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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

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

Bottomonium-like resonances Zb(10610) and Zb'(10650) are good candidates of hadronic molecules composed of BBbar* (or B*Bbar) and B*Bbar*, respectively. Considering Zb (Zb') as heavy meson molecules, we investigate the decays of Zb(')^+ ->…

High Energy Physics - Phenomenology · Physics 2014-04-23 Shunsuke Ohkoda , Shigehiro Yasui , Atsushi Hosaka

We have evaluated the decay modes of the $\Upsilon(4s), \Upsilon(3d), \Upsilon(5s), \Upsilon(6s)$ states into $B\bar B, B\bar B^*+c.c., B^* \bar B^*, B_s \bar B_s, B_s \bar B^*_s +c.c., B^*_s \bar B_s^* $ using the $^3P_0$ model to…

High Energy Physics - Phenomenology · Physics 2020-03-11 Wei-Hong Liang , Natsumi Ikeno , Eulogio Oset

The decays of the $Z_b(10610)$ and the $Z_b(10650)$ to $\Upsilon(nS)\pi$, $h_b(mP)\pi$ and $\chi_{bJ}(mP)\gamma$ ($n=1,2,3$, $m=1,2$ and $J=0,1,2$) are investigated within a nonrelativistic effective field theory. It is argued that, while…

High Energy Physics - Phenomenology · Physics 2013-04-25 Martin Cleven , Qian Wang , Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner , Qiang Zhao

The $\Upsilon(10753)$ state has been recently observed by the Belle and Belle~II collaborations with enough global significance to motivate an assessment of the high-energy spectrum usually predicted by any reasonable \emph{na\"ive} quark…

High Energy Physics - Phenomenology · Physics 2024-03-07 P. G. Ortega , D. R. Entem , F. Fernández , J. Segovia

At least one state in the first family of D-wave $b \bar b$ quarkonium levels has been discovered near the predicted mass of 10.16 GeV/$c^2$. This state is probably the one with J=2. This state and the ones with J=1 and J=3 may contribute a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jonathan L. Rosner

Heavy quark spin symmetry is useful to make predictions on ratios of decay or production rates of systems involving heavy quarks. The breaking of spin symmetry is generally of the order of $O({\Lambda_{\rm QCD}/m_Q})$, with $\Lambda_{\rm…

High Energy Physics - Phenomenology · Physics 2014-10-14 Feng-Kun Guo , Ulf-G. Meißner , Cheng-Ping Shen

The Belle collaboration recently discovered two resonances, $Z_b(10610)$ and $Z_b(10650)$ --- denoted $Z_b$ and $Z_b^\prime$ --- in the decays $\Upsilon(5S) \to \Upsilon(nS) \pi^+ \pi^-$ for $n$ = 1, 2, or 3, and $\Upsilon(5S) \to h_b(mP)…

High Energy Physics - Phenomenology · Physics 2015-06-16 Thomas Mehen , Josh Powell

We calculate the masses and leptonic decay widths of the bottomonium $b\bar b$ and charmonium $c\bar c$ states in a constituent quark model where the Cornell-like potential and spin-dependent interaction are employed, with all model…

Recent data from Belle show unusually large partial widths Upsilon(5S) --> Upsilon(1S) pi^+pi^- and \Upsilon(5S) --> \Upsilon(2S) pi^+ pi^-. The Z(4430) narrow resonance also reported by Belle in psi' pi^+ spectrum has the properties…

High Energy Physics - Phenomenology · Physics 2008-03-04 Marek Karliner , Harry J. Lipkin

The dipion transitions $\Upsilon(10860)\to\pi^+\pi^-\Upsilon(nS)$ ($n=1,2,3$) are studied in the framework of a unitary and analytic coupled-channel formalism previously developed for analysing experimental data on the bottomoniumlike…

High Energy Physics - Phenomenology · Physics 2021-02-24 V. Baru , E. Epelbaum , A. A. Filin , C. Hanhart , R. V. Mizuk , A. V. Nefediev , S. Ropertz

We report new measurements of the total cross sections for $e^+e^-\to \Upsilon(n{\rm S})\pi^+\pi^-$ ($n$ = 1, 2, 3) and $e^+e^-\to b\bar b$ from a high-luminosity fine scan of the region $\sqrt{s} = 10.63$-$11.05$ GeV with the Belle…

High Energy Physics - Experiment · Physics 2016-09-20 Belle Collaboration , D. Santel , K. Kinoshita , P. Chang , A. Abdesselam , I. Adachi , H. Aihara , S. Al Said , K. Arinstein , D. M. Asner , T. Aushev , R. Ayad , A. M. Bakich , V. Bansal , B. Bhuyan , A. Bobrov , A. Bondar , G. Bonvicini , M. Bračko , T. E. Browder , D. Červenkov , V. Chekelian , B. G. Cheon , K. Chilikin , K. Cho , V. Chobanova , S. -K. Choi , Y. Choi , D. Cinabro , J. Dalseno , M. Danilov , J. Dingfelder , Z. Doležal , Z. Drásal , A. Drutskoy , S. Eidelman , H. Farhat , J. E. Fast , T. Ferber , V. Gaur , N. Gabyshev , A. Garmash , D. Getzkow , R. Gillard , Y. M. Goh , J. Haba , T. Hara , K. Hayasaka , H. Hayashii , X. H. He , W. -S. Hou , H. J. Hyun , T. Iijima , K. Inami , A. Ishikawa , R. Itoh , Y. Iwasaki , I. Jaegle , D. Joffe , T. Julius , K. H. Kang , E. Kato , T. Kawasaki , C. Kiesling , D. Y. Kim , H. J. Kim , J. B. Kim , J. H. Kim , M. J. Kim , S. H. Kim , Y. J. Kim , B. R. Ko , P. Kodyš , S. Korpar , P. Križan , P. Krokovny , A. Kuzmin , J. S. Lange , I. S. Lee , Y. Li , L. Li Gioi , J. Libby , D. Liventsev , P. Lukin , D. Matvienko , K. Miyabayashi , H. Miyata , R. Mizuk , G. B. Mohanty , A. Moll , T. Mori , R. Mussa , E. Nakano , M. Nakao , T. Nanut , Z. Natkaniec , N. K. Nisar , S. Nishida , S. Ogawa , S. Okuno , S. L. Olsen , C. Oswald , P. Pakhlov , G. Pakhlova , C. W. Park , H. Park , T. K. Pedlar , M. Petrič , L. E. Piilonen , E. Ribežl , M. Ritter , A. Rostomyan , S. Ryu , Y. Sakai , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , C. Schwanda , A. J. Schwartz , K. Senyo , M. E. Sevior , V. Shebalin , T. -A. Shibata , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , Y. -S. Sohn , E. Solovieva , M. Starič , M. Steder , U. Tamponi , G. Tatishvili , Y. Teramoto , K. Trabelsi , M. Uchida , T. Uglov , Y. Unno , S. Uno , C. Van Hulse , P. Vanhoefer , G. Varner , A. Vinokurova , M. N. Wagner , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , E. Won , J. Yamaoka , Y. -P. Yang , S. Yashchenko , Y. Yook , Y. Yusa , Z. P. Zhang , V. Zhilich , V. Zhulanov , A. Zupanc

Under the Initial Single Pion Emission mechanism, we study the hidden-bottom dipion decays of $\Upsilon(11020)$, i.e., $\Upsilon(11020)\to \Upsilon(nS)\pi^+\pi^-$ $(n=1,2,3)$ and $\Upsilon(11020)\to h_b(mP)\pi^+\pi^-$ $(m=1,2)$. We predict…

High Energy Physics - Phenomenology · Physics 2011-10-25 Dian-Yong Chen , Xiang Liu , Takayuki Matsuki

Motivated by the two charged bottomonium-like resonances $Z_b$(10610) and $Z_b$(10650) newly observed by the Belle collaboration, the possible molecular states composed of a pair of heavy mesons, $B\bar{B}, B\bar{B}^*, B^*\bar{B}^*,…

High Energy Physics - Phenomenology · Physics 2015-05-28 Youchang Yang , Jialun Ping , Chengrong Deng , Hong-Shi Zong

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

The $D_s(2320)$ state recently observed by BaBar in the $D_s^+\pi^0$ channel may be the first of a host of $cq\bar q\bar q$ four-quark states. We give a phenomenological account of the masses and decay modes. The isosinglet $D_s(2320)$…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hai-Yang Cheng , Wei-Shu Hou

We examine the electronic width ratios of Upsilon resonances below the BBbar threshold by means of an effective (Cornell-type) QCD potential incorporating 1/m_b corrections obtained from a prior fit to the bottomonium spectrum. From our…

High Energy Physics - Phenomenology · Physics 2008-11-26 Juan-Luis Domenech-Garret , Miguel-Angel Sanchis-Lozano

We perform a theoretical study of the decay process $\Upsilon \to D^{-} \bar{B}^{0} D_s^{+}$ in search of the doubly heavy tetraquark states $T_{bc\bar{s}}$ with quark content $bc\bar{s}\bar{d}$. These $T_{bc\bar{s}}$ states are assumed to…

High Energy Physics - Phenomenology · Physics 2025-08-27 Wen-Ying Liu , Hua-Xing Chen

The $Z_b(10610)^\pm$ and $Z_b(10650)^\pm$ are two bottomonium-like structures discovered in the $\pi h_b(mP)$, $\pi \Upsilon(nS)$ and $B^\ast\bar B^{(\ast)}+h.c.$ invariant mass spectra, where $m=\{1,2\}$ and $n=\{1,2,3\}$. Their nature is…

High Energy Physics - Phenomenology · Physics 2021-11-17 Pablo G. Ortega , Jorge Segovia , Francisco Fernandez
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