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Related papers: Positron annihilation in the MuPs system

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The lifetimes of the B- and B0-bar mesons are measured using the partially reconstructed semileptonic decays B-bar -> D l- nu-bar X, where D is either a D0 or D*+ meson. The data were collected by the CDF detector at the Fermilab Tevatron…

High Energy Physics - Experiment · Physics 2010-05-12 F. Abe

We analyse SPI/INTEGRAL data on the 511 keV line from the Galactic Centre, accumulated over ~6 years of observations. We decompose the X-ray and soft gamma-ray emission of the central part of the Milky Way into a relatively compact "Bulge"…

High Energy Astrophysical Phenomena · Physics 2015-05-20 E. Churazov , S. Sazonov , S. Tsygankov , R. Sunyaev , D. Varshalovich

Accurate measurement of the lifetime of the neutron (which is unstable to beta decay) is important for understanding the weak nuclear force and the creation of matter during the Big Bang. Previous measurements of the neutron lifetime have…

The search for axion-like particles $X$ in muon decays is an excellent opportunity for the MEG II and Mu3e experiments to extend their horizons beyond $\mu^+ \to e^+ \gamma$ and $\mu^+ \to e^+ e^- e^+$. A suitable process for both…

High Energy Physics - Phenomenology · Physics 2024-02-01 A. Gurgone

We calculate the proton lifetime in an SO(10) supersymmetric grand unified theory [SUSY GUT] with U(2) family symmetry. This model fits the low energy data, including the recent data for neutrino oscillations. We discuss the predictions of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Radovan Dermisek

Magneto-optically trapped atoms enable the determination of lifetimes of metastable states and higher lying excited states like the $\rm{5d^{2}~^{3}F_{2}}$ state in barium. The state is efficiently populated by driving strong transitions…

Atomic Physics · Physics 2015-06-24 S. De , U. Dammalapati , L. Willmann

We measure the mean lifetime, tau=2/(Gamma_L+Gamma_H), and the width difference, DeltaGamma=Gamma_L-Gamma_H, of the light and heavy mass eigenstates of the B0s meson, B0sL and B0sH, in B0s -> J/psi phi decays using 1.7 fb^-1 of data…

High Energy Physics - Experiment · Physics 2010-05-12 CDF collaboration , T. Aaltonen

Three light sterile neutrinos (\nu_e^s, \nu_\mu^s and \nu_\tau^s) are introduced to accommodate all the available neutrino data: the atmospheric neutrino anomaly is explained by \nu_\mu-\nu_\mu^s oscillation with maximal mixing; the solar…

High Energy Physics - Phenomenology · Physics 2009-11-07 Chun Liu , Jeonghyeon Song

We study the radiative leptonic $D$ meson decays of $D^+_{(s)}\to \l^+\nu_{\l}\gamma$ ($\l=e,\mu,\tau$), $D^0\to \nu\bar{\nu}\gamma$ and $D^0\to \l^+\l^-\gamma$ ($l=e,\mu$) within the light front quark model. In the standard model, we find…

High Energy Physics - Phenomenology · Physics 2009-10-31 C. Q. Geng , C. C. Lih , Wei-Min Zhang

True muonium, the bound state of a muon and an antimuon ($\mu^+\mu^-$), has long been theoretically predicted but remains experimentally elusive. We investigate the production of true para-muonium in the radiative decay of $J/\psi$…

High Energy Physics - Phenomenology · Physics 2024-12-18 Jian-Ping Dai , Hai-Bo Li , Shuai Zhao , Zong-Ying Zheng

We calculate the corrections of orders alpha^3, alpha^4 and alpha^5 to the Lamb shift of the 1S and 2S energy levels of muonic hydrogen (mu p) and muonic deuterium (mu d). The nuclear structure effects are taken into account in terms of the…

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

To test the predictive power of ab initio nuclear structure theory, the lifetime of the second 2+ state in neutron-rich 20O, tau(2+_2 ) = 150(+80-30) fs, and an estimate for the lifetime of the second 2+ state in 16C have been obtained, for…

Models of supersymmetric grand unified theories based on SU(5)_GUT \times U(N)_H gauge group (N = 2,3) have a symmetry that guarantees light Higgs doublets and absence of dimension-five proton decay operators. We analysed the proton decay…

High Energy Physics - Phenomenology · Physics 2009-11-10 Masahiro Ibe , T. Watari

Existing limits on the non-radiative decay of one neutrino to another plus a massless particle (e.g., a singlet Majoron) are very weak. The best limits on the lifetime to mass ratio come from solar neutrino observations, and are $\tau/m…

High Energy Physics - Phenomenology · Physics 2010-04-06 John F. Beacom , Nicole F. Bell , Dan Hooper , Sandip Pakvasa , Thomas J. Weiler

The present status of theoretical and experimental investigations of the decay rate of a positronium is considered. The increasing interest to this problem has been caused by the disagreement of the calculated value of $\Gamma_3 (o-Ps)$ and…

High Energy Physics - Phenomenology · Physics 2009-10-22 Valeri V. Dvoeglazov , Rudolf N. Faustov , Yuri N. Tyukhtyaev

Metastable ${2S}$ muonic-hydrogen atoms undergo collisional ${2S}$-quenching, with rates which depend strongly on whether the $\mu p$ kinetic energy is above or below the ${2S}\to {2P}$ energy threshold. Above threshold, collisional ${2S}…

Recently a new technique for the production of muon ($\mu^+$) and muonium ($\mu^+e^-$) beams of unprecedented brightness has been proposed. As one consequence and using a highly stable Mach-Zehnder type interferometer, a measurement of the…

Atomic Physics · Physics 2007-05-23 K. Kirch

A search for proton decay into three charged leptons has been performed by using 0.37$\,$Mton$\cdot$years of data collected in Super-Kamiokande. All possible combinations of electrons, muons and their anti-particles consistent with charge…

High Energy Physics - Experiment · Physics 2020-04-01 Kamiokande Collaboration , M. Tanaka , K. Abe , C. Bronner , Y. Hayato , M. Ikeda , S. Imaizumi , H. Ito , J. Kameda , Y. Kataoka , Y. Kato , Y. Kishimoto , Ll. Marti , M. Miura , S. Moriyama , T. Mochizuki , M. Nakahata , Y. Nakajima , S. Nakayama , T. Okada , K. Okamoto , A. Orii , G. Pronost , H. Sekiya , M. Shiozawa , Y. Sonoda , A. Takeda , A. Takenaka , H. Tanaka , T. Yano , R. Akutsu , T. Kajita , K. Okumura , R. Wang , J. Xia , D. Bravo-Berguño , L. Labarga , P. Fernandez , F. d. M. Blaszczyk , E. Kearns , J. L. Raaf , J. L. Stone , L. Wan , T. Wester , J. Bian , N. J. Griskevich , W. R. Kropp , S. Locke , S. Mine , M. B. Smy , H. W. Sobel , V. Takhistov , P. Weatherly , J. Hill , J. Y. Kim , I. T. Lim , R. G. Park , B. Bodur , K. Scholberg , C. W. Walter , A. Coffani , O. Drapier , S. El Hedri , M. Gonin , Th. A. Mueller , P. Paganini , T. Ishizuka , T. Nakamura , J. S. Jang , J. G. Learned , S. Matsuno , R. P. Litchfield , A. A. Sztuc , Y. Uchida , V. Berardi , M. G. Catanesi , E. Radicioni , N. F. Calabria , G. De Rosa , G. Collazuol , F. Iacob , L. Ludovici , Y. Nishimura , S. Cao , M. Friend , T. Hasegawa , T. Ishida , T. Kobayashi , T. Nakadaira , K. Nakamura , Y. Oyama , K. Sakashita , T. Sekiguchi , T. Tsukamoto , M. Hasegawa , Y. Isobe , H. Miyabe , Y. Nakano , T. Shiozawa , T. Sugimoto , A. T. Suzuki , Y. Takeuchi , A. Ali , Y. Ashida , S. Hirota , M. Jiang , T. Kikawa , M. Mori , KE. Nakamura , T. Nakaya , R. A. Wendell , L. H. V. Anthony , N. McCauley , P. Mehta , A. Pritchard , K. M. Tsui , Y. Fukuda , Y. Itow , T. Niwa , M. Taani , M. Tsukada , P. Mijakowski , K. Frankiewicz , C. K. Jung , C. Vilela , M. J. Wilking , C. Yanagisawa , D. Fukuda , M. Harada , K. Hagiwara , T. Horai , H. Ishino , S. Ito , Y. Koshio , M. Sakuda , Y. Takahira , C. Xu , Y. Kuno , D. Barrow , L. Cook , C. Simpson , D. Wark , F. Nova , T. Boschi , F. Di Lodovico , S. Molina Sedgwick , S. Zsoldos , S. B. Kim , J. Y. Yang , M. Thiesse , L. Thompson , H. Okazawa , Y. Choi , K. Nishijima , M. Koshiba , M. Yokoyama , A. Goldsack , K. Martens , B. Quilain , Y. Suzuki , M. R. Vagins , M. Kuze , T. Yoshida , M. Ishitsuka , R. Matsumoto , K. Ohta , J. F. Martin , C. M. Nantais , H. A. Tanaka , T. Towstego , M. Hartz , A. Konaka , P. de Perio , N. W. Prouse , S. Chen , B. D. Xu , B. Richards , B. Jamieson , J. Walker , A. Minamino , K. Okamoto , G. Pintaudi

Ongoing improvements in the measurement of positronium transition intervals motivate the calculation of the $O(m \alpha^7)$ corrections to these intervals. In this work we focus on corrections to the spin-singlet parapositronium energies…

High Energy Physics - Phenomenology · Physics 2016-05-25 Gregory S. Adkins , Lam M. Tran , Ruihan Wang

We show that the PAMELA anomaly in the positron fraction as well as the ATIC/PPB-BETS excesses in the e^- + e^+ flux are simultaneously explained in our scenario that a hidden U(1)H gauge boson constitutes dark matter of the Universe and…

Astrophysics · Physics 2009-09-28 Chuan-Ren Chen , Mihoko M. Nojiri , Fuminobu Takahashi , T. T. Yanagida
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