English
Related papers

Related papers: Bottomonium dipion transitions

200 papers

Using data collected by the CLEO detector in the Upsilon(4S) region, we report new measurements of the exclusive decays of B mesons into final states of the type Lambda_c^+ p-bar n(pi), where n=0,1,2,3. We find signals in modes with one,…

High Energy Physics - Experiment · Physics 2010-04-08 S. A Dytman , CLEO Collaboration

It is shown that the basic shape of dipion mass distributions in the two-pion transitions of both charmonia and bottomonia states are explained by an unified mechanism based on the contribution of the $\pi\pi$, $K\overline{K}$ and…

High Energy Physics - Phenomenology · Physics 2016-12-21 Yu. S. Surovtsev , P. Bydžovský , T. Gutsche , R. Kamiński , V. E. Lyubovitskij , M. Nagy

We present a comprehensive study of the electronic transitions in neutral cadmium (Cd I) with a focus on forbidden transitions, motivated by recent advances in laser technology and the growing relevance of cadmium in quantum gas research,…

Atomic Physics · Physics 2025-10-07 P. J. Robert , S. Manzoor , M. Chiarotti , N. Poli

We investigate the quantum phase transitions of bosonic polar molecules in a two-dimensional double layer system. We show that an interlayer bound state of dipoles (dimers) can be formed when the dipole strength is above a critical value,…

Other Condensed Matter · Physics 2007-05-23 Daw-Wei Wang

The mixing of $S-D$ partial waves for the heavy meson pairs in the decays $\Upsilon(5S) \to [B^* \bar B+ {\rm c.c.}] \pi$ and $\Upsilon(5S) \to B^* \bar B^* \pi$ is considered. It is argued that this mixing, enhanced by the heavy meson…

High Energy Physics - Phenomenology · Physics 2013-04-17 M. B. Voloshin

We study the rare hadronic transitions $\Upsilon(2S)\rightarrow \Upsilon(1S)\eta$ and $\Upsilon(2S)\rightarrow \Upsilon(1S)\pi^0$ using a sample of 158 $\times 10^6$ $\Upsilon(2S)$ decays collected with the Belle detector at the KEKB…

High Energy Physics - Experiment · Physics 2013-05-30 Belle Collaboration , U. Tamponi , R. Mussa , I. Adachi , H. Aihara , D. M. Asner , V. Aulchenko , T. Aushev , A. M. Bakich , M. Barrett , B. Bhuyan , A. Bondar , A. Bozek , M. Bra\v , T. E. Browder , A. Chen , P. Chen , B. G. Cheon , K. Chilikin , I. -S. Cho , K. Cho , Y. Choi , J. Dalseno , Z. Dole\v , Z. Drásal , D. Dutta , S. Eidelman , D. Epifanov , S. Esen , H. Farhat , J. E. Fast , A. Frey , V. Gaur , R. Gillard , Y. M. Goh , B. Golob , K. Hayasaka , Y. Horii , Y. Hoshi , H. J. Hyun , T. Iijima , A. Ishikawa , Y. Iwasaki , I. Jaegle , J. H. Kang , T. Kawasaki , H. O. Kim , J. H. Kim , K. T. Kim , M. J. Kim , Y. J. Kim , J. Klucar , B. R. Ko , P. Kody\v , S. Korpar , R. T. Kouzes , P. Kri\v , P. Krokovny , T. Kumita , A. Kuzmin , S. -H. Lee , Y. Li , C. Liu , Y. Liu , Z. Q. Liu , D. Liventsev , H. Miyata , R. Mizuk , G. B. Mohanty , A. Moll , N. Muramatsu , M. Nakao , Z. Natkaniec , C. Ng , S. Nishida , O. Nitoh , S. Ogawa , T. Ohshima , S. Okuno , S. L. Olsen , Y. Onuki , P. Pakhlov , H. K. Park , K. S. Park , T. K. Pedlar , R. Pestotnik , M. Petri\v , L. E. Piilonen , M. Röhrken , Y. Sakai , S. Sandilya , D. Santel , L. Santelj , T. Sanuki , O. Schneider , G. Schnell , C. Schwanda , K. Senyo , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , F. Simon , P. Smerkol , Y. -S. Sohn , A. Sokolov , E. Solovieva , M. Stari\v , T. Sumiyoshi , K. Tanida , N. Taniguchi , G. Tatishvili , Y. Teramoto , K. Trabelsi , S. Uehara , S. Uno , C. Van Hulse , P. Vanhoefer , G. Varner , C. H. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , K. M. Williams , E. Won , B. D. Yabsley , Y. Yamashita , C. Z. Yuan , Z. P. Zhang , V. Zhilich , V. Zhulanov , A. Zupanc

The effect of isoscalar S-wave multi-channel pion-pion scattering ($\pi\pi\to\pi\pi,K\bar{K},\eta\eta$) is considered in the analysis of data on decays of the $\Upsilon$-meson family -- $\Upsilon(2S)\to\Upsilon(1S)\pi\pi$,…

High Energy Physics - Phenomenology · Physics 2014-10-14 Yu. S. Surovtsev , P. Bydzovsky , T. Gutsche , R. Kaminski , V. E. Lyubovitskij , M. Nagy

The results of a search for the bottomonium counterpart, denoted as Xb, of the exotic charmonium state X(3872) is presented. The analysis is based on a sample of pp collisions at sqrt(s) = 8 TeV collected by the CMS experiment at the LHC,…

High Energy Physics - Experiment · Physics 2013-11-12 CMS Collaboration

Recent progress on the bottomonium states is reported. This talk briefly reviews the observation of $h_b(1P), h_b(2P), Z_{b1}^+, Z_{b2}^+$ states, transition of $h_b(nP)\to \eta_b(mS)\gamma$ and new studies on the $\eta_b(2S)$ state. Other…

High Energy Physics - Experiment · Physics 2012-09-21 Jin Li

We make comments on ref.[Z.Phys. C73, 541 (1997)], and provide partial wave analysis to the decays of excited heavy S-wave $1^-$ quarkonia into the basic $1^-$ quarkonia state plus $\pi\pi$. It is revealed that there exist contributions of…

High Energy Physics - Phenomenology · Physics 2011-09-13 Mu-Lin Yan , Yi Wei , Ting-Liang Zhuang

Based on a data sample of an integrated luminosity of 57.4 fb-1 at the Upsilon(4S) resonance taken with the BaBar detector using the SLAC PEP-II asymmetric-energy $B$-Factory, hadronic decays of B meson with the final states D(*) and three…

High Energy Physics - Experiment · Physics 2007-05-23 H. W. Zhao

We report a search for the decays $B^{0} \to D_{s}^{-} D_{s}^{+}$, $B^{0} \to D_{s}^{*-} D_{s}^{+}$, $B^{0} \to D_{s}^{*-} D_{s}^{*+}$ in a sample of 232 million $\Upsilon(4S)$ decays to \BBb ~pairs collected with the \babar detector at the…

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

We consider the isospin one-half example system, with $D \,\pi , D\,\eta, D_s \bar K, D^* \pi , D^*\eta, D^*\bar K$ coupled channels in the $J^P = 1^-$ partial wave, chosen such that various phenomena that come with the opening of an…

High Energy Physics - Phenomenology · Physics 2023-03-08 Csaba L. Korpa , Matthias F. M. Lutz , Xiao-Yu Guo , Yonggoo Heo

We studied the radiative transitions between the $\Upsilon(10753)$, the $S$-$D$ mixed state of the $\Upsilon(4S)$ and $\Upsilon_1(3\,{}^3D_1)$, and the $X_b$, the heavy quark flavor symmetry counterpart of the $X(3782)$ in the bottomonium…

High Energy Physics - Phenomenology · Physics 2024-05-13 Shi-Dong Liu , Hao-Dong Cai , Zu-Xin Cai , Hong-Shuo Gao , Gang Li , Fan Wang , Ju-Jun Xie

Using 9.32, 5.88 million Upsilon(2S,3S) decays taken with the CLEO-III detector, we obtain five product branching fractions for the exclusive processes Upsilon(2S) => gamma chi_{b0,1,2}(1P) => gamma gamma Upsilon(1S) and Upsilon(3S) =>…

Great strides have been made in the understanding of bound states of a bottom quark $b$ and its antiquark $\bar b$ since the discovery of the first $\Upsilon$ resonances in 1977. These {\it bottomonium} bound states have a rich spectrum…

High Energy Physics - Experiment · Physics 2017-08-23 Claudia Patrignani , Todd K. Pedlar , Jonathan L. Rosner

In this paper, we model $\Upsilon(10753)$ as a $4S$-$3D$ bottomonium mixture and $\Upsilon(10860)$ as a $5S$-$4D$ mixture, and predict the properties of a new bottomonium state, $\Upsilon(10950)$, as the mixing partner of $\Upsilon(10860)$.…

High Energy Physics - Phenomenology · Physics 2025-10-20 Zheng-Li Luo , Yi-Lin Song , Feng-Kun Guo

We investigate the radiative decay $\Upsilon(10753) \to \gamma X_{b0}$ within the framework of nonrelativistic effective field theory (NREFT). The $\Upsilon(10753)$ is treated as an $S$-$D$ mixed state of the $\Upsilon(4S)$ and $\YD$, while…

High Energy Physics - Phenomenology · Physics 2026-05-05 Yuan-Jun Gao , Gang Li , Shi-Dong Liu , Qi Wu

Inspired by the newly observed two charged bottomonium-like states, we consider the possible contribution from the intermediate $Z_b(10610)$ and $Z_b(10650)$ states to the $\Upsilon(5S)\to \Upsilon(2S)\pi^+\pi^-$ decay process, which…

High Energy Physics - Phenomenology · Physics 2011-10-13 Dian-Yong Chen , Xiang Liu , Shi-Lin Zhu

We consider hadronic transitions from the $h_b(2P)$ bottomonium resonance to lower states of bottomonium with emission of either $\omega$ meson, or two pions, or $\eta$ meson. For the former two transitions the branching ratios are related…

High Energy Physics - Phenomenology · Physics 2013-05-30 Xin Li , M. B. Voloshin
‹ Prev 1 4 5 6 7 8 10 Next ›