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The next generation of very-short-baseline reactor experiments will require compact detectors operating at surface level and close to a nuclear reactor. This paper presents a new detector concept based on a composite solid scintillator…

The Accelerator Neutrino Neutron Interaction Experiment (ANNIE) is designed to serve as a test bed for new detector technologies in future water and liquid scintillator based neutrino experiments. Located on the Booster Neutrino Beam at…

Instrumentation and Detectors · Physics 2019-10-22 Emrah Tiras

The Short Baseline Near Detector (SBND) is a 112 ton active mass liquid argon time projection chamber (LArTPC) that will begin operations in the Booster Neutrino Beamline at Fermilab in 2020. Its main physics goals include high-statistics…

Instrumentation and Detectors · Physics 2019-10-21 Georgia Karagiorgi

We report the observation of neutrino interactions without final state muons at the LHC, with a significance of 6.4$ \sigma$. A data set of proton-proton collisions at $\sqrt{s}= 13.6$ TeV collected by SND@LHC in 2022 and 2023 is used,…

High Energy Physics - Experiment · Physics 2024-12-02 LHC Collaboration

The Forward Physics Facility (FPF) plans to use neutrinos produced at the Large Hadron Collider (LHC) to make a variety of measurements at previously unexplored TeV energies. Its primary goals include precision measurements of the neutrino…

High Energy Physics - Phenomenology · Physics 2023-10-11 Callum Wilkinson , Alfonso Garcia Soto

Hadron collisions at the LHC offer a unique opportunity to study strong interactions. The exciting data collected by the four RHIC experiments suggest that in heavy-ion collisions at sqrt(s_NN) = 200 GeV, an equilibrated, strongly-coupled…

Nuclear Experiment · Physics 2007-05-23 Christof Roland

The model of heavy neutral leptons (HNLs) is one of the well-motivated models beyond the standard model (BSM) from both theoretical and phenomenological point of views. It is an indispensable ingredient to explain the puzzle of tiny…

High Energy Physics - Phenomenology · Physics 2020-11-04 Kingman Cheung , Yi-Lun Chung , Hiroyuki Ishida , Chih-Ting Lu

We describe a start-timing detector for the PHENIX experiment at the relativistic heavy-ion collider RHIC. The role of the detector is to detect a nuclear collision, provide precise time information with an accuracy of 50ps, and determine…

Instrumentation and Detectors · Physics 2009-10-31 K. Ikematsu , Y. Iwata , K. Kaimi , M. Kaneta , T. Kohama , N. Maeda , K. Matsukado , H. Ohnishi , K. Ono , A. Sakaguchi , T. Sugitate , Y. Sumi , Y. Takata , M. Tanabe , A. Yokoro

In addition to their broad physics reach enabled by their high energies and precision, future multi-TeV muon colliders will also be the world's most intense sources of neutrinos. This offers the opportunity to search for new non-standard…

High Energy Physics - Phenomenology · Physics 2026-05-11 Felix Kling , Yang Ma , Krzysztof Mękała , Jürgen Reuter , Zahra Tabrizi

The Multi-Purpose Detector (MPD) is to be installed at the Nuclotron Ion Collider fAcility (NICA) of the Joint Institute for Nuclear Research (JINR). Its main goal is to study the phase diagram of the strongly interacting matter produced in…

In July 2018 an optimization run for the proposed charm cross section measurement for SHiP was performed at the CERN SPS. A heavy, moving target instrumented with nuclear emulsion films followed by a silicon pixel tracker was installed in…

Instrumentation and Detectors · Physics 2022-03-21 SHiP Collaboration

In view of the LHC upgrade for the High Luminosity Phase (HL-LHC), the ATLAS experiment is planning to replace the Inner Detector with an all-Silicon system. The n-on-p technology represents a valid solution for the modules of most of the…

FASER$\nu$ is a newly proposed detector whose main mission is to detect the neutrino flux from the collision of the proton beams at the ATLAS Interaction Point (IP) during the run III of the LHC in 2022-2024. We show that this detector can…

High Energy Physics - Phenomenology · Physics 2021-04-28 Pouya Bakhti , Yasaman Farzan , Silvia Pascoli

The SHiP-charm project was proposed to measure the associated charm production induced by 400 GeV/c protons in a thick target, including the contribution from cascade production. An optimisation run was performed in July 2018 at CERN SPS…

High Energy Physics - Experiment · Physics 2024-06-10 SHiP Collaboration

In this work, prospects to probe an overlooked facet of axion-like particles (ALPs) -- their potential couplings to sterile neutrinos -- are presented. We found that mono-photon searches have the potential to constrain ALP couplings to…

High Energy Physics - Phenomenology · Physics 2020-08-18 Alexandre Alves , Alex G. Dias , Diego D. Lopes

The prototype of a TDC board has been developed for the new high granular time-of-flight neutron detector (HGND). The board is based on the standard LVDS 4x asynchronous oversampling using the xc7k160 FPGA with a 100 ps bin width. The HGND…

Instrumentation and Detectors · Physics 2024-01-23 D. Finogeev , F. Guber , A. Izvestnyy , N. Karpushkin , A. Makhnev , S. Morozov , D. Serebryakov

The Multipurpose Detector (MPD) \cite{cite1.MPD_CDR} is designed to study of hot and dense baryonic matter in collisions of heavy ions over the atomic mass range 1--197 at the centre of mass energy up to $\sqrt{S_{NN}}$ = 11 GeV (for…

SBND is a 112 ton liquid argon time projection chamber (LArTPC) neutrino detector located 110 meters from the Booster Neutrino Beam (BNB) target at Fermilab. Its main goals include searches for eV-scale sterile neutrinos as part of the…

High Energy Physics - Experiment · Physics 2025-04-08 SBND Collaboration , R. Acciarri , L. Aliaga-Soplin , O. Alterkait , R. Alvarez-Garrote , D. Andrade Aldana , C. Andreopoulos , A. Antonakis , L. Arellano , W. Badgett , S. Balasubramanian , A. Barnard , V. Basque , J. Bateman , A. Beever , E. Belchior , M. Betancourt , A. Bhat , M. Bishai , A. Blake , B. Bogart , J. Bogenschuetz , D. Brailsford , A. Brandt , S. Brickner , M. B. Brunetti , A. Bueno , L. Camilleri , A. Campos , D. Caratelli , D. Carber , B. Carlson , M. Carneiro , R. Castillo , F. Cavanna , A. Chappell , H. Chen , S. Chung , R. Coackley , J. I. Crespo-Anadón , C. Cuesta , Y. Dabburi , O. Dalager , M. Dall'Olio , R. Darby , M. Del Tutto , V. Di Benedetto , Z. Djurcic , V. do Lago Pimentel , S. Dominguez-Vidales , K. Duffy , S. Dytman , A. Ereditato , J. J. Evans , A. Ezeribe , C. Fan , A. Filkins , B. Fleming , W. Foreman , D. Franco , G. Fricano , I. Furic , A. Furmanski , S. Gao , D. Garcia-Gamez , S. Gardiner , G. Ge , I. Gil-Botella , S. Gollapinni , P. Green , W. C. Griffith , R. Guenette , P. Guzowski , L. Hagaman , A. Hamer , P. Hamilton , M. Hernandez-Morquecho , B. Howard , Z. Imani , C. James , R. S. Jones , M. Jung , T. Junk , D. Kalra , G. Karagiorgi , L. Kashur , K. Kelly , W. Ketchum , M. King , J. Klein , L. Kotsiopoulou , S. Kr Das , T. Kroupova , V. A. Kudryavtsev , N. Lane , H. Lay , R. LaZur , J. -Y. Li , K. Lin , B. Littlejohn , L. Liu , W. C. Louis , E. Lourenco , X. Lu , X. Luo , A. Machado , P. Machado , C. Mariani , F. Marinho , J. Marshall , A. Mastbaum , K. Mavrokoridis , N. McConkey , B. McCusker , M. Mooney , A. F. Moor , G. Moreno Granados , C. A. Moura , J. Mueller , S. Mulleriababu , A. Navrer-Agasson , M. Nebot-Guinot , V. C. L. Nguyen , F. J. Nicolas-Arnaldos , J. Nowak , S. Oh , N. Oza , O. Palamara , N. Pallat , V. Pandey , A. Papadopoulou , H. B. Parkinson , J. L. Paton , L. Paudel , L. Paulucci , Z. Pavlovic , D. Payne , L. Pelegrina Gutiérrez , J. Plows , F. Psihas , G. Putnam , X. Qian , R. Rajagopalan , P. Ratoff , H. Ray , M. Reggiani-Guzzo , M. Roda , J. Romeo-Araujo , M. Ross-Lonergan , N. Rowe , P. Roy , I. Safa , A. Sanchez-Castillo , P. Sanchez-Lucas , D. W. Schmitz , A. Schneider , A. Schukraft , H. Scott , E. Segreto , J. Sensenig , M. Shaevitz , B. Slater , J. Smith , M. Soares-Nunes , M. Soderberg , S. Söldner-Rembold , J. Spitz , M. Stancari , T. Strauss , A. M. Szelc , C. Thorpe , D. Totani , M. Toups , C. Touramanis , L. Tung , G. A. Valdiviesso , R. G. Van de Water , A. Vázquez Ramos , L. Wan , M. Weber , H. Wei , T. Wester , A. White , A. Wilkinson , P. Wilson , T. Wongjirad , E. Worcester , M. Worcester , S. Yadav , E. Yandel , T. Yang , L. Yates , B. Yu , H. Yu , J. Yu , B. Zamorano , J. Zennamo , C. Zhang

A plastic scintillator paddle detector with embedded fiber light guides and photomultiplier tube readout, referred to as the Reaction Plane Detector (RXNP), was designed and installed in the PHENIX experiment prior to the 2007 run of the…

In view of the LHC upgrade phases towards the High Luminosity LHC (HL-LHC), the ATLAS experiment plans to upgrade the Inner Detector with an all-silicon system. Because of its radiation hardness and cost effectiveness, the n-on-p silicon…

Instrumentation and Detectors · Physics 2013-11-18 M. Bomben , A. Bagolini , M. Boscardin , L. Bosisio , G. Calderini , J. Chauveau , G. Giacomini , A. La Rosa , G. Marchori , N. Zorzi
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