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Related papers: The $\eta_c(3654)$ and hyperfine splitting in char…

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The h_c(1P1) state of charmonium has been observed in the reaction \psi(2S) -> \pi0 h_c -> (\gamma\gamma)(\gamma\eta_c) using 3.08 million \psi(2S) decays recorded in the CLEO detector. Data have been analyzed both for the inclusive…

High Energy Physics - Experiment · Physics 2010-04-08 J. L. Rosner , CLEO Collaboration

Corrections of orders alpha^5, alpha^6 are calculated in the hyperfine splitting of the 2S state in the muonic hydrogen. The nuclear structure effects are taken into account in the one- and two-loop Feynman amplitudes by means of the proton…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. P. Martynenko

The hyperfine splittings in heavy quarkonia are studied using new experimental data on the di-electron widths. The smearing of the spin-spin interaction is taken into account, while the radius of smearing is fixed by the known…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. M. Badalian , B. L. G. Bakker

We report on the observation of the eta_{c}^{prime}(2^{1}S_{0}), the radial excitation of eta_{c}(1^{1}S_{0}) ground state of charmonium, in the two-photon fusion reaction gamma gamma rightarrow eta_{c}^{prime} rightarrow…

High Energy Physics - Experiment · Physics 2010-04-08 D. M. Asner , CLEO Collaboration

Corrections of orders alpha^5 and alpha^6 are calculated in the hyperfine splittings of 1S and 2S - energy levels in the ion of muonic helium. The electron vacuum polarization effects, the nuclear structure corrections and recoil…

High Energy Physics - Phenomenology · Physics 2014-11-18 A. P. Martynenko

The hyperfine splittings in heavy quarkonia are studied in a model-independent way using the experimental data on di-electron widths. Relativistic correlations are taken into account together with the smearing of the spin-spin interaction.…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. M. Badalian , B. L. G. Bakker

By analyzing existing data on pseudoscalar charmonium decays, we obtain the ratio of the branching fractions of $\eta_c(2S)$ and $\eta_c$ decays into ten different final states with light hadrons. For the first time, we test the two…

High Energy Physics - Phenomenology · Physics 2022-05-17 Hongpeng Wang , Chang-Zheng Yuan

Predictions for the hyperfine splitting of 2S bottomonia are compared with the two recent experimental candidates for the \eta_b(2S). The smaller splitting of the Belle state is consistent with unquenched lattice QCD computations, many…

High Energy Physics - Phenomenology · Physics 2013-05-30 T. J. Burns

The suitability of using non-relativistic quantum mechanics to investigate heavy quark mesons is illustrated through a study of the charmonium meson. We consider a limiting form of the QCD potential which is a simple combination of the…

High Energy Physics - Phenomenology · Physics 2021-03-05 Chandrashekar Radhakrishnan

The measurement of the eta_b mass, together with a QCD result for the hyperfine splitting E_{HFS}=M_{Upsilon(1S)}-M_{eta_b}, allows us to determine the strong coupling constant alpha_s at a low energy scale. The result…

High Energy Physics - Phenomenology · Physics 2011-02-25 Pietro Colangelo , Pietro Santorelli , Egidio Scrimieri

The spin-singlet P-wave state of charmonium, hc(1P1), has been observed in the decay psi(2S) -> pi0 hc followed by hc -> gamma etac. Inclusive and exclusive analyses of the M(hc) spectrum have been performed. Two complementary inclusive…

High Energy Physics - Experiment · Physics 2010-04-08 P. Rubin , CLEO Collaboration

In this talk, I review the recent experimental results on charmonium spectroscopy from BESIII, Belle, BaBar and CLEOc. Below the open-charm threshold, the masses and widths of spin-singlet states eta_c, eta_c(2S), h_c are measured with high…

High Energy Physics - Experiment · Physics 2013-11-15 Jingzhi Zhang

Recent measurements of the $\eta_b(1S)$, the ground state of the $b\bar{b}$ system, show the splitting between it and the $\Up(1S)$ to be 69.5$\pm$3.2 MeV, considerably larger than lattice QCD and potential model predictions, including…

High Energy Physics - Phenomenology · Physics 2011-08-09 Stanley F. Radford , Wayne W. Repko

We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting using the nonrelativistic renormalization group. On the basis of this result, we predict the mass of the $\eta_b$ meson to be $M(\eta_b)=9419…

High Energy Physics - Phenomenology · Physics 2010-05-25 B. A. Kniehl , A. A. Penin , A. Pineda , V. A. Smirnov , M. Steinhauser

Experimentally the charmonium hyperfine splitting is $M_{J/\psi}-M_{\eta_c}=117$ MeV and current lattice results are generally below this value. The difference could be due to the effects of the disconnected flavor singlet diagrams which…

High Energy Physics - Lattice · Physics 2010-11-15 C. DeTar , L. Levkova

The recent results on charmonium and charmoniumlike states from Belle experiment are reviewed. We summarise searches in $B$ decays for possible $X$-like states in final states containing $\eta_c$. The new measurement of…

High Energy Physics - Experiment · Physics 2015-09-15 Xiaolong Wang

We study relativistic charmonium on very fine quenched lattices (beta=6.4 and 6.6). We concentrate on the calculation of the hyperfine splitting between eta_c and J/psi, aiming for a controlled continuum extrapolation of this quantity.…

We measure the cross section of $e^+e^-\rightarrow\eta_c J/\psi$ at the $\Upsilon(nS) (n=1$ -- $5)$ on-resonance and 10.52 GeV off-resonance energy points using the full data sample collected by the Belle detector with an integrated…

High Energy Physics - Experiment · Physics 2023-08-08 Belle Collaboration , J. H. Yin , Y. B. Li , E. Won , I. Adachi , H. Aihara , S. Al Said , D. M. Asner , T. Aushev , R. Ayad , V. Babu , Sw. Banerjee , P. Behera , K. Belous , J. Bennett , M. Bessner , T. Bilka , D. Biswas , D. Bodrov , G. Bonvicini , J. Borah , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , D. Červenkov , M. -C. Chang , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , J. Cochran , S. Das , 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. Giri , P. Goldenzweig , E. Graziani , T. Gu , Y. Guan , K. Gudkova , C. Hadjivasiliou , S. Halder , T. Hara , K. Hayasaka , H. Hayashii , D. Herrmann , W. -S. Hou , C. -L. Hsu , T. Iijima , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , Q. P. Ji , S. Jia , Y. Jin , K. K. Joo , J. Kahn , A. B. Kaliyar , T. Kawasaki , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , H. Kindo , K. Kinoshita , P. Kodyš , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , P. Krokovny , T. Kuhr , M. Kumar , R. Kumar , K. Kumara , T. Lam , J. S. Lange , S. C. Lee , L. K. Li , Y. Li , J. Libby , K. Lieret , Y. -R. Lin , D. Liventsev , M. Masuda , T. Matsuda , D. Matvienko , S. K. Maurya , F. Meier , M. Merola , F. Metzner , R. Mizuk , G. B. Mohanty , R. Mussa , I. Nakamura , D. Narwal , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , N. K. Nisar , S. Nishida , S. Ogawa , H. Ono , P. Oskin , G. Pakhlova , S. Pardi , H. Park , J. Park , S. -H. Park , A. Passeri , S. Patra , S. Paul , 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 , Y. Seino , K. Senyo , W. Shan , M. Shapkin , C. Sharma , J. -G. Shiu , E. Solovieva , M. Starič , Z. S. Stottler , M. Sumihama , M. Takizawa , K. Tanida , F. Tenchini , R. Tiwary , M. Uchida , T. Uglov , Y. Unno , S. Uno , Y. Usov , S. E. Vahsen , G. Varner , A. Vinokurova , D. Wang , E. Wang , M. -Z. Wang , X. L. Wang , S. Watanuki , O. Werbycka , X. Xu , B. D. Yabsley , W. Yan , S. B. Yang , J. Yelton , Y. Yook , C. Z. Yuan , Z. P. Zhang , V. Zhilich , V. Zhukova

In this talk, we will present the results on the charmonium spin singlet states below the open charm threshold, including h_c, \eta_c, and \eta_c(2S). The masses, widthes, and production rates of these states will be reported. The results…

High Energy Physics - Experiment · Physics 2019-08-13 Liangliang Wang

The hyperfine splitting in heavy quarkonia is considered in its relation to the leptonic decay rates with the account of relativistic and radiative corrections. The calculated decay rates agree well with the available experimental data,…

High Energy Physics - Phenomenology · Physics 2009-11-10 D. Ebert , R. N. Faustov , V. O. Galkin
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