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Related papers: \Upsilon(1s)-->\gamma(\eta',\eta) decays

200 papers

The ${\Upsilon}(1S)$ ${\to}$ $B_{c}D_{s}^{\ast}$ weak decay is studied with the perturbative QCD approach firstly. It is found that (1) main contributions to branching ratio come from the longitudinal and parallel helicity amplitudes, (2)…

High Energy Physics - Phenomenology · Physics 2016-04-26 Junfeng Sun , Yueling Yang , Qingxia Li , Gongru Lu , Jinshu Huang , Qin Chang

We present the complete next-to-next-to-next-to-leading order short-distance and bound-state QCD correction to the leptonic decay rate Gamma(Upsilon(1S)->l+l-) of the lowest-lying spin-1 bottomonium state. The perturbative QCD prediction is…

High Energy Physics - Phenomenology · Physics 2014-04-24 Martin Beneke , Yuichiro Kiyo , Peter Marquard , Alexander Penin , Jan Piclum , Dirk Seidel , Matthias Steinhauser

The Light-front quark model (LFQM) has been applied to calculate the transition matrix elements of heavy hadron decays. However, it is noted that using the traditional wave functions of the LFQM given in literature, the theoretically…

High Energy Physics - Phenomenology · Physics 2010-08-24 Hong-Wei Ke , Xue-Qian Li , Zheng-Tao Wei , Xiang Liu

We present a limit on the branching fraction for the decay $B^0 \to \gamma \gamma$ using data collected at the $\Upsilon(4S)$ resonance with the BABAR detector at the PEP-II asymmetric--energy $e^+e^-$ collider. Based on the observation of…

High Energy Physics - Experiment · Physics 2010-05-28 the BABAR Collaboration , B. Aubert

We present a detailed analysis of the Higgs boson decays $h\rightarrow Z \gamma$ and $h\rightarrow m_V Z$ in the $U(1)_X$SSM, with $m_V$ denoting the meson ($\omega,\rho,\phi,J/{\psi},\Upsilon$). Using the effective Lagrangian method, we…

High Energy Physics - Phenomenology · Physics 2022-10-18 Xi Wang , Shu-Min Zhao , Tong-Tong Wang , Lu-Hao Su , Wei Li , Ze-Ning Zhang , Zhong-Jun Yang , Tai-Fu Feng

Based on previous studies that support the important role of the $f_2(1270)$, $f'_2(1525)$, and $\bar{K}^{*}_{2}(1430)$ resonances in the $J/\psi [\psi(2S)] \to \phi (\omega) VV$ decays, we make an analysis of the analogous decays of…

High Energy Physics - Phenomenology · Physics 2015-11-30 Lian-Rong Dai , Ju-Jun Xie , E. Oset

Using substantially larger data samples collected by the CLEO III detector, we report on new measurements of the decays of Upsilon(1S) to charmonium final states, including J/Psi, psi(2S), and chi_cJ. The latter two are first observations…

High Energy Physics - Experiment · Physics 2010-04-08 R. A Briere , CLEO Collaboration

We calculate the rate for $\Upsilon$ decay into a pair of bottom squarks as a function of the masses of the bottom squark and the gluino. Data from decays of the $\Upsilon$ states could provide significant new bounds on the existence and…

High Energy Physics - Phenomenology · Physics 2011-01-27 Edmond L. Berger , L. Clavelli

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

The radiative decays $\eta'(\eta)\rta\gamma\gamma$ are discussed. The modifications of the conventional PCAC formulae due to the gluonic contribution to the flavour singlet axial anomaly are given. The decay constants satisfy a modified…

High Energy Physics - Phenomenology · Physics 2009-10-31 G. M. Shore

The recently observed by CLEO cascade decays Upsilon(3S) -> gamma chi_{bJ}^\prime -> gamma omega Upsilon are discussed. It is shown that within the nonrelativistic description of bottomonium in the heavy b quark limit, the ratio of the…

High Energy Physics - Phenomenology · Physics 2011-01-27 M. B. Voloshin

We report the first observation of $B^0 \to J/\psi \eta$ decay. These results are obtained from a data sample that contains 449 million $B\bar{B}$ pairs accumulated at the $\Upsilon(4S)$ resonance with the Belle detector at the KEKB…

High Energy Physics - Experiment · Physics 2019-08-14 M. -C. Chang

The recent measurements by CLEO Collaboration for the inclusive J/Psi and Psi(2S) production in Upsilon(1S) decay and our previous calculation are analyzed. The J/Psi momentum spectrum and the production ratio of Psi(2S) versus J/Psi favour…

High Energy Physics - Phenomenology · Physics 2011-03-23 Wei Han , Shi-Yuan Li

It is shown that the rates of the decays Upsilon(1^3D_1) -> eta Upsilon(1S) and Upsilon(1^3D_2) -> eta Upsilon(1S) should be comparable to and likely exceed that of the recently discussed in the literature two-pion transition Upsilon(1D) ->…

High Energy Physics - Phenomenology · Physics 2009-11-10 M. B. Voloshin

We have reconstructed the radiative decays $\chi_{b}(1P) \to \Upsilon(1S) \gamma $ and $\chi_{b}(2P) \to \Upsilon(1S) \gamma $ in $p \bar{p}$ collisions at $\sqrt{s} = 1.8$ TeV, and measured the fraction of $\Upsilon(1S)$ mesons that…

High Energy Physics - Experiment · Physics 2010-05-12 CDF Collaboration , T. Affolder

The ratio $R_{\tau\mu}(\Upsilon(1S)) = \Gamma_{\Upsilon(1S)\to\tau^+\tau^-}/\Gamma_{\Upsilon(1S)\to\mu^+\mu^-}$ is measured using a sample of $(121.8\pm1.2)\times10^6$ $\Upsilon(3S)$ events recorded by the BABAR detector. This measurement…

High Energy Physics - Experiment · Physics 2010-05-25 The BABAR Collaboration , P. del Amo Sanchez

We study the electromagnetic Dalitz (EM) decays, $\psi \to \eta_{c} l^{+} l^{-}$ and $\Upsilon \to \eta_{b} l^{+} l^{-}$ ($l = e$ or $\mu$), in which the lepton pair comes from the virtual photon emitted by the M1 transition from $c\bar{c}$…

High Energy Physics - Phenomenology · Physics 2019-08-09 Li-Min Gu , Hai-Bo Li , Xin-Xin Ma , Mao-Zhi Yang

Using $\gamma \gamma J/\psi, J/\psi \ra e^+ e^-$ and $\mu^+ \mu^-$ events from a sample of $14.0\times 10^6$ $\psip$ decays collected with the BESII detector, the branching fractions for $\psip\ra \pi^0\J$, $\eta\J$, and…

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

In the paper, we study the $\Upsilon(1S)$ leptonic decay width $\Gamma(\Upsilon(1S)\to \ell^+\ell^-)$ by using the principle of maximum conformality (PMC) scale-setting approach. The PMC adopts the renormalization group equation to set the…

High Energy Physics - Phenomenology · Physics 2019-08-13 Xu-Dong Huang , Xing-Gang Wu , Jun Zeng , Qing Yu , Jian-Ming Shen

We report the first evidence for the $h_{b}(\text{2P}) \to \Upsilon(\text{1S})\eta$ transition with a significance of $3.5$ standard deviations. The decay branching fraction is measured to be $\mathcal{B}[h_{b}(\text{2P}) \to…

High Energy Physics - Experiment · Physics 2024-07-08 Belle Collaboration , E. Kovalenko , I. Adachi , H. Aihara , D. M. Asner , T. Aushev , R. Ayad , V. Babu , Sw. Banerjee , K. Belous , J. Bennett , M. Bessner , T. Bilka , D. Biswas , A. Bobrov , D. Bodrov , A. Bondar , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , M. -C. Chang , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , Y. Choi , S. Choudhury , N. Dash , G. De Nardo , G. De Pietro , R. Dhamija , F. Di Capua , Z. Doležal , T. V. Dong , S. Dubey , P. Ecker , D. Epifanov , D. Ferlewicz , B. G. Fulsom , R. Garg , V. Gaur , A. Garmash , A. Giri , P. Goldenzweig , E. Graziani , T. Gu , Y. Guan , K. Gudkova , C. Hadjivasiliou , T. Hara , K. Hayasaka , S. Hazra , W. -S. Hou , C. -L. Hsu , K. Inami , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , Y. Jin , T. Kawasaki , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , A. Korobov , S. Korpar , P. Križan , P. Krokovny , T. Kuhr , R. Kumar , K. Kumara , A. Kuzmin , Y. -J. Kwon , Y. -T. Lai , T. Lam , D. Levit , L. K. Li , L. Li Gioi , J. Libby , D. Liventsev , Y. Ma , A. Martini , M. Masuda , T. Matsuda , D. Matvienko , F. Meier , M. Merola , K. Miyabayashi , R. Mizuk , G. B. Mohanty , R. Mussa , I. Nakamura , M. Nakao , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , M. Niiyama , S. Nishida , S. Ogawa , H. Ono , G. Pakhlova , S. Pardi , J. Park , S. -H. Park , A. Passeri , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , E. Prencipe , M. T. Prim , M. V. Purohit , N. Rout , G. Russo , S. Sandilya , L. Santelj , V. Savinov , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , W. Shan , C. Sharma , J. -G. Shiu , B. Shwartz , A. Sokolov , E. Solovieva , M. Starič , M. Sumihama , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , R. Tiwary , M. Uchida , Y. Unno , S. Uno , Y. Usov , A. Vinokurova , D. Wang , E. Wang , M. -Z. Wang , X. L. Wang , E. Won , B. D. Yabsley , W. Yan , S. B. Yang , J. Yelton , J. H. Yin , Y. Yook , C. Z. Yuan , Z. P. Zhang , V. Zhilich