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Related papers: Positronium-ion decay

200 papers

In this paper, a study of two-photon and two-gluon decays in the context of p-wave heavy quarkonia is presented. Within the covariant light-front framework, the annihilation rates of scalar and tensor quarkonium states are derived. In the…

High Energy Physics - Phenomenology · Physics 2015-03-17 Chien-Wen Hwang , Rurng-Sheng Guo

In the framework of a scalar QFT, we evaluate the decay of an initial massive state into two massless particles through a triangle-shaped diagram in which virtual fields propagate. Under certain conditions, the decaying state can be seen as…

High Energy Physics - Phenomenology · Physics 2023-11-14 Milena Piotrowska , Francesco Giacosa

The BESIII experiment at the Beijing Electron Positron collider, run as a ``hyperon factory'', recently reported the first measurement of the asymmetry parameter of the $\Lambda\to n\gamma$ decay and updated its branching fraction, which…

High Energy Physics - Phenomenology · Physics 2023-04-03 Rui-Xiang Shi , Li-Sheng Geng

Despite its very short lifetime positronium provides us with a number of accurate tests of the bound state QED. In this note a brief overview of QED theory and precision experiments on the spectrum and annihilation decay of the positronium…

High Energy Physics - Phenomenology · Physics 2009-11-07 Savely G. Karshenboim

We report the first observation of the annihilation of positronium from the 2S state. Positronium (Ps) is excited with a two-photon transition from the 1S to the 2S state where its lifetime is increased by a factor of eight compared to the…

We report on the accuracy of the measurement of the two photon decay width of a Higgs boson with the mass of 120 GeV at the TESLA Photon Collider, assuming a $\gamma \gamma$ integrated luminosity of 80 fb$^{-1}$ in the hard part of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Aura Rosca , Klaus Moenig

We have completed theoretical predictions for positronium energy levels through order alpha^6 m by the calculation of the spin independent, radiative recoil correction. This contribution is significant and amounts to 10.64 MHz for the 1S…

High Energy Physics - Phenomenology · Physics 2009-10-30 Krzysztof Pachucki , Savely G. Karshenboim

Theory results on precision measurements in electron-positron annihilation at low and high energies are collected. These cover pure QCD calculations as well as mixed electroweak and QCD results, involving light and heavy quarks. The impact…

High Energy Physics - Phenomenology · Physics 2016-07-29 Konstantin Chetyrkin , Johann H. Kühn

Motivated by concerns regarding possible two-body contributions to the recently-measured inclusive Upsilon(nS)->gamma+X (n=1, 2, 3) direct photon spectra, we report on a new study of exclusive radiative decays of these narrow Upsilon(nS)…

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

A 510 day long-term measurement of a 45.3 g platinum foil acting as the sample and high voltage contact in an ultra-low-background high purity germanium detector was performed at Laboratori Nazionali del Gran Sasso (Italy). The data was…

Nuclear Experiment · Physics 2023-05-31 B. Broerman , M. Laubenstein , S. Nagorny , S. Nisi , N. Song , A. C. Vincent

We present the result for the three-loop singlet QCD corrections to the decay of a Higgs boson into two photons and improve the calculation for the non-singlet case. With the new result presented, the decay width Gamma(H -> \gamma \gamma)…

High Energy Physics - Phenomenology · Physics 2015-06-12 P. Maierhöfer , P. Marquard

The probability of W-boson decay into a lepton and a neutrino in a strong electromagnetic field is calculated. On the basis of the method for deriving exact solutions to relativistic wave equations for charged particles, an exact analytic…

High Energy Physics - Phenomenology · Physics 2009-08-20 Alexander V. Kurilin

Currently, the experimental uncertainty for the determination of the ortho-positronium (o-Ps) decay rate is at 150 ppm precision; this is two orders of magnitude lower than the theoretical one, at 1 ppm level. Here we propose a new proof of…

Atomic Physics · Physics 2022-01-26 C. Vigo , M. Raajimakers , L. Gerchow , B. Radics , A. Rubbia , P. Crivelli

We evaluate the rate of energy loss of a plasmon in a disorder-free carbon nanotube. The plasmon decays into neutral bosonic excitations of the electron liquid. The process is mediated either by phonon-assisted backscattering of a single…

Strongly Correlated Electrons · Physics 2011-09-12 Wei Chen , A. V. Andreev , E. G. Mishchenko , L. I. Glazman

We discuss the two-photon decay width of heavy hadron molecules and study the dependence on the constituent meson masses and on the binding energy. In addition finite size effects due to the extended structure of the bound state are shown…

High Energy Physics - Phenomenology · Physics 2010-10-20 Tanja Branz , Thomas Gutsche , Valery E. Lyubovitskij

Based on a data sample of 106 M $\psi^{\prime}$ events collected with the BESIII detector, the decays $\psi^{\prime}\ar\gamma\chi_{c0, 2}$,$\chi_{c0, 2}\ar\gamma\gamma$ are studied to determine the two-photon widths of the $\chi_{c0, 2}$…

High Energy Physics - Experiment · Physics 2015-06-05 BESIII Collaboration , M. Ablikim , M. N. Achasov , D. J. Ambrose , F. F. An , Q. An , Z. H. An , J. Z. Bai , R. B. Ferroli , Y. Ban , J. Becker , N. Berger , M. B. Bertani , J. M. Bian , E. Boger , O. Bondarenko , I. Boyko , R. A. Briere , V. Bytev , X. Cai , A. C. Calcaterra , G. F. Cao , J. F. Chang , G. Chelkov , G. Chen , H. S. Chen , J. C. Chen , M. L. Chen , S. J. Chen , Y. 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 , F. Feldbauer , C. Q. Feng , C. D. Fu , J. L. 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 , Y. P. Guo , Y. L. Han , X. Q. Hao , F. A. Harris , K. L. He , M. He , Z. Y. He , T. Held , Y. K. Heng , Z. L. Hou , H. M. Hu , J. F. Hu , T. Hu , B. Huang , G. M. Huang , J. S. Huang , X. T. Huang , Y. P. Huang , T. Hussain , C. S. Ji , Q. Ji , X. B. Ji , X. L. Ji , L. K. Jia , L. L. Jiang , X. S. Jiang , J. B. Jiao , Z. Jiao , D. P. Jin , S. Jin , F. F. Jing , N. Kalantar-Nayestanaki , M. Kavatsyuk , W. Kuehn , W. Lai , J. S. Lange , J. K. C. Leung , C. H. Li , Cheng Li , Cui Li , D. M. Li , F. Li , G. Li , H. B. Li , J. C. Li , K. Li , Lei Li , N. B. 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 , B. J. Liu , B. J. Liu , C. L. Liu , C. X. Liu , C. Y. 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 , Kun Liu , Kai Liu , K. Y. Liu , P. L. Liu , S. B. Liu , X. Liu , X. H. Liu , Y. B. Liu , Y. 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 , Y. Ma , F. E. Maas , M. Maggiora , Q. A. Malik , H. Mao , Y. J. Mao , Z. P. Mao , J. G. Messchendorp , J. Min , T. J. Min , R. E. Mitchell , X. H. Mo , C. Morales Morales , C. Motzko , N. Yu. Muchnoi , Y. Nefedov , C. Nicholson , I. B. Nikolaev , Z. Ning , S. L. Olsen , Q. Ouyang , S. P. Pacetti , J. W. Park , M. Pelizaeus , K. Peters , J. L. Ping , R. G. Ping , R. Poling , E. Prencipe , C. S. J. Pun , M. Qi , S. Qian , C. F. Qiao , X. S. Qin , Y. Qin , Z. H. Qin , J. F. Qiu , K. H. Rashid , G. Rong , X. D. Ruan , A. Sarantsev , J. Schulze , 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 , X. D. Sun , Y. J. Sun , Y. Z. Sun , Z. J. Sun , Z. T. Sun , C. J. Tang , X. Tang , E. H. Thorndike , H. L. Tian , D. Toth , M. U. Ulrich , G. S. Varner , B. Wang , B. Q. Wang , K. Wang , L. L. Wang , L. S. Wang , M. Wang , P. Wang , P. L. Wang , Q. Wang , Q. J. Wang , S. G. Wang , X. F. Wang , X. L. Wang , Y. D. Wang , Y. F. Wang , Y. Q. Wang , Z. Wang , Z. G. Wang , Z. Y. Wang , D. H. Wei , P. Weidenkaff , Q. G. Wen , S. P. Wen , M. W. 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 , H. Xu , Q. J. Xu , X. P. Xu , Y. Xu , Z. R. Xu , F. Xue , Z. Xue , L. Yan , W. B. Yan , Y. H. Yan , H. X. Yang , T. Yang , Y. Yang , Y. X. Yang , H. Ye , M. Ye , M. H. Ye , B. X. Yu , C. X. Yu , J. S. Yu , S. P. Yu , C. Z. Yuan , W. L. Yuan , Y. Yuan , A. A. Zafar , A. Z. Zallo , Y. Zeng , B. X. Zhang , B. Y. Zhang , C. C. Zhang , D. H. Zhang , H. H. Zhang , H. Y. Zhang , J. Zhang , J. G. Zhang , J. Q. Zhang , J. W. Zhang , J. Y. Zhang , J. Z. Zhang , L. Zhang , S. H. Zhang , T. R. Zhang , X. J. Zhang , X. Y. Zhang , Y. Zhang , Y. H. Zhang , Y. S. Zhang , Z. P. Zhang , Z. Y. Zhang , G. Zhao , H. S. Zhao , J. W. Zhao , K. X. Zhao , Lei Zhao , Ling Zhao , M. G. Zhao , Q. Zhao , S. J. Zhao , T. C. Zhao , X. H. Zhao , Y. B. Zhao , Z. G. Zhao , A. Zhemchugov , B. Zheng , J. P. Zheng , Y. H. Zheng , Z. P. Zheng , B. Zhong , J. Zhong , L. Zhou , X. K. Zhou , X. R. Zhou , C. Zhu , K. Zhu , K. J. Zhu , S. H. Zhu , X. L. Zhu , X. W. Zhu , Y. M. Zhu , Y. S. Zhu , Z. A. Zhu , J. Zhuang , B. S. Zou , J. H. Zou , J. X. Zuo

In the traditional non-relativistic bound state calculation, the two-photon decay amplitudes of the $P$-wave $\chi_{c0,2}$ and $\chi_{b0,2}$ states depend on the derivative of the wave function at the origin which can only be obtained from…

High Energy Physics - Phenomenology · Physics 2011-01-27 J. P. Lansberg , T. N. Pham

The lighter top squark in supersymmetry can live long enough to form hadronic bound states if it has no kinematically allowed two-body decays that conserve flavor. In this case, scalar stoponium may be observable through its diphoton decay…

High Energy Physics - Phenomenology · Physics 2009-09-01 Stephen P. Martin , James E. Younkin

The pi+pi- atom decays -in the ground state - predominantly into two neutral pions. We present a general expression for the corresponding decay width in the framework of QCD (including photons). It contains all terms at leading and…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. Gall , J. Gasser , V. E. Lyubovitskij , A. Rusetsky