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The LArIAT experiment has performed the world's first measurement of the total charged-current pion cross-section on an argon target, using the repurposed ArgoNeuT detector in the Fermilab test beam. Presented here are the results of that…

High Energy Physics - Experiment · Physics 2016-11-04 Pip Hamilton

Low-Gain Avalanche Diodes (LGADs) are fast silicon sensors with internal charge multiplication and are key candidates for precision timing layers in future high-energy hadron colliders. Their operation in harsh radiation environments,…

We present selected results on strong interaction physics from the SLD experiment at the SLAC Linear Collider. We report on several new studies of 3- and 4-jet hadronic Z decays, in which jets are identified as quark, antiquark or gluon.…

High Energy Physics - Experiment · Physics 2008-11-26 D. Muller

Gain-layer degradation from exposure to radiation limits the use of Low-Gain Avalanche Diodes (LGADs) in high energy particle physics detector experiments. Proper understanding of how the gain-layer is destroyed is not available on a defect…

The main goal of the spectroscopy program at COMPASS is to explore the light-meson spectrum in the mass range below about $2\,\text{GeV}/c^2$ using diffractive dissociation reactions. Our flagship channel is the production of three charged…

High Energy Physics - Experiment · Physics 2022-09-21 Stefan Wallner

Using $(10087 \pm 44) \times 10^6$ $J/\psi$ events collected with the BESIII detector in 2009, 2012, 2018 and 2019, the tracking efficiency of charged pions is studied using the decay $J/\psi \rightarrow \pi^+ \pi^- \pi^0$. The systematic…

The QED processes e^+ e^- -> e^+ e^- \mu^+ \mu^- and e^+ e^- -> e^+ e^- \tau^+ \tau^- are studied with the L3 detector at LEP using an untagged data sample collected at centre-of-mass energies 161 GeV < sqrt{s} < 209 GeV. The tau-pairs are…

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

Upcoming experiments need improved simulations of neutrino scattering. This work uses the popular GENIE event generator to test a variety of neutrino interaction models against recent MicroBooNE measurements of pionless charged-current…

High Energy Physics - Phenomenology · Physics 2026-05-18 Liang Liu , Steven Gardiner , Steven Dytman

To extract the charge radius of the proton, $r_{p}$, from the electron scattering data, the PRad collaboration at Jefferson Lab has developed a rigorous framework for finding the best functional forms - the fitters - for a robust extraction…

This paper describes a new way to reconstruct and identify muons with high efficiency and high pion rejection. Since muons at the ILC are often produced with or in jets, for many of the physics channels of interest[1], an efficient…

Instrumentation and Detectors · Physics 2015-06-26 C. Milstene , G. Fisk , A. Para

The Deep Underground Neutrino Experiment (DUNE) Far Detector (FD) will be formed by four 10-kton Liquid Argon (LAr) Time Projection Chambers (TPC) using both single and dual-phase technology. The dual-phase technology foreseen the charge…

Instrumentation and Detectors · Physics 2019-11-19 Chiara Lastoria

We searched for proton decay via $p \to e^{+}\pi^{0}\pi^{0}$ and $p \to \mu^{+}\pi^{0}\pi^{0}$ in 0.401 megaton-years of data collected in all pure water detector phases of Super-Kamiokande (SK) I-V. A theoretical study predicts proton…

High Energy Physics - Experiment · Physics 2026-04-17 Kamiokande Collaboration , K. Abe , S. Abe , Y. Asaoka , M. Harada , Y. Hayato , K. Hiraide , T. H. Hung , K. Hosokawa , K. Ieki , M. Ikeda , J. Kameda , Y. Kanemura , R. Kaneshima , Y. Kashiwagi , Y. Kataoka , S. Miki , S. Mine , M. Miura , S. Moriyama , K. Nakagiri , M. Nakahata , S. Nakayama , Y. Noguchi , G. Pronost , K. Okamoto , K. Sato , H. Sekiya , H. Shiba , K. Shimizu , R. Shinoda , M. Shiozawa , Y. Sonoda , Y. Suzuki , A. Takeda , Y. Takemoto , A. Takenaka , H. Tanaka , T. Yano , S. Chen , Y. Itow , T. Kajita , R. Nishijima , K. Okumura , T. Tashiro , T. Tomiya , X. Wang , S. Yoshida , P. Fernandez , L. Labarga , D. Samudio , B. Zaldivar , F. G. Garay , B. W. Pointon , C. Yanagisawa , B. Jargowsky , E. Kearns , J. Mirabito , J. L. Raaf , L. Wan , T. Wester , J. Bian , B. Cortez , N. J. Griskevich , Y. Jiang , S. Locke , M. B. Smy , H. W. Sobel , V. Takhistov , H. G. Berns , J. Hill , M. C. Jang , S. H. Lee , D. H. Moon , R. G. Park , B. S. Yang , B. Bodur , K. Scholberg , C. W. Walter , A. Beauchêne , O. Drapier , A. Ershova , M. Ferey , A. Giampaolo , Z. Hu , E. Le Blévec , Th. A. Mueller , A. D. Santos , P. Paganini , C. Quach , R. Rogly , T. Nakamura , J. S. Jang , R. P. Litchfield , L. N. Machado , F. J. P. Soler , 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 , N. Ospina , E. Radicioni , A. Langella , G. De Rosa , G. Collazuol , M. Feltre , F. Iacob , M. Mattiazzi , L. Ludovici , M. Gonin , L. Périssé , B. Quilain , M. Fukazawa , C. Fujisawa , S. Horiuchi , A. Kawabata , M. Kobayashi , Y. M. Liu , Y. Maekawa , Y. Nishimura , A. Oka , R. Okazaki , R. Akutsu , M. Friend , T. Hasegawa , Y. Hino , 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 , G. T. Burton , F. Di Lodovico , J. Gao , A. Goldsack , T. Katori , R. Kralik , N. Latham , J. Migenda , R. M. Ramsden , V. Siccardi , S. Zsoldos , S. Aoyama , H. Bambara , H. Ito , T. Sone , A. T. Suzuki , Y. Takagi , Y. Takeuchi , S. Wada , H. Zhong , M. Nishigami , Y. Inaba , J. Feng , L. Feng , S. Han , J. Hikida , J. R. Hu , M. Kawaue , T. Kikawa , T. Nakaya , T. V. Ngoc , R. A. Wendell , K. Yasutome , S. J. Jenkins , N. McCauley , P. Mehta , A. Tarrant , M. Fanì , M. J. Wilking , Z. Xie , Y. Fukuda , H. Menjo , K. Ninomiya , Y. Yoshioka , J. Lagoda , M. Mandal , P. Mijakowski , J. Zalipska , M. Mori , M. Jia , J. Jiang , C. K. Jung , W. Shi , K. Hamaguchi , H. Ishino , Y. Koshio , F. Nakanishi , S. Sakai , T. Tada , T. Tano , Y. Asano , S. Ohshita , T. Ishizuka , G. Barr , D. Barrow , L. Cook , S. Samani , D. Wark , A. Holin , F. Nova , M. Jo , S. Jung , J. Y. Yang , J. Yoo , J. E. P. Fannon , L. Kneale , M. Malek , J. M. McElwee , T. Peacock , P. Stowell , M. D. Thiesse , L. F. Thompson , S. T. Wilson , H. Okazawa , S. M. Lakshmi , S. Hong , S. B. Kim , E. Kwon , M. W. Lee , J. W. Seo , I. Yu , Y. Ashida , A. K. Ichikawa , K. D. Nakamura , S. Tairafune , A. Eguchi , S. Goto , H. Hayasaki , S. Kodama , Y. Kong , Y. Masaki , Y. Mizuno , T. Muro , M. Sekiyama , T. Yamazumi , Y. Nakajima , S. Shima , N. Taniuchi , E. Watanabe , M. Yokoyama , P. de Perio , S. Fujita , C. Jesús-Valls , K. Martens , Ll. Marti , K. M. Tsui , M. R. Vagins , J. Xia , M. Kuze , S. Izumiyama , R. Matsumoto , K. Terada , R. Asaka , M. Ishitsuka , C. Ise , Y. Ommura , N. Shigeta , M. Shinoki , M. Sugo , M. Wako , K. Yamauchi , T. Yoshida , Y. Nakano , A. Yankelevich , F. Cormier , R. Gaur , V. Gousy-Leblanc , M. Hartz , A. Konaka , X. Li , B. R. Smithers , S. Chen , Y. Wu , B. D. Xu , A. Q. Zhang , B. Zhang , H. Adhikary , M. Girgus , P. Govindaraj , M. Posiadala-Zezula , Y. S. Prabhu , S. B. Boyd , R. Edwards , D. Hadley , M. Nicholson , M. O'Flaherty , B. Richards , A. Ali , B. Jamieson , S. Amanai , C. Bronner , D. Horiguchi , A. Minamino , Y. Sasaki , R. Shibayama , R. Shimamura , S. Suzuki

The multipole content of pion photoproduction at the $\Delta^+ (1232)$ resonance has been extracted from a data set dominated by recent Mainz Microtron (MAMI) precision measurements. The analysis has been carried out in the Athens Model…

Nuclear Experiment · Physics 2018-08-01 L. Markou , E. Stiliaris , C. N. Papanicolas

Low Gain Avalanche Detectors (LGADs) are n-on-p silicon sensors with an extra p-layer below the collection electrode which provides signal amplification. When the primary electrons reach the amplification region new electron-hole pairs are…

A search was made for a new light gauge boson $X$ which might be produced in $\pi^{0}\to\gamma + X$ decay from neutral pions generated by 450-GeV protons in the CERN SPS neutrino target. The X's would penetrate the downstream shielding and…

High Energy Physics - Experiment · Physics 2008-11-26 The NOMAD Collaboration , J. Altegoer et al

Low Gain Avalanche Detector (LGAD) is the baseline sensing technology of the recently proposed Minimum Ionizing Particle (MIP) end-cap timing detectors (MTD) at the Atlas and CMS experiments. The current MTD sensor is designed as a…

The main goal of the spectroscopy program at COMPASS is to explore the light-meson spectrum below about $2\,\text{GeV}/c^2$ in diffractive production. Our flagship channel is the decay into three charged pions: $p + \pi^-\to \pi^-\pi^-\pi^+…

High Energy Physics - Experiment · Physics 2018-10-26 Stefan Wallner

The ARIADNE Experiment, utilising a 1-ton dual-phase Liquid Argon Time Projection Chamber (LArTPC), aims to develop and mature optical readout technology for large scale LAr detectors. This paper describes the characterisation, using cosmic…

Instrumentation and Detectors · Physics 2020-12-02 Adam Lowe , Krishanu Majumdar , Konstantinos Mavrokoridis , Barney Philippou , Adam Roberts , Christos Touramanis , Jared Vann

This paper reports the last technological development on the Low Gain Avalanche Detector (LGAD) and introduces a new architecture of these detectors called inverse-LGAD (iLGAD). Both approaches are based on the standard Avalanche Photo…

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