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The purpose of the MIPP experiment is to study the inclusive production of photons, pions, kaons and nucleons in pi, K and p interactions on various targets using beams from the Main Injector at Fermilab. The function of the calorimeters is…

We report results from the first search for $\nu_\mu\to\nu_e$ transitions by the NOvA experiment. In an exposure equivalent to $2.74\times10^{20}$ protons-on-target in the upgraded NuMI beam at Fermilab, we observe 6 events in the Far…

High Energy Physics - Experiment · Physics 2016-05-03 P. Adamson , C. Ader , M. Andrews , N. Anfimov , I. Anghel , K. Arms , E. Arrieta-Diaz , A. Aurisano , D. S. Ayres , C. Backhouse , M. Baird , B. A. Bambah , K. Bays , R. Bernstein , M. Betancourt , V. Bhatnagar , B. Bhuyan , J. Bian , K. Biery , T. Blackburn , V. Bocean , D. Bogert , A. Bolshakova , M. Bowden , C. Bower , D. Broemmelsiek , C. Bromberg , G. Brunetti , X. Bu , A. Butkevich , D. Capista , E. Catano-Mur , T. R. Chase , S. Childress , B. C. Choudhary , B. Chowdhury , T. E. Coan , J. A. B. Coelho , M. Colo , J. Cooper , L. Corwin , D. Cronin-Hennessy , A. Cunningham , G. S. Davies , J. P. Davies , M. Del Tutto , P. F. Derwent , K. N. Deepthi , D. Demuth , S. Desai , G. Deuerling , A. Devan , J. Dey , R. Dharmapalan , P. Ding , S. Dixon , Z. Djurcic , E. C. Dukes , H. Duyang , R. Ehrlich , G. J. Feldman , N. Felt , E. J. Fenyves , E. Flumerfelt , S. Foulkes , M. J. Frank , W. Freeman , M. Gabrielyan , H. R. Gallagher , M. Gebhard , T. Ghosh , W. Gilbert , A. Giri , S. Goadhouse , R. A. Gomes , L. Goodenough , M. C. Goodman , V. Grichine , N. Grossman , R. Group , J. Grudzinski , V. Guarino , B. Guo , A. Habig , T. Handler , J. Hartnell , R. Hatcher , A. Hatzikoutelis , K. Heller , C. Howcroft , J. Huang , X. Huang , J. Hylen , M. Ishitsuka , F. Jediny , C. Jensen , D. Jensen , C. Johnson , H. Jostlein , G. K. Kafka , Y. Kamyshkov , S. M. S. Kasahara , S. Kasetti , K. Kephart , G. Koizumi , S. Kotelnikov , I. Kourbanis , Z. Krahn , V. Kravtsov , A. Kreymer , Ch. Kulenberg , A. Kumar , T. Kutnink , R. Kwarciancy , J. Kwong , K. Lang , A. Lee , W. M. Lee , K. Lee , S. Lein , J. Liu , M. Lokajicek , J. Lozier , Q. Lu , P. Lucas , S. Luchuk , P. Lukens , G. Lukhanin , S. Magill , K. Maan , W. A. Mann , M. L. Marshak , M. Martens , J. Martincik , P. Mason , K. Matera , M. Mathis , V. Matveev , N. Mayer , E. McCluskey , R. Mehdiyev , H. Merritt , M. D. Messier , H. Meyer , T. Miao , D. Michael , S. P. Mikheyev , W. H. Miller , S. R. Mishra , R. Mohanta , A. Moren , L. Mualem , M. Muether , S. Mufson , J. Musser , H. B. Newman , J. K. Nelson , E. Niner , A. Norman , J. Nowak , Y. Oksuzian , A. Olshevskiy , J. Oliver , T. Olson , J. Paley , P. Pandey , A. Para , R. B. Patterson , G. Pawloski , N. Pearson , D. Perevalov , D. Pershey , E. Peterson , R. Petti , S. Phan-Budd , L. Piccoli , A. Pla-Dalmau , R. K. Plunkett , R. Poling , B. Potukuchi , F. Psihas , D. Pushka , X. Qiu , N. Raddatz , A. Radovic , R. A. Rameika , R. Ray , B. Rebel , R. Rechenmacher , B. Reed , R. Reilly , D. Rocco , D. Rodkin , K. Ruddick , R. Rusack , V. Ryabov , K. Sachdev , S. Sahijpal , H. Sahoo , O. Samoylov , M. C. Sanchez , N. Saoulidou , P. Schlabach , J. Schneps , R. Schroeter , J. Sepulveda-Quiroz , P. Shanahan , B. Sherwood , A. Sheshukov , J. Singh , V. Singh , A. Smith , D. Smith , J. Smolik , N. Solomey , A. Sotnikov , A. Sousa , K. Soustruznik , Y. Stenkin , M. Strait , L. Suter , R. L. Talaga , M. C. Tamsett , S. Tariq , P. Tas , R. J. Tesarek , R. B. Thayyullathil , K. Thomsen , X. Tian , S. C. Tognini , R. Toner , J. Trevor , G. Tzanakos , J. Urheim , P. Vahle , L. Valerio , L. Vinton , T. Vrba , A. V. Waldron , B. Wang , Z. Wang , A. Weber , A. Wehmann , D. Whittington , N. Wilcer , R. Wildberger , D. Wildman , K. Williams , S. G. Wojcicki , K. Wood , M. Xiao , T. Xin , N. Yadav , S. Yang , S. Zadorozhnyy , J. Zalesak , B. Zamorano , A. Zhao , J. Zirnstein , R. Zwaska

Knowledge of the neutrino flux produced by the Neutrinos at the Main Injector (NuMI) beamline is essential to the neutrino oscillation and neutrino interaction measurements of the MINERvA, MINOS+, NOvA and MicroBooNE experiments at Fermi…

This paper presents a novel neutral-pion reconstruction that takes advantage of the machine learning technique of semantic segmentation using MINERvA data collected between 2013-2017, with an average neutrino energy of $6$ GeV. Semantic…

We report on the response of a prototype CMS hadron calorimeter module to charged particle beams of pions, muons, and electrons with momenta up to 375 GeV/c. The data were taken at the H2 and H4 beamlines at CERN in 1995 and 1996. The…

Measurements of the double-differential $\pi^{\pm}$ production cross-section in the range of momentum $0.5 \GeVc \leq p \le 8.0 \GeVc$ and angle $0.025 \rad \leq \theta \le 0.25 \rad$ in interactions of charged pions on beryllium, carbon,…

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

This Letter presents an investigation of low-energy electron-neutrino interactions in the Fermilab Booster Neutrino Beam by the MicroBooNE experiment, motivated by the excess of electron-neutrino-like events observed by the MiniBooNE…

High Energy Physics - Experiment · Physics 2025-07-16 MicroBooNE collaboration , P. Abratenko , D. Andrade Aldana , L. Arellano , J. Asaadi , A. Ashkenazi , S. Balasubramanian , B. Baller , A. Barnard , G. Barr , D. Barrow , J. Barrow , V. Basque , J. Bateman , O. Benevides Rodrigues , S. Berkman , A. Bhat , M. Bhattacharya , M. Bishai , A. Blake , B. Bogart , T. Bolton , M. B. Brunetti , L. Camilleri , D. Caratelli , F. Cavanna , G. Cerati , A. Chappell , Y. Chen , J. M. Conrad , M. Convery , L. Cooper-Troendle , J. I. Crespo-Anadon , R. Cross , M. Del Tutto , S. R. Dennis , P. Detje , R. Diurba , Z. Djurcic , K. Duffy , S. Dytman , B. Eberly , P. Englezos , A. Ereditato , J. J. Evans , C. Fang , B. T. Fleming , W. Foreman , D. Franco , A. P. Furmanski , F. Gao , D. Garcia-Gamez , S. Gardiner , G. Ge , S. Gollapinni , E. Gramellini , P. Green , H. Greenlee , L. Gu , W. Gu , R. Guenette , P. Guzowski , L. Hagaman , M. D. Handley , O. Hen , C. Hilgenberg , G. A. Horton-Smith , A. Hussain , B. Irwin , M. S. Ismail , C. James , X. Ji , J. H. Jo , R. A. Johnson , Y. J. Jwa , D. Kalra , G. Karagiorgi , W. Ketchum , M. Kirby , T. Kobilarcik , N. Lane , J. -Y. Li , Y. Li , K. Lin , B. R. Littlejohn , L. Liu , W. C. Louis , X. Luo , T. Mahmud , C. Mariani , D. Marsden , J. Marshall , N. Martinez , D. A. Martinez Caicedo , S. Martynenko , A. Mastbaum , I. Mawby , N. McConkey , L. Mellet , J. Mendez , J. Micallef , K. Mistry , T. Mohayai , A. Mogan , M. Mooney , A. F. Moor , C. D. Moore , L. Mora Lepin , M. M. Moudgalya , S. Mulleria Babu , D. Naples , A. Navrer-Agasson , N. Nayak , M. Nebot-Guinot , C. Nguyen , 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 , K. Pletcher , I. Pophale , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , M. Reggiani-Guzzo , J. Rodriguez Rondon , M. Rosenberg , M. Ross-Lonergan , I. Safa , 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 , N. Taniuchi , K. Terao , C. Thorpe , D. Torbunov , D. Totani , M. Toups , A. Trettin , Y. -T. Tsai , J. Tyler , M. A. Uchida , T. Usher , B. Viren , J. Wang , M. Weber , H. Wei , A. J. White , S. Wolbers , T. Wongjirad , M. Wospakrik , K. Wresilo , W. Wu , E. Yandel , T. Yang , L. E. Yates , H. W. Yu , G. P. Zeller , J. Zennamo , C. Zhang

NOvA is a long-baseline neutrino oscillation experiment. It is optimized to measure $\nu_e$ appearance and $\nu_{\mu}$ disappearance at the Far Detector in the $\nu_{\mu}$ beam produced by the NuMI facility at Fermilab. NOvA uses a…

Instrumentation and Detectors · Physics 2019-10-30 Shiqi Yu

Predictions from widely-used neutrino-nucleus interaction event generators are compared to measurements of transverse kinematic imbalances, made by both the T2K and MINERvA experiments, to allow a joint characterisation of the nuclear…

High Energy Physics - Experiment · Physics 2018-11-05 Stephen Dolan

Calorimeters for particle physics experiments with integration time of a few ns will substantially improve the capability of the experiment to resolve event pileup and to reject backgrounds. In this paper the time development of hadronic…

Instrumentation and Detectors · Physics 2018-05-24 Dmitri Denisov , Strahinja Lukić , Nikolai Mokhov , Sergei Striganov , Predrag Ujić

The velocity of a ~3 GeV neutrino beam is measured by comparing detection times at the Near and Far detectors of the MINOS experiment, separated by 734 km. A total of 473 Far Detector neutrino events was used to measure (v-c)/c = 5.1 +/-…

High Energy Physics - Experiment · Physics 2008-11-26 MINOS Collaboration , P. Adamson

Recent results obtained by the HARP collaboration on the measurements of the double-differential production cross-section of positive and negative pions in proton interactions with nuclear targets from Beryllium to Lead are presented. They…

High Energy Physics - Experiment · Physics 2019-08-13 Roumen Tsenov

NOvA is a long-baseline neutrino oscillation experiment. It uses the NuMI beam from Fermilab and two sampling calorimeter detectors placed off-axis from the beam. The 293 ton Near Detector measures the unoscillated neutrino energy spectrum,…

High Energy Physics - Experiment · Physics 2017-10-12 Biswaranjan Behera

This is an updated version of the NOvA proposal. The detector is a 30 kiloton tracking calorimeter, 15.7 m by 15.7 m by 132 m long, with alternating horizontal and vertical rectangular cells of liquid scintillator contained in PVC extrusion…

High Energy Physics - Experiment · Physics 2007-05-23 The NOvA Collaboration , D. Ayres

The fine-sampling electromagnetic calorimeter prototype has been experimentally tested using the 1-19 GeV/c tagged beams of negatively charged particles at the U70 accelerator at IHEP, Protvino. The energy resolution measured by electrons…

The electron-neutrino charged-current quasi-elastic (CCQE) cross-section on nuclei is an important input parameter to appearance-type neutrino oscillation experiments. Current experiments typically work from the muon neutrino cross-section…

High Energy Physics - Experiment · Physics 2019-08-13 Jeremy Wolcott

A large area plastic scintillator detector array(~ 1 m x1m) has been set up for fast neutron spectroscopy at the BARC-TIFR Pelletron laboratory, Mumbai. The energy, time and position response has been measured for electrons using…

Nuclear Experiment · Physics 2009-01-16 P. C. Rout , D. R. Chakrabarty , V. M. Datar , Suresh Kumar , E. T. Mirgule , A. Mitra , V. Nanal , R. Kujur

The total systematic uncertainty of the neutrino flux in accelerator-based neutrino experiments is dominated by the Monte Carlo modeling of hadronic interactions. Direct hadron production measurements for T2K and Fermilab neutrino…

High Energy Physics - Experiment · Physics 2020-11-03 Simona Ilieva