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相关论文: (Vector) Glueballs and Charmonium Decay Revisited

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We compare the matrix model and integrable system approaches to calculating the exact vacuum structure of general N=1 deformations of either the basic N=2 theory or its generalization with a massive adjoint hypermultiplet, the N=2* theory.…

高能物理 - 理论 · 物理学 2010-02-03 Timothy J. Hollowood

The mass of the lowest scalar glueball is discussed by using QCD sum rules. We find that the glueball mass is sensitive to the choice of moments and slightly depends on the radiative corrections. With the help of suitable moments and…

高能物理 - 唯象学 · 物理学 2007-05-23 Tao Huang , Ai-lin Zhang

In pure-glue QCD, gluon-gluon scattering in the $J^{PC}=0^{-+}$ channel is described by a very simple equation, especially if one considers just the leading contribution to the scattering kernel. Of all components in this kernel, only the…

核理论 · 物理学 2020-02-19 E. V. Souza , M. N. Ferreira , A. C. Aguilar , J. Papavassiliou , C. D. Roberts , S. -S. Xu

We provide the first explanation of the counter-intuitive scalar glueball couplings to pseudoscalar mesons found in lattice QCD and predict hitherto uncalculated decay modes. Significant a_1 pi and (pi pi)_S (pi pi)_S couplings are found.…

高能物理 - 唯象学 · 物理学 2014-11-17 Leonid Burakovsky , Philip R. Page

The SU(2) gluonic correlation functions, glueball effective masses in the $J^{P}=0^{+}$, $2^{+}$ and $0^{-}$ channels were calculated from the lattice classical gauge configurations which were obtained by smoothing the thermal gauge…

高能物理 - 格点 · 物理学 2017-08-23 Ying Chen , Ji-Min Wu , Bing He

Pure gauge glueballs at finite temperature are investigated in a large temperature range from $0.3T_c$ to $1.9T_c$ on anisotropic lattices. Optimized glueball operators are used to obtain better signals. It is found in all 20 symmetry…

高能物理 - 格点 · 物理学 2010-11-05 The CLQCD Collaboration , X. -F. Meng , G. Li , Y. Chen , C. Liu , Y. -B. Liu , J. -P. Ma , J. -B. Zhang

According to the QCD expectations the lightest glueball should be a scalar particle (J^{PC}=0^{++}). Different scenarios have been considered for a classification of these states but -- despite considerable progress in recent years -- the…

高能物理 - 唯象学 · 物理学 2008-11-26 Wolfgang Ochs

We discuss a notion of gluon-glueball duality analogous to quark-hadron duality. We apply this idea to the radiative decay of heavy orthoquarkonium, $Q\bar Q \to \gamma g g$, which has been used to search for glueballs. The duality is first…

高能物理 - 唯象学 · 物理学 2009-09-24 Shmuel Nussinov , Robert Shrock

We present a two-flavour linear sigma model with global chiral symmetry and (axial-)vector mesons as well as an additional glueball degree of freedom. We study the structure of the well-established scalar resonances f0(1370) and f0(1500):…

高能物理 - 唯象学 · 物理学 2012-06-14 Stanislaus Janowski , Denis Parganlija , Francesco Giacosa , Dirk H. Rischke

We suggest a procedure of the lightest glueball detection in a head-on collision of photons whose center-of-mass energy is in the range $1.3-2$ GeV. Recent evidence for the scattering of light by light in experiments at the Large Hadron…

高能物理 - 唯象学 · 物理学 2021-08-31 B. P. Kosyakov , E. Yu. Popov , M. A. Vronsky

A 2.25$\times10^8$ $\jpsi$ event sample accumulated with the BESIII detector is used to study the doubly OZI suppressed decay modes $\jpsi\to\gamma\of$, $\omega\to\ppp$, $\phi\to\kk$. A strong deviation ($>$ 30$\sigma$) from three-body…

高能物理 - 实验 · 物理学 2014-10-01 M. Ablikim , M. N. Achasov , O. Albayrak , D. J. Ambrose , F. F. An , Q. An , J. Z. Bai , Y. Ban , J. Becker , J. V. Bennett , M. Bertani , J. M. Bian , E. Boger , O. Bondarenko , I. Boyko , R. A. Briere , V. Bytev , X. Cai , O. Cakir , A. Calcaterra , G. F. Cao , S. A. Cetin , J. F. Chang , G. Chelkov , G. Chen , H. S. Chen , J. C. Chen , M. L. Chen , S. J. Chen , X. Chen , Y. B. Chen , H. P. Cheng , Y. P. Chu , D. Cronin-Hennessy , H. L. Dai , J. P. Dai , D. Dedovich , Z. Y. Deng , A. Denig , I. Denysenko , M. Destefanis , W. M. Ding , Y. Ding , L. Y. Dong , M. Y. Dong , S. X. Du , J. Fang , S. S. Fang , L. Fava , C. Q. Feng , R. B. Ferroli , P. Friedel , C. D. Fu , Y. Gao , C. Geng , K. Goetzen , W. X. Gong , W. Gradl , M. Greco , M. H. Gu , Y. T. Gu , Y. H. Guan , A. Q. Guo , L. B. Guo , T. Guo , Y. P. Guo , Y. L. Han , F. A. Harris , K. L. He , M. He , Z. Y. He , T. Held , Y. K. Heng , Z. L. Hou , C. Hu , H. M. Hu , J. F. Hu , T. Hu , G. M. Huang , G. S. Huang , J. S. Huang , L. Huang , X. T. Huang , Y. Huang , Y. P. Huang , T. Hussain , C. S. Ji , Q. Ji , Q. P. Ji , X. B. Ji , X. L. Ji , L. L. Jiang , X. S. Jiang , J. B. Jiao , Z. Jiao , D. P. Jin , S. Jin , F. F. Jing , N. Kalantar-Nayestanaki , M. Kavatsyuk , B. Kopf , M. Kornicer , W. Kuehn , W. Lai , J. S. Lange , M. Leyhe , C. H. Li , Cheng Li , Cui Li , D. M. Li , F. Li , G. Li , H. B. Li , J. C. Li , K. Li , Lei Li , Q. J. Li , S. L. Li , W. D. Li , W. G. Li , X. L. Li , X. N. Li , X. Q. Li , X. R. Li , Z. B. Li , H. Liang , Y. F. Liang , Y. T. Liang , G. R. Liao , X. T. Liao , D. Lin , B. J. Liu , C. L. Liu , C. X. Liu , F. H. Liu , Fang Liu , Feng Liu , H. Liu , H. B. Liu , H. H. Liu , H. M. Liu , H. W. Liu , J. P. Liu , K. Liu , K. Y. Liu , Kai Liu , P. L. Liu , Q. Liu , S. B. Liu , X. Liu , Y. B. Liu , Z. A. Liu , Zhiqiang Liu , Zhiqing Liu , H. Loehner , G. R. Lu , H. J. Lu , J. G. Lu , Q. W. Lu , X. R. Lu , Y. P. Lu , C. L. Luo , M. X. Luo , T. Luo , X. L. Luo , M. Lv , C. L. Ma , F. C. Ma , H. L. Ma , Q. M. Ma , S. Ma , T. Ma , X. Y. Ma , F. E. Maas , M. Maggiora , Q. A. Malik , Y. J. Mao , Z. P. Mao , J. G. Messchendorp , J. Min , T. J. Min , R. E. Mitchell , X. H. Mo , C. Morales Morales , N. Yu. Muchnoi , H. Muramatsu , Y. Nefedov , C. Nicholson , I. B. Nikolaev , Z. Ning , S. L. Olsen , Q. Ouyang , S. PacettiB , J. W. Park , M. Pelizaeus , H. P. Peng , K. Peters , J. L. Ping , R. G. Ping , R. Poling , E. Prencipe , M. Qi , S. Qian , C. F. Qiao , L. Q. Qin , X. S. Qin , Y. Qin , Z. H. Qin , J. F. Qiu , K. H. Rashid , G. Rong , X. D. Ruan , A. Sarantsev , B. D. Schaefer , M. Shao , C. P. Shen , X. Y. Shen , H. Y. Sheng , M. R. Shepherd , X. Y. Song , S. Spataro , B. Spruck , D. H. Sun , G. X. Sun , J. F. Sun , S. S. Sun , Y. J. Sun , Y. Z. Sun , Z. J. Sun , Z. T. Sun , C. J. Tang , X. Tang , I. Tapan , E. H. Thorndike , D. Toth , M. Ullrich , G. S. Varner , B. Q. Wang , D. Wang , D. Y. Wang , K. Wang , L. L. Wang , L. S. Wang , M. Wang , P. Wang , P. L. Wang , Q. J. Wang , S. G. Wang , X. F. Wang , X. L. Wang , Y. F. Wang , Z. Wang , Z. G. Wang , Z. Y. Wang , D. H. Wei , J. B. Wei , P. Weidenkaff , Q. G. Wen , S. P. Wen , M. Werner , U. Wiedner , L. H. Wu , N. Wu , S. X. Wu , W. Wu , Z. Wu , L. G. Xia , Z. J. Xiao , Y. G. Xie , Q. L. Xiu , G. F. Xu , G. M. Xu , Q. J. Xu , Q. N. Xu , X. P. Xu , Z. R. Xu , F. Xue , Z. Xue , L. Yan , W. B. Yan , Y. H. Yan , H. X. Yang , Y. Yang , Y. X. Yang , H. Ye , M. Ye , M. H. Ye , B. X. Yu , C. X. Yu , H. W. Yu , J. S. Yu , S. P. Yu , C. Z. Yuan , Y. Yuan , A. A. Zafar , A. Zallo , Y. Zeng , B. X. Zhang , B. Y. Zhang , C. Zhang , C. C. Zhang , D. H. Zhang , H. H. Zhang , H. Y. Zhang , J. Q. Zhang , J. W. Zhang , J. Y. Zhang , J. Z. Zhang , R. Zhang , S. H. Zhang , X. J. Zhang , X. Y. Zhang , Y. Zhang , Y. H. Zhang , Z. P. Zhang , Z. Y. Zhang , Zhenghao Zhang , G. Zhao , H. S. Zhao , J. W. Zhao , K. X. Zhao , Lei Zhao , Ling Zhao , M. G. Zhao , Q. Zhao , Q. Z. Zhao , S. J. Zhao , T. C. Zhao , Y. B. Zhao , Z. G. Zhao , A. Zhemchugov , B. Zheng , J. P. Zheng , Y. H. Zheng , B. Zhong , Z. Zhong , L. Zhou , X. K. Zhou , X. R. Zhou , C. Zhu , K. Zhu , K. J. Zhu , S. H. Zhu , X. L. Zhu , Y. C. Zhu , Y. M. Zhu , Y. S. Zhu , Z. A. Zhu , J. Zhuang , B. S. Zou , J. H. Zou

We study the pseudoscalar glueball candidates in a chiral effective Lagrangian model proposed by 't hooft, motived by taking into account the instanton effects, which can describe not only the chiral symmetry breaking, but also the solution…

高能物理 - 唯象学 · 物理学 2010-01-27 Song He , Mei Huang , Qi-Shu Yan

Belle data on gamma-gamma -> eta'-pi-pi are refitted using a broad J^{PC}=0^(-+) signal peaking in the mass range 2250-2300 MeV, but without \eta (1760). There is the possibility that this broad 0^(-+) signal may be identified with the…

高能物理 - 实验 · 物理学 2015-06-11 D. V. Bugg

In the present work a consistent kinematic-based framework for glueball states is proposed. It relates the glueball, the Pomeron, QCD lattice calculations, the $0^{++}$ scalar states $f_0(1710)$ and $\chi_{c0}(1P)$, the $2^{++}$ states…

高能物理 - 唯象学 · 物理学 2015-11-19 Simone Giani , Hubert Niewiadomski , Luca Trentadue

The mixing angles between scalar isoscalar resonances and a scalar glueball are determined from their decays into two pseudoscalar mesons. For $f_0(1370)$ and $f_0(1500)$, at most a small glueball component is admitted by the data. The…

高能物理 - 唯象学 · 物理学 2022-03-14 Eberhard Klempt , Andrey V. Sarantsev

We continue the study of flavor aspects of strong interaction. The answer to the question of glueball existence is probably a necessary step in this investigation. The existence of the glueball implies the existence of the decuplet. The…

高能物理 - 唯象学 · 物理学 2015-10-20 Michal Majewski

We address the nature of the $X(2370)$ resonance observed in the $J/\psi$ radiative decays, $J/\psi\rightarrow\gamma K^{+} K^{-}\eta'$, $J/\psi\rightarrow\gamma K_S K_S\eta'$ and $J/\psi\rightarrow\gamma \pi^{+}\pi^{-}\eta'$. By studying…

高能物理 - 唯象学 · 物理学 2022-02-15 Xiang Sun , Ling-Yun Dai , Shi-Qing Kuang , Wen Qin , A. P. Szczepaniak

We show that the newly discovered scalar meson $f_0(1500)$ at LEAR has properties compatible with the lightest scalar glueball predicted by lattice QCD and incompatible with a $\qqbar$ state. We suggest that decays of glueballs are into…

高能物理 - 唯象学 · 物理学 2009-09-25 Claude Amsler , Frank Close

We study the interaction of scalar glueball with quark-antiquark and four-quark spinless meson fields within the framework of a generalized linear sigma model in which the trace anomaly of QCD is exactly realized. To determine the pure…

高能物理 - 唯象学 · 物理学 2018-07-31 Amir H. Fariborz , Renata Jora

The masses of pure gauge glueballs are calculated with the use of relativistic string Hamiltonian without fitting parameters. The string tension $\sigma_f=0.184$~GeV$^2$ in fundamental representation is fixed, using the Necco-Sommer lattice…

高能物理 - 唯象学 · 物理学 2025-09-18 A. M. Badalian , M. S. Lukashov