , W Kühn , J S Lange , P. Larin , L Lavezzi , H Leithoff , T Lenz , C Li , Cheng Li , D M Li , F Li , F Y Li , G Li , H B Li , H J Li , J C Li , J W Li , Ke Li , L K Li , Lei Li , P L Li , P R Li , Q Y Li , W D Li , W G Li , X H Li , X L Li , X N Li , X Q Li , Z B Li , Z Y Li , H Liang , H Liang , Y F Liang , Y T Liang , G R Liao , L Z Liao , J Libby , C X Lin , D X Lin , Y J Lin , B Liu , B J Liu , C X Liu , D Liu , D Y Liu , F H Liu , Fang Liu , Feng Liu , H B Liu , H M Liu , Huanhuan Liu , Huihui Liu , J B Liu , J Y Liu , K Y Liu , Ke Liu , L Y Liu , Q Liu , S B Liu , T Liu , X Liu , X Y Liu , Y B Liu , Z A Liu , Zhiqing Liu , Y. F Long , X C Lou , H J Lu , J D Lu , J G Lu , Y Lu , Y P Lu , C L Luo , M X Luo , P W Luo , T Luo , X L Luo , S Lusso , X R Lyu , F C Ma , H L Ma , L L. Ma , M M Ma , Q M Ma , X N Ma , X X Ma , X Y Ma , Y M Ma , F E Maas , M Maggiora , S Maldaner , S Malde , Q A Malik , A Mangoni , Y J Mao , Z P Mao , S Marcello , Z X Meng , J G Messchendorp , G Mezzadri , J Min , T J Min , R E Mitchell , X H Mo , Y J Mo , C Morales Morales , N Yu Muchnoi , H Muramatsu , A Mustafa , S Nakhoul , Y Nefedov , F Nerling , I B Nikolaev , Z Ning , S Nisar , S L Niu , S L Olsen , Q Ouyang , S Pacetti , Y Pan , M Papenbrock , P Patteri , M Pelizaeus , H P Peng , K Peters , J Pettersson , J L Ping , R G Ping , A Pitka , R Poling , V Prasad , M Qi , T Y Qi , S Qian , C F Qiao , N Qin , X P Qin , X S Qin , Z H Qin , J F Qiu , S Q Qu , K H Rashid , C F Redmer , M Richter , A Rivetti , V Rodin , M Rolo , G Rong , Ch Rosner , M Rump , A Sarantsev , M Savrié , K Schoenning , W Shan , X Y Shan , M Shao , C P Shen , P X Shen , X Y Shen , H Y Sheng , X Shi , X D Shi , J J Song , Q Q Song , X Y Song , S Sosio , C Sowa , S Spataro , F F. Sui , G X Sun , J F Sun , L Sun , S S Sun , X H Sun , Y J Sun , Y K Sun , Y Z Sun , Z J Sun , Z T Sun , Y T Tan , C J Tang , G Y Tang , X Tang , V Thoren , B Tsednee , I Uman , B Wang , B L Wang , C W Wang , D Y Wang , H H Wang , K Wang , L L Wang , L S Wang , M Wang , M Z Wang , Meng Wang , P L Wang , R M Wang , W P Wang , X Wang , X F Wang , X L Wang , Y Wang , Y Wang , Y F Wang , Z Wang , Z G Wang , Z Y Wang , Zongyuan Wang , T Weber , D H Wei , P Weidenkaff , H W Wen , S P Wen , U Wiedner , G Wilkinson , M Wolke , L H Wu , L J Wu , Z Wu , L Xia , Y Xia , S Y Xiao , Y J Xiao , Z J Xiao , Y G Xie , Y H Xie , T Y Xing , X A Xiong , Q L Xiu , G F Xu , L Xu , Q J Xu , W Xu , X P Xu , F Yan , L Yan , W B Yan , W C Yan , Y H Yan , H J Yang , H X Yang , L Yang , R X Yang , S L Yang , Y H Yang , Y X Yang , Yifan Yang , Z Q Yang , M Ye , M H Ye , J H Yin , Z Y You , B X Yu , C X Yu , J S Yu , C Z Yuan , X Q Yuan , Y Yuan , A Yuncu , A A Zafar , Y Zeng , B X Zhang , B Y Zhang , C C Zhang , D H Zhang , H H Zhang , H Y Zhang , J Zhang , J L Zhang , J Q Zhang , J W Zhang , J Y Zhang , J Z Zhang , K Zhang , L Zhang , S F Zhang , T J Zhang , X Y Zhang , Y Zhang , Y H Zhang , Y T Zhang , Yang Zhang , Yao Zhang , Yi Zhang , Yu Zhang , Z H Zhang , Z P Zhang , Z Y Zhang , G Zhao , J W Zhao , J Y Zhao , J Z Zhao , Lei Zhao , Ling Zhao , M G Zhao , Q Zhao , S J Zhao , T C Zhao , Y B Zhao , Z G Zhao , A Zhemchugov , B Zheng , J P Zheng , Y Zheng , Y H Zheng , B Zhong , L Zhou , L P Zhou , Q Zhou , X Zhou , X K Zhou , X R Zhou , Xiaoyu Zhou , Xu Zhou , A N Zhu , J Zhu , J Zhu , K Zhu , K J Zhu , S H Zhu , W J Zhu , X L Zhu , Y C Zhu , Y S Zhu , Z A Zhu , J Zhuang , B S Zou , J H Zou

We investigate the role of the electromagnetic interaction in the formation and decay of the $X(3872)$. The binding properties of the $X(3872)$ are studied by assuming the molecular nature and considering the $S$-$D$ wave mixing, isospin…

High Energy Physics - Phenomenology · Physics 2024-05-03 Ping Chen , Zhan-Wei Liu , Zi-Le Zhang , Si-Qiang Luo , Fu-Lai Wang , Jun-Zhang Wang , Xiang Liu

We present results of a search for the X(3872) in B0-->X(3872)KS0,X(3872)-->J/psi pi+ pi-, improved measurements of B-->X(3872)K-, and a study of the J/psi pi+ pi- mass region above the X(3872). We use 232x106 B[overline B] pairs collected…

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

We investigate the $B^0\to \pi^- K^+ X(3872)$ decay via the $D_{s1}(2536)\bar{D} D^*$ rescattering diagram. The line shape of the $K^+X(3872)$ distribution curve around $D_{s1}(2536)\bar{D}$ threshold is very sensitive to the $X(3872)$ mass…

High Energy Physics - Phenomenology · Physics 2022-12-14 Mao-Jun Yan , Ying-Hui Ge , Xiao-Hai Liu

We study $D\bar{D}^*$ ($D^*\bar{D}$) scattering in the framework of unitarized heavy meson chiral perturbation theory with pion exchange and a contact interaction. $^3S_1-$$^3D_1$ mixing effects are taken into account. A loosely bound state…

High Energy Physics - Phenomenology · Physics 2013-04-04 P. Wang , X. G. Wang

We present a quark model calculation of the charmonium spectrum with self energy corrections due to the coupling to the meson-meson continuum. The bare masses used in the calculation are computed within the relativized quark model by…

High Energy Physics - Phenomenology · Physics 2015-10-05 J. Ferretti , G. Galatà , E. Santopinto

From a picture of the X(3872) where the resonance is a bound state of $\bar{D}D^*-c.c.$, we evaluate the decay width into the $J/\psi \gamma$ channel, which is sensitive to the internal structure of this state. For this purpose we evaluate…

High Energy Physics - Phenomenology · Physics 2013-05-30 F. Aceti , R. Molina , E. Oset

We present measurements of the decays B+ -> X(3872) K+ and B0 -> X(3872) K0 with X(3872) -> Jpsi pi+ pi-. The data sample used, collected with the BABAR detector at the PEP-II e+e- asymmetric-energy storage ring, corresponds to 455 x 10^6…

High Energy Physics - Experiment · Physics 2010-04-12 The BABAR Collaboration , B. Aubert

We report on the search for a charged partner of the X(3872) in the decay $B \to X^\pm K$, $X^\pm \to J/\psi \pi^\pm \pi^0$, using 213 million $B\bar B$ events collected at the $\Upsilon(4S)$ resonance with the BaBar detector at the PEP-II…

High Energy Physics - Experiment · Physics 2007-05-23 The BABAR Collaboration , B. Aubert
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