English
Related papers

Related papers: Charged kaon lifetime at KLOE

200 papers

Recent results are presented for (1) the charge asymmetry in semielectronic kaon decay; (2) the charge radius of the neutral kaon; (3) the decay Klong -> pi0 pi0 e+e-; (4) constraints on rho(CKM) from kaon decays; (5) lepton flavor…

High Energy Physics - Experiment · Physics 2019-08-14 L. Bellantoni

With the aim of achieving a better and more complete understanding of neutrino interactions with nuclear targets, the coherent production of charged kaons induced by neutrinos and antineutrinos is investigated in the energy range of some of…

Nuclear Theory · Physics 2013-05-30 L. Alvarez-Ruso , J. Nieves , I. Ruiz Simo , M. Valverde , M. J. Vicente Vacas

A sample of 1.25x10^9 phi decays, collected with the KLOE detector at the Frascati phi-factory DAFNE at center of mass energy ~ Mphi, has been used to study the radiative decay phi to eta pi0 gamma. This decay is dominated by phi to a0(980)…

High Energy Physics - Experiment · Physics 2012-08-27 The KLOE collaboration

The Liquid Argon Purity Demonstrator was an R&D test stand designed to determine if electron drift lifetimes adequate for large neutrino detectors could be achieved without first evacuating the cryostat. We describe here the cryogenic…

The KLOE-2 experiment is undergoing commissioning at the DA$\Phi$NE $e^{+}e^{-}$ collider of the Frascati National Laboratory of the INFN, after the integration of new detectors in the former KLOE apparatus. The Inner Tracker, a very light…

Instrumentation and Detectors · Physics 2015-06-23 A. Di Cicco , G. Morello

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

Electric field enhanced electron spin coherence is characterized using time-resolved Faraday rotation spectroscopy in n-type ZnO epilayers grown by molecular beam epitaxy. An in-plane dc electric field E almost doubles the transverse spin…

Materials Science · Physics 2009-11-13 S. Ghosh , D. W. Steuerman , B. Maertz , K. Ohtani , Huaizhe Xu , H. Ohno , D. D. Awschalom

The study of the electromagnetic form factors of the nucleon in both the space-like and time-like domains plays a key role for the understanding of the internal structure and dynamics of this basic building block of the matter. Form factors…

High Energy Physics - Experiment · Physics 2007-05-23 P. Rossi

DA$\Phi$NE $e^+ e^-$ collider is an abundant source of low energy $K \bar K$ pairs suitable to explore different fields of non perturbative QCD regime. Two different experiments, DEAR and FINUDA, using different experimental techniq ues are…

Nuclear Experiment · Physics 2012-05-22 Paola Gianotti

Experimental data on the number of neutrons born in the heavy water targets of the large neutrino detectors are used to set the limit on the proton life-time independently on decay mode through the reaction d -> n+?. The best up-to-date…

Nuclear Experiment · Physics 2008-11-26 V. I. Tretyak , Yu. G. Zdesenko

Electron-photon temporal correlations in electron energy loss (EELS) and cathodoluminescence (CL) spectroscopies have recently been used to measure the relative quantum efficiency of materials. This combined spectroscopy, named…

The tau lepton lifetime is measured with the L3 detector at LEP using the complete data taken at centre-of-mass energies around the Z pole resulting in tau_tau = 293.2 +/- 2.0 (stat) +/- 1.5 (syst) fs. The comparison of this result with the…

High Energy Physics - Experiment · Physics 2012-08-27 L3 Collaboration

Phonon lifetime calculations from first principles usually rely on time consuming molecular dynamics calculations, or density functional perturbation theory (DFPT) where the zero temperature crystal structure is assumed to be dynamically…

Statistical Mechanics · Physics 2015-05-27 Petros Souvatzis

The absolute branching ratio of the $K^+ \rightarrow \pi^+\pi^-\pi^+(\gamma)$ decay, inclusive of final-state radiation, has been measured using $\sim$17 million tagged $K^+$ mesons collected with the KLOE detector at DA$\Phi$NE, the…

High Energy Physics - Experiment · Physics 2014-09-16 2 Collaboration

We report a measurement of the positive muon lifetime to a precision of 1.0 parts per million (ppm); it is the most precise particle lifetime ever measured. The experiment used a time-structured, low-energy muon beam and a segmented plastic…

The decay $\eta \rightarrow \pi^+ \pi^- \pi^0$ is studied with the KLOE detector, at the DA$\phi$NE e$^+$e$^-$ collider. Using a data sample corresponding to an integrated luminosity of $1.6$ fb$^{-1}$ a new study of the Dalitz plot is…

High Energy Physics - Experiment · Physics 2018-07-08 L. Caldeira Balkeståhl

Charged and neutral current low energy neutrino cross section predictions from a variety of Monte Carlo generators in present use are compared against existing experimental data. Comparisons are made to experimental data on quasi-elastic,…

High Energy Physics - Experiment · Physics 2007-05-23 G. P. Zeller

In this work we calculate the lifetime of quarkonium moving with velocity $v$ through a quark gluon plasma at temperature $T$. We also investigate the stability of heavy mesons with respect to the effects of color charge screening. An…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sidi Cherkawi Benzahra , Benjamin F. Bayman