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Peng Zhang , Ping Zhang , Qingmin Zhang , Rongping Zhang , Rui Zhang , Shaoping Zhang , Shiqi Zhang , Shu Zhang , Shuihan Zhang , Siyuan Zhang , Tao Zhang , Xiaofeng Zhang , Xiaomei Zhang , Xin Zhang , Xu Zhang , Xuan Zhang , Xuantong Zhang , Xuesong Zhang , Xueyao Zhang , Yan Zhang , Yibing Zhang , Yinhong Zhang , Yiyu Zhang , Yizhou Zhang , Yongjie Zhang , Yongpeng Zhang , Yu Zhang , Yuanyuan Zhang , Yue Zhang , Yueyuan Zhang , Yumei Zhang , Yuning Zhang , Zhenyu Zhang , Zhicheng Zhang , Zhijian Zhang , Zhixuan Zhang , Baoqi Zhao , Fengyi Zhao , Jie Zhao , Liang Zhao , Mei Zhao , Rong Zhao , Runze Zhao , Shujun Zhao , Tianchi Zhao , Tianhao Zhao , Yubin Zhao , Dongqin Zheng , Hua Zheng , Xiangyu Zheng , Yangheng Zheng , Weili Zhong , Weirong Zhong , Albert Zhou , Guorong Zhou , Li Zhou , Lishui Zhou , Min Zhou , Shun Zhou , Tong Zhou , Xiang Zhou , Xing Zhou , Yan Zhou , Haiwen Zhu , Jiang Zhu , Jingsen Zhu , Jingyu Zhu , Kangfu Zhu , Kejun Zhu , Zhihang Zhu , Ivan Zhutikov , Bo Zhuang , Honglin Zhuang , Liang Zong , Jiaheng Zou , Sebastian Zwickel , Jan Züfle
We report the measurement of the differential cross section $d^{2}\sigma (E_{\nu})/ d\cos(\theta_{\mu}) dP_{\mu}$ for inclusive muon-neutrino charged-current scattering on argon. This measurement utilizes data from 6.4$\times10^{20}$…
High Energy Physics - Experiment · Physics
2025-11-27
MicroBooNE Collaboration , P. Abratenko , O. Alterkait , D. Andrade Aldana , L. Arellano , J. Asaadi , A. Ashkenazi , S. Balasubramanian , B. Baller , G. Barr , D. Barrow , J. Barrow , V. Basque , O. Benevides Rodrigues , S. Berkman , A. Bhanderi , A. Bhat , M. Bhattacharya , M. Bishai , A. Blake , B. Bogart , T. Bolton , J. Y. Book , L. Camilleri , Y. Cao , D. Caratelli , I. Caro Terrazas , F. Cavanna , G. Cerati , Y. Chen , J. M. Conrad , M. Convery , L. Cooper-Troendle , J. I. Crespo-Anadon , M. Del Tutto , S. R. Dennis , P. Detje , A. Devitt , R. Diurba , Z. Djurcic , R. Dorrill , K. Duffy , S. Dytman , B. Eberly , P. Englezos , A. Ereditato , J. J. Evans , R. Fine , O. G. Finnerud , B. T. Fleming , N. Foppiani , W. Foreman , D. Franco , A. P. Furmanski , D. Garcia-Gamez , S. Gardiner , G. Ge , S. Gollapinni , O. Goodwin , E. Gramellini , P. Green , H. Greenlee , W. Gu , R. Guenette , P. Guzowski , L. Hagaman , O. Hen , R. Hicks , C. Hilgenberg , G. A. Horton-Smith , Z. Imani , B. Irwin , R. Itay , C. James , X. Ji , L. Jiang , J. H. Jo , R. A. Johnson , Y. J. Jwa , D. Kalra , N. Kamp , G. Karagiorgi , W. Ketchum , M. Kirby , T. Kobilarcik , I. Kreslo , M. B. Leibovitch , I. Lepetic , J. -Y. Li , K. Li , Y. Li , K. Lin , B. R. Littlejohn , H. Liu , W. C. Louis , X. Luo , C. Mariani , D. Marsden , J. Marshall , N. Martinez , D. A. Martinez Caicedo , A. Mastbaum , N. McConkey , V. Meddage , J. Micallef , K. Miller , K. Mistry , T. Mohayai , A. Mogan , M. Mooney , A. F. Moor , C. D. Moore , L. Mora Lepin , M. Moudgalya , S. Mulleria Babu , D. Naples , A. Navrer-Agasson , N. Nayak , M. Nebot-Guinot , J. Nowak , N. Oza , O. Palamara , N. Pallat , V. Paolone , A. Papadopoulou , V. Papavassiliou , H. Parkinson , S. F. Pate , N. Patel , Z. Pavlovic , E. Piasetzky , I. Ponce-Pinto , I. Pophale , S. Prince , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , M. Reggiani-Guzzo , L. Ren , L. Rochester , J. Rodriguez Rondon , M. Rosenberg , M. Ross-Lonergan , C. Rudolph von Rohr , I. Safa , G. Scanavini , D. W. Schmitz , A. Schukraft , W. Seligman , M. H. Shaevitz , R. Sharankova , J. Shi , E. L. Snider , M. Soderberg , S. Soldner-Rembold , J. Spitz , M. Stancari , J. St. John , T. Strauss , A. M. Szelc , W. Tang , N. Taniuchi , K. Terao , C. Thorpe , D. Torbunov , D. Totani , M. Toups , Y. -T. Tsai , J. Tyler , M. A. Uchida , T. Usher , B. Viren , M. Weber , H. Wei , A. J. White , Z. Williams , S. Wolbers , T. Wongjirad , M. Wospakrik , K. Wresilo , N. Wright , W. Wu , E. Yandel , T. Yang , L. E. Yates , H. W. Yu , G. P. Zeller , J. Zennamo , C. Zhang
The central detector in the MuSun experiment is a pad-plane time projection ionization chamber that operates without gas amplification in deuterium at 31 K; it is used to measure the rate of the muon capture process $\mu^- + d \rightarrow n…
Instrumentation and Detectors · Physics
2015-06-19
R. A. Ryan , F. Wauters , F. E. Gray , P. Kammel , A. Nadtochy , D. Peterson , T. van Wechel , E. Gross , M. Gubanich , L. Kochenda , P. Kravtsov , M. H. Murray , D. Orozco , R. Osofsky , G. E. Petrov , J. D. Phillips , J. Stroud , V. Trofimov , A. Vasilyev , M. Vznuzdaev
Future LHC luminosity upgrades will significantly increase the amount of background hits from photons, neutrons and protons in the detectors of the ATLAS muon spectrometer. At the proposed LHC peak luminosity of 5*10^34 1/cm^2s, background…
Instrumentation and Detectors · Physics
2017-08-23
Andre Zibell , Otmar Biebel , Ralf Hertenberger , Alexander Ruschke , Christopher Schmitt , Hubert Kroha , Bernhard Bittner , Philipp Schwegler , Jörg Dubbert , Sebastian Ott
The ATLAS Forward Proton (AFP) detector is intended to measure protons scattered at small angles from the ATLAS interaction point. To this end, a combination of 3D Silicon pixel tracking modules and Quartz-Cherenkov time-of-flight (ToF)…
Instrumentation and Detectors · Physics
2016-11-03
J. Lange , L. Adamczyk , G. Avoni , E. Banas , A. Brandt , M. Bruschi , P. Buglewicz , E. Cavallaro , D. Caforio , G. Chiodini , L. Chytka , K. Ciesla , P. M. Davis , M. Dyndal , S. Grinstein , K. Janas , K. Jirakova , M. Kocian , K. Korcyl , I. Lopez Paz , D. Northacker , L. Nozka , M. Rijssenbeek , L. Seabra , R. Staszewski , P. Swierska , T. Sykora
A muon tracking system consisting of four 9cm x 10cm sized bulk Micromegas detectors with 128um amplification-gap and two 10cm x 10cm triple GEM detectors is foreseen for high-precision tracking of 140GeV muons at the H8 beamline at CERN…
Instrumentation and Detectors · Physics
2015-06-03
Jonathan Bortfeldt , Otmar Biebel , David Heereman , Ralf Hertenberger
The Deep Underground Neutrino Experiment currently under construction in the US will be a long-baseline neutrino oscillation experiment dedicated to determining the neutrino mass ordering and to measure the CP violation phase in the lepton…
The underground muon detector of the Pierre Auger Observatory is aimed at attaining direct measurements of the muonic component of extensive air showers produced by cosmic rays with energy from $10^{16.5}$ eV up to the region of the ankle…
Instrumentation and Methods for Astrophysics · Physics
2021-09-01
A. M. Botti , F. Sánchez , M. Roth , A. Etchegoyen
We developed a 12-liter volume neutron detector filled with the liquid scintillator EJ301 that measures neutrons in an underground laboratory where dark matter and neutrino experiments are located. The detector target is a cylindrical…
Instrumentation and Detectors · Physics
2015-06-15
C. Zhang , D. -M. Mei , P. Davis , B. Woltman , F. Gray
The performance of a muon radiography system designed to image the inner structure of a nuclear plant located at a distance of 64 m was evaluated. We concluded absence of the fuel in the pressure vessel during the measurement period and…
Instrumentation and Detectors · Physics
2016-06-21
H. Fujii , K. Hara , S. Hashimoto , F. Ito , H. Kakuno , S. H. Kim , M. Kochiyama , K. Nagamine , A. Suzuki , Y. Takada , Y. Takahashi , F. Takasaki , S. Yamashita
Liquid Argon Time Projection Chambers (LArTPCs) have been selected for the future long-baseline Deep Underground Neutrino Experiment (DUNE). To allow LArTPCs to operate in the high-multiplicity near detector environment of DUNE, a new…
Instrumentation and Detectors · Physics
2018-01-30
J. Asaadi , M. Auger , A. Ereditato , D. Goeldi , R. Haenni , U. Kose , I Kreslo , D. Lorca , M. Luethi , C. Rudolf Von Rohr , J. R. Sinclair , F. Stocker , C. Tognina , M. Weber
As part of the upgrade of the Pierre Auger Observatory, known as AugerPrime, the Underground Muon Detector is being installed in the low-energy extension of the Surface Detector, allowing for a direct measurement of the muonic component of…
DUNE (Deep Underground Neutrino Experiment) is a proposed long-baseline neutrino experiment in the US with a baseline of 1300 km from Fermi National Accelerator Laboratory (Fermilab) to Sanford Underground Research Facility, which will…
DUNE (Dark Universe Explorer) is a proposed mission to measure parameters of dark energy using weak gravitational lensing The particular challenges of both optical and infrared focal planes and the DUNE baseline solution is discussed. The…
Astrophysics · Physics
2009-11-13
Jeff Booth , Mark Cropper , Frank Eisenhauer , Alexandre Refregier , the DUNE collaboration
DUNE is an international project, currently in its design phase, for neutrino physics and proton-decay searches. It will consist of two detectors exposed to a megawatt-scale muon neutrino beam that will be produced at Fermilab (Illinois,…
The ATLAS detector at the Large Hadron Collider has collected several hundred million cosmic ray events during 2008 and 2009. These data were used to commission the Muon Spectrometer and to study the performance of the trigger and tracking…
A prototype for the instrumented decay tunnel of ENUBET was tested in 2018 at the CERN East Area facility with charged particles up to 5 GeV. This detector is a longitudinal sampling calorimeter with lateral scintillation light readout. The…
Instrumentation and Detectors · Physics
2020-08-26
F. Acerbi , M. Bonesini , F. Bramati , A. Branca , C. Brizzolari , G. Brunetti , S. Capelli , S. Carturan , M. G. Catanesi , S. Cecchini , F. Cindolo , G. Collazuol , E. Conti , F. Dal Corso , C. Delogu , G. De Rosa , A. Falcone , A. Gola , C. Jollet , B. Klicek , Y. Kudenko , M. Laveder , A. Longhin , L. Ludovici , E. Lutsenko , L. Magaletti , G. Mandrioli , A. Margotti , V. Mascagna , N. Mauri , L. Meazza , A. Meregaglia , M. Mezzetto , A. Paoloni , M. Pari , E. Parozzi , L. Pasqualini , G. Paternoster , L. Patrizii , M. Pozzato , M. Prest , F. Pupilli , E. Radicioni , C. Riccio , A. C. Ruggeri , C. Scian , G. Sirri , M. Stipcevic , M. Tenti , F. Terranova , M. Torti , E. Vallazza , L. Votano