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We calculate the transverse muon polarization in the decay $K^{\pm}\to\pi^0\mu^{\pm}\nu$ induced by the electromagnetic two-photon final-state interaction. For the central part of the Dalitz plot the typical value of this polarization is…

High Energy Physics - Phenomenology · Physics 2009-10-31 V. P. Efrosinin , I. B. Khriplovich , G. G. Kirilin , Yu. G. Kudenko

We test whether or not the tau lepton manifests the same couplings as the mu lepton by investigating the relative decay rates in purely leptonic D+ meson decays. Specifically, we place the first upper limit on the ratio R=Gamma(D+ -> tau+…

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

Recent STAR measurements suggest a difference in the global spin polarization between hyperons and anti-hyperons, especially at relatively low collision beam energy. One possible cause of this difference is the potential presence of…

Nuclear Theory · Physics 2019-09-18 Yu Guo , Shuzhe Shi , Shengqin Feng , Jinfeng Liao

We point out the following astrophysical consequences of a tau neutrino with mass in the MeV range: (i) if it has a small electric charge which will allow it to become a cold dark matter of the universe, then present limits on the 511 KeV…

High Energy Physics - Phenomenology · Physics 2016-09-01 R. N. Mohapatra , S. Nussinov

The time-dependent analysis of the decays $\Lambda_b\to \Lambda +D^0(t)$ and $\Lambda_b\to \Lambda +\bar{D}^0(t)$ is discussed. The effect of particle mixing due to time evolution of $D^0$ and $\bar{D}^0$ on the observables for these decays…

High Energy Physics - Phenomenology · Physics 2007-05-23 Fayyazuddin

The HyperCP collaboration has recently reported the observation of three events for the decay Sigma^+ -> p mu^+ mu^-. They have suggested that new physics may be required to understand the implied decay rate and the observed M_{mumu}…

High Energy Physics - Phenomenology · Physics 2009-11-11 Xiao-Gang He , Jusak Tandean , G. Valencia

Recently, much work has been devoted to the calculation of order $\alpha$ corrections to the decay rate of pionium, the $\pi^+ \pi^-$ bound state. In previous calculations, nonrelativistic QED corrections were neglected since they start at…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Labelle , K. Buckley

A generalization of the Gell-Mann-Low theorem is applied to the antimuon-electron system. The bound state spectrum is extracted numerically. As a result, fine and hyperfine structure are reproduced correctly near the nonrelativistic limit…

High Energy Physics - Theory · Physics 2008-11-26 Axel Weber

A search for proton decay into $e^+/\mu^+$ and a $\eta$ meson has been performed using data from a 0.373 Mton$\cdot$year exposure (6050.3 live days) of Super-Kamiokande. Compared to previous searches this work introduces an improved model…

High Energy Physics - Experiment · Physics 2024-10-01 Kamiokande Collaboration , N. Taniuchi , K. Abe , S. Abe , Y. Asaoka , C. Bronner , M. Harada , Y. Hayato , K. Hiraide , K. Hosokawa , K. Ieki , M. Ikeda , J. Kameda , Y. Kanemura , R. Kaneshima , Y. Kashiwagi , Y. Kataoka , S. Miki , S. Mine , M. Miura , S. Moriyama , M. Nakahata , S. Nakayama , Y. Noguchi , G. Pronost , K. Okamoto , K. Sato , H. Sekiya , H. Shiba , K. Shimizu , M. Shiozawa , Y. Sonoda , Y. Suzuki , A. Takeda , Y. Takemoto , A. Takenaka , H. Tanaka , S. Watanabe , T. Yano , T. Kajita , K. Okumura , T. Tashiro , T. Tomiya , X. Wang , S. Yoshida , G. D. Megias , P. Fernandez , L. Labarga , N. Ospina , B. Zaldivar , B. W. Pointon , E. Kearns , J. Mirabito , J. L. Raaf , L. Wan , T. Wester , J. Bian , N. J. Griskevich , W. R. Kropp , S. Locke , M. B. Smy , H. W. Sobel , V. Takhistov , A. Yankelevich , J. Hill , M. C. Jang , J. Y. Kim , S. H. Lee , I. T. Lim , D. H. Moon , R. G. Park , B. S. Yang , B. Bodur , K. Scholberg , C. W. Walter , A. Beauchêne , L. Bernard , A. Coffani , O. Drapier , S. El Hedri , A. Giampaolo , Th. A. Mueller , A. D. Santos , P. Paganini , R. Rogly , T. Nakamura , J. S. Jang , L. N. Machado , J. G. Learned , K. Choi , N. Iovine , S. Cao , L. H. V. Anthony , D. Martin , N. W. Prouse , M. Scott , A. A. Sztuc , Y. Uchida , V. Berardi , N. F. Calabria , M. G. Catanesi , E. Radicioni , A. Langella , G. De Rosa , G. Collazuol , M. Feltre , F. Iacob , M. Lamoureux , M. Mattiazzi , L. Ludovici , M. Gonin , L. Périssé , B. Quilain , C. Fujisawa , S. Horiuchi , M. Kobayashi , Y. M. Liu , Y. Maekawa , Y. Nishimura , R. Okazaki , R. Akutsu , M. Friend , T. Hasegawa , T. Ishida , T. Kobayashi , M. Jakkapu , T. Matsubara , T. Nakadaira , K. Nakamura , Y. Oyama , A. Portocarrero Yrey , K. Sakashita , T. Sekiguchi , T. Tsukamoto , N. Bhuiyan , T. Boschi , G. T. Burton , F. Di Lodovico , J. Gao , A. Goldsack , T. Katori , J. Migenda , R. M. Ramsden , M. Taani , Z. Xie , S. Zsoldos , Y. Kotsar , H. Ozaki , A. T. Suzuki , Y. Takagi , Y. Takeuchi , S. Yamamoto , H. Zhong , J. Feng , L. Feng , S. Han , J. R. Hu , Z. Hu , M. Kawaue , T. Kikawa , M. Mori , T. Nakaya , R. A. Wendell , K. Yasutome , S. J. Jenkins , N. McCauley , P. Mehta , A. Tarrant , M. J. Wilking , Y. Fukuda , Y. Itow , H. Menjo , K. Ninomiya , Y. Yoshioka , J. Lagoda , M. Mandal , P. Mijakowski , Y. S. Prabhu , J. Zalipska , M. Jia , J. Jiang , C. K. Jung , W. Shi , C. Yanagisawa , Y. Hino , H. Ishino , S. Ito , H. Kitagawa , Y. Koshio , W. Ma , F. Nakanishi , S. Sakai , T. Tada , T. Tano , T. Ishizuka , G. Barr , D. Barrow , L. Cook , S. Samani , D. Wark , A. Holin , F. Nova , S. Jung , J. Y. Yang , J. Yoo , J. E. P. Fannon , L. Kneale , M. Malek , J. M. McElwee , O. Stone , P. Stowell , M. D. Thiesse , L. F. Thompson , S. T. Wilson , H. Okazawa , S. M. Lakshmi , S. B. Kim , E. Kwon , M. W. Lee , J. W. Seo , I. Yu , A. K. Ichikawa , K. D. Nakamura , S. Tairafune , K. Nishijima , M. Koshiba , A. Eguchi , S. Goto , K. Iwamoto , Y. Mizuno , T. Muro , K. Nakagiri , Y. Nakajima , S. Shima , E. Watanabe , M. Yokoyama , P. de Perio , S. Fujita , C. Jesús-Valls , K. Martens , Ll. Marti , K. M. Tsui , M. R. Vagins , J. Xia , S. Izumiyama , M. Kuze , R. Matsumoto , K. Terada , R. Asaka , M. Inomoto , M. Ishitsuka , H. Ito , T. Kinoshita , Y. Ommura , N. Shigeta , M. Shinoki , T. Suganuma , K. Yamauchi , T. Yoshida , Y. Nakano , J. F. Martin , H. A. Tanaka , T. Towstego , R. Gaur , V. Gousy-Leblanc , M. Hartz , A. Konaka , X. Li , S. Chen , Y. Wu , B. D. Xu , A. Q. Zhang , B. Zhang , M. Posiadala-Zezula , S. B. Boyd , R. Edwards , D. Hadley , M. Nicholson , M. O'Flaherty , B. Richards , A. Ali , B. Jamieson , S. Amanai , A. Minamino , G. Pintaudi , S. Sano , R. Sasaki , R. Shibayama , R. Shimamura , S. Suzuki , K. Wada

The ratio of B+ and B0 meson lifetimes was measured using data collected in 2002-2004 by the D0 experiment in Run II of the Fermilab Tevatron Collider. These mesons were reconstructed in B -> mu+ nu D*- X decays, which are dominated by B0,…

High Energy Physics - Experiment · Physics 2008-11-26 D0 Collaboration , V. M. Abazov

We have searched for proton decays via p -> e^+ pi^0 and p -> mu^+ pi^0 using data from a 91.7 kiloton year exposure of Super-Kamiokande-I and a 49.2 kiloton year exposure of Super-Kamiokande-II. No candidate events were observed with…

High Energy Physics - Experiment · Physics 2012-08-27 Kamiokande Collaboration , H. Nishino , S. Clark

As we have pointed out in (arXiv:1806.10107 [hep-ph]), the existence of neutron dark matter decay modes "n -> chi + anything", where "chi" is a dark matter fermion, for the solution of the neutron lifetime problem changes priorities and…

High Energy Physics - Phenomenology · Physics 2018-12-05 A. N. Ivanov , R. Höllwieser , N. I. Troitskaya , M. Wellenzohn , Ya. A. Berdnikov

We have derived constraints on the tau neutrino mass and fourth generation mixing from an analysis of the partial widths of tau lepton decays, in particular: tau -> e nu nu_tau, tau -> mu nu nu_tau, tau -> pi nu_tau, tau -> K nu_tau. We…

High Energy Physics - Phenomenology · Physics 2008-11-26 John Swain , Lucas Taylor

We construct an effective non-relativistic quantum field theory that describes bound states of pi+ pi- pairs and their hadronic decays. We then derive a general expression for the lifetime of the ground state at next-to-leading order in…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. Gasser , V. E. Lyubovitskij , A. Rusetsky , A. Gall

Experiments such as MACS and the proposed MACE study muonium-antimuonium conversion by the energies of the final-state $e^\pm$. The $e^+$ and $e^-$ from an antimuonium decay tend to be non-relativistic and relativistic, respectively, and…

High Energy Physics - Phenomenology · Physics 2025-10-31 Mitrajyoti Ghosh , Kevin Liguori , Takemichi Okui , Kohsaku Tobioka

We have searched for the leptonic and radiative leptonic B decays, B^+ -> mu^+ nu, B^+ -> e^+ nu gamma and B^+ -> mu^+ nu gamma. Using a 140 fb^{-1} data sample collected with the Belle detector at the KEKB asymmetric e^+ e^- collider, we…

High Energy Physics - Experiment · Physics 2019-08-14 K. Abe

Results on $B \to \mu^+ \mu^-$ decays with the CMS experiment are reported, using 61 fb$^{-1}$ of data recorded during LHC Run 1 and 2016. With an improved muon identification algorithm and refined unbinned maximum likelihood fitting…

High Energy Physics - Experiment · Physics 2020-12-02 Urs Langenegger

The complete 2-loop quantum electrodynamic corrections to the muon lifetime are calculated in the Fermi theory. The exact result for the effects of virtual and real photons, virtual electrons, muons as well as e+e- pair creation is Delta…

High Energy Physics - Phenomenology · Physics 2008-11-26 Timo van Ritbergen , Robin G. Stuart

Some recent precision experiments in low energy muon physics are discussed. Spectroscopy on the muonium atom, the bound state of a positve muon and an electron, has provided precise tests of standard theory and yielded most precise values…

Nuclear Experiment · Physics 2016-09-08 Klaus P. Jungmann