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Related papers: Doubly Heavy Baryon Xi_cc Production in Upsilon (1…

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Belle and Belle II experiments have collected $e^+e^-$ collision data with center-of-mass energies at or near the $\Upsilon(4S)$ resonance. Using total $1.4\,\mathrm{ab}^{-1}$ combined dataset, we present new measurements of branching…

High Energy Physics - Experiment · Physics 2026-03-24 Jaeyoung Kim

Theoretical predictions for inclusive semileptonic B decay rates are rewritten in terms of the Upsilon(1S) meson mass instead of the b quark mass, using a modified perturbation expansion. This method gives theoretically consistent and…

High Energy Physics - Phenomenology · Physics 2009-10-31 Andre H. Hoang , Zoltan Ligeti , Aneesh V. Manohar

We investigate the production of $X_b$ in the process $\Upsilon(5S,6S)\to \gamma X_b$, where $X_b$ is assumed to be a $B {\bar B}^*$ molecular state. Two kinds of meson loops of $B^{(*)}{\bar B}^{(*)}$ and $B_1^{\prime}{\bar B}^{(*)}$ were…

High Energy Physics - Phenomenology · Physics 2023-03-22 Xiao-Yun Wang , Zu-Xin Cai , Gang Li , Shi-Dong Liu , Chun-Sheng An , Ju-Jun Xie

We systematically analyzed the production of semi-inclusive doubly heavy baryons ($\Xi_{cc}$, $\Xi_{bc}$ and $\Xi_{bb}$) for the process $H^0 \rightarrow \Xi_{QQ'}+ \bar {Q'} + \bar {Q}$ through four main Higgs decay channels within the…

High Energy Physics - Phenomenology · Physics 2019-04-17 Juan-Juan Niu , Lei Guo , Hong-Hao Ma , Xing-Gang Wu

We study flavor changing processes $\Upsilon \to B/{\bar B} X_s$ and $J/\psi \to D/{\bar D} X_u$ in the B factories and the Tau-Charm factories. In the standard model, these processes are predicted to be unobservable, so they serve as a…

High Energy Physics - Phenomenology · Physics 2009-10-31 Alakabha Datta , Patrick. J. O'Donnell , Sandip Pakvasa , Xinmin Zhang

With anticipation of abundant Upsilons data sample at high-luminosity heavy-flavor experiments in the future, we studied nonleptonic two-body weak decays of ${\Upsilon}(nS)$ below the open-bottom threshold with $n$ $=$ $1$, $2$ and $3$. It…

High Energy Physics - Phenomenology · Physics 2016-10-30 Junfeng Sun , Lili Chen , Na Wang , Jinshu Huang , Yueling Yang , Qin Chang

We study the $\Upsilon$ exclusive decay into double charmonium, specifically, the $S$-wave charmonium $ J/\psi$ plus the $P$-wave charmonium $\chi_{c0,1,2}$ in the NRQCD factorization framework. Three distinct decay mechanisms, i.e., the…

High Energy Physics - Phenomenology · Physics 2013-05-15 Jia Xu , Hai-Rong Dong , Feng Feng , Ying-Jia Gao , Yu Jia

In this paper, we study double charmonia production in Upsilon peaks, especially, a S-wave charmonium $\eta_c$ and a P-wave charmonium $h_c(^1P_1)$, or a S-wave charmonium $J/\psi$ and the $X(3940)$ and $X(4160)$ within the nonrelativistic…

High Energy Physics - Phenomenology · Physics 2015-10-21 Ruilin Zhu

The branching ratio and direct $CP$ asymmetry of the ${\Upsilon}(1S)$ ${\to}$ $B_{c}D_{s}$ weak decay are estimated with the perturbative QCD approach. It is found that (1) The direct $CP$-violating asymmetry is close to zero. (2) the…

High Energy Physics - Phenomenology · Physics 2017-03-02 Junfeng Sun , Yueling Yang , Qingxia Li , Haiyan Li , Na Wang , Qin Chang , Jinshu Huang

We study the doubly charmed baryonic B decays $B\to \Xi_{c} \Lambda_{c}$ and $B\to \Lambda^{+}_{c} \Lambda^{-}_{c} K$, recently observed by BELLE. We find that the unexpected large branching ratios (BRs) could be ascribed to the final state…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chuan-Hung Chen

Using data collected in the region of the Upsilon(4S) resonance with the CLEO II detector operating at the Cornell Electron Storage Ring CESR, we present the first observation of B mesons decaying into the charmed strange baryons Xi_c0 and…

High Energy Physics - Experiment · Physics 2010-04-08 CLEO Collaboration , B. Barish et al

The doubly heavy baryon $\Xi_{QQ^{\prime}}$ ($Q^{(\prime)}$ = $b$ or $c$) is different from the ordinary baryons. The production of the doubly heavy baryon can provide valuable insight on how the colored $(QQ^{\prime})$-diquark can be…

High Energy Physics - Phenomenology · Physics 2013-03-26 Jun Jiang , Xing-Gang Wu , Shao-Ming Wang , Jia-Wei Zhang , Zhen-Yun Fang

In this paper, we carry out a detailed study of doubly-charmed baryon production in $Z$ boson decay, on the basis of the nonrelativistic QCD factorization. With the inclusion of the di-quark states $(cc)[^3S_1]_{\bar{\textbf{3}}}$ and…

High Energy Physics - Phenomenology · Physics 2022-06-15 Xuan Luo , Ying-Zhao Jiang , Gui-Yuan Zhang , Zhan Sun

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

There are two apparent puzzles connected with the two-body and three-body doubly charmed baryonic B decays. First, earlier calculations based on QCD sum rules or the diquark model predict $Br(\bar B^0\to\Xi_c^+\bar\Lambda_c^-)\approx…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hai-Yang Cheng , Chun-Khiang Chua , Shang-Yuu Tsai

We present the first evidence for the production of Upsilon(1D) states in the four-photon cascade, Upsilon(3S)-->gamma chib(2P), chib(2P)-->gamma Upsilon(1D), Upsilon(1D)-->gamma chib(1P), chib(1P)-->gamma Upsilon(1S), followed by the…

High Energy Physics - Experiment · Physics 2010-04-08 G. Bonvicini , CLEO Collaboration

We extend the analysis of weak decays of heavy hadrons to the case of doubly charmed baryons, \Xi_{cc}^{++}, \Xi_{cc}^{+} and \Omega_{cc}^{+}. Doubly charmed baryons are modeled as a heavy-light system containing a heavy cc-diquark and a…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Guberina , B. Melic , H. Stefancic

We report the first observation of the radiative decay of the $\Upsilon(1S)$ into a charmonium state. The statistical significance of the observed signal of $\Upsilon(1S) \to \gamma \chi_{c1}$ is 6.3 standard deviations including…

High Energy Physics - Experiment · Physics 2020-04-01 P. Katrenko , I. Adachi , H. Aihara , S. Al Said , D. M. Asner , T. Aushev , I. Badhrees , S. Bahinipati , P. Behera , C. Beleno , J. Bennett , V. Bhardwaj , B. Bhuyan , J. Biswal , A. Bobrov , G. Bonvicini , M. Bracko , M. Campajola , L. Cao , D. Cervenkov , 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 , F. Di Capua , S. Di Carlo , Z. Dolezal , T. V. Dong , S. Eidelman , D. Epifanov , J. E. Fast , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Garmash , A. Giri , P. Goldenzweig , B. Golob , O. Grzymkowska , O. Hartbrich , K. Hayasaka , H. Hayashii , W. -S. Hou , T. Iijima , K. Inami , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , H. B. Jeon , S. Jia , Y. Jin , D. Joffe , K. K. Joo , G. Karyan , H. Kichimi , D. Y. Kim , K. T. Kim , S. H. Kim , K. Kinoshita , P. Kodys , S. Korpar , R. Kroeger , T. Kuhr , I. S. Lee , S. C. Lee , P. Lewis , Y. B. Li , L. Li Gioi , J. Libby , K. Lieret , C. MacQueen , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , K. Miyabayashi , H. Miyata , R. Mizuk , G. B. Mohanty , T. J. Moon , T. Mori , R. Mussa , E. Nakano , T. Nakano , M. Nakao , M. Nayak , N. K. Nisar , S. Nishida , K. Nishimura , H. Ono , Y. Onuki , P. Oskin , P. Pakhlov , G. Pakhlova , T. Pang , S. Pardi , C. W. Park , H. Park , S. -H. Park , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , V. Popov , E. Prencipe , M. T. Prim , M. Ritter , A. Rostomyan , N. Rout , G. Russo , D. Sahoo , Y. Sakai , S. Sandilya , T. Sanuki , V. Savinov , O. Schneider , G. Schnell , J. Schueler , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , C. P. Shen , J. -G. Shiu , E. Solovieva , M. Staric , Z. S. Stottler , T. Sumiyoshi , W. Sutcliffe , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , K. Trabelsi , M. Uchida , S. Uehara , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Usov , R. Van Tonder , G. Varner , A. Vossen , B. Wang , C. H. Wang , M. -Z. Wang , P. Wang , X. L. Wang , E. Won , S. B. Yang , H. Ye , J. Yelton , J. H. Yin , C. Z. Yuan , Y. Yusa , Z. P. Zhang , V. Zhilich , V. Zhukova

The calculation of the partial width of the rare t-quark decay into Upsilon-meson, W-boson and b-quark (t -> \Upsilon W b) is presented. The branching ratio equals Br(t -> Upsilon W b) = 1.3 * 10^{-5} that make possible searches for this…

High Energy Physics - Phenomenology · Physics 2021-10-06 Sergei Slabospitskii

We estimate the branching ratio for the inclusive decays $\Xi_{bbq} \rightarrow {\bar B}_c^{(*)}+X_{c,s,q}$ to be approximately 1%. Our estimate is performed using non-relativistic potential quark model methods that are appropriate if the…

High Energy Physics - Phenomenology · Physics 2019-04-17 Alexander K. Ridgway , Mark B. Wise