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The Big Bang should have created equal amounts of matter and antimatter; however today matter remains in the Universe. The European Spallation Source neutrino Super Beam's (ESSnuSB) main objective is to demonstrate the feasibility of using…

High Energy Physics - Experiment · Physics 2018-04-03 Gul Gokbulut

The HIBEAM/NNBAR program is a proposed two-stage experiment at the European Spallation Source focusing on searches for baryon number violation via processes in which neutrons convert to antineutrons. This paper outlines the computing and…

Neutron correlation spectroscopy can exceed direct spectroscopy in the incoming beam intensity by up to two orders of magnitude at the same energy resolution. However, the propagation of the counting noise in the correlation algorithm of…

Instrumentation and Detectors · Physics 2016-09-13 F. Mezei , M. T. Caccamo , F. Migliardo , S. Magazù

Using the Monte Carlo ray tracing package McStas, we illustrate the possibilities of creating virtual experiments of the neutron spectrometer BIFROST at the European Spallation Source, ESS. With this model, we are able to benchmark BIFROST…

Instrumentation and Detectors · Physics 2025-12-24 Kristine M. L. Krighaar , Silas B. Schack , Nicolai L. Amin , Gregory S. Tucker , Rasmus Toft-Petersen , Kim Lefmann

The COHERENT experiment measures neutrino-induced recoils from coherent elastic neutrino-nucleus scattering (CEvNS) with multiple nuclear targets at the Spallation Neutron Source (SNS) at the Oak Ridge National Laboratory (ORNL), USA.…

High Energy Physics - Experiment · Physics 2026-02-18 M. Adhikari , M. Ahn , D. Amaya Matamoros , P. S. Barbeau , V. Belov , I. Bernardi , C. Bock , A. Bolozdynya , R. Bouabid , J. Browning , B. Cabrera-Palmer , N. Cedarblade-Jones , S. Chen , A. I. Colón Rivera , V. da Silva , J. Daughhetee , Y. Efremenko , S. R. Elliott , A. Erlandson , L. Fabris , M. L. Fischer , S. Foster , A. Galindo-Uribarri , E. Granados Vazquez , M. P. Green , B. Hackett , J. Hakenmüller , M. Harada , M. R. Heath , S. Hedges , Y. Hino , H. Huang , W. Huang , H. Jeong , B. A. Johnson , T. Johnson , A. Khromov , D. Kim , L. Kong , A. Konovalov , Y. Koshio , E. Kozlova , A. Kumpan , O. Kyzylova , Y. Lee , S. M. Lee , G. Li , L. Li , Z. Li , J. M. Link , J. Liu , Q. Liu , X. Lu , M. Luxnat , D. M. Markoff , J. Mattingly , H. McLaurin , K. McMichael , N. Meredith , Y. Nakajima , F. Nakanishi , J. Newby , B. Nolan , J. O'Reilly , A. Orvedahl , D. S. Parno , D. Pérez-Loureiro , D. Pershey , C. G. Prior , J. Queen , R. Rapp , H. Ray , O. Razuvaeva , D. Reyna , D. Rudik , J. Runge , D. J. Salvat , J. Sander , K. Scholberg , H. Sekiya , J. Seligman , A. Shakirov , G. Simakov , J. Skweres , W. M. Snow , V. Sosnovtsev , Q. Stefan , M. Stringer , C. Su , T. Subedi , B. Suh , B. Sur , R. Tayloe , Y. -T. Tsai , J. Vaccaro , E. E. van Nieuwenhuizen , C. J. Virtue , G. Visser , K. Walkup , E. M. Ward , R. Wendell , T. Wongjirad , C. Yang , Y. Yang , J. Yoo , C. -H. Yu , Y. Yu , A. Zaalishvili , J. Zettlemoyer , Y. Zheng

The European Spallation Source (ESS) accelerator is composed of superconducting elliptical cavities. When the facility is running, the cavities are fed with electrical field from klystrons. Parameters of this field are monitored and…

Accelerator Physics · Physics 2020-11-02 K. Klys , W. Cichalewski , W. Jalmuzna , A. Mielczarek , P. Perek , A. Napieralski

One of the key requirements for neutron scattering instruments is the Signal-to-Background ratio (SBR). This is as well a design driving requirement for many instruments at the European Spallation Source (ESS), which aspires to be the…

Instrumentation and Detectors · Physics 2019-02-20 E. Dian , K. Kanaki , A. Khaplanov , T. Kittelmann , P. Zagyvai , R. Hall-Wilton

The deployment of a low-noise 3 kg p-type point contact germanium detector at the Dresden-II power reactor, 8 meters from its 2.96 GW$_{th}$ core, is described. This location provides an unprecedented (anti)neutrino flux of 8.1$\times…

High Energy Physics - Experiment · Physics 2021-10-13 J. Colaresi , J. I. Collar , T. W. Hossbach , A. R. L. Kavner , C. M. Lewis , A. E. Robinson , K. M. Yocum

Transition-edge sensors (TESs) are capable of highly accurate single particle energy measurement. TESs have been used for a wide range of photon detection applications, particularly in astronomy, but very little consideration has been given…

Instrumentation and Detectors · Physics 2023-05-11 K. M. Patel , S. Withington , C. N. Thomas , A. G. Shard , D. J. Goldie

The so-called $X17$ particle has been proposed in order to explain a very significant resonant behaviour (in both the angular separation and invariant mass) of $e^+e^-$ pairs produced during a nuclear transition of excited $^8$Be, $^4$He…

High Energy Physics - Phenomenology · Physics 2025-09-19 Joakim Cederkäll , Yaşar Hiçyılmaz , Else Lytken , Stefano Moretti , Johan Rathsman

The wavelengths and energies of thermal and cold neutrons are ideally matched to the length and energy scales in the materials that underpin technologies of the present and future: ranging from semiconductors to magnetic devices, composites…

Accelerator Physics · Physics 2007-05-23 T. E. Mason , T. A. Gabriel , R. K. Crawford , K. W. Herwig , F. Klose , J. F. Ankner

The coherent contribution of all neutrons in neutrino nucleus scattering due to the neutral current is examined considering the Spallation Neutron Source (SNS) as a source of neutrinos. SNS is a prolific pulsed source of electron and muon…

High Energy Physics - Phenomenology · Physics 2009-06-30 J. D. Vergados , F. T. Avignone , I. Giomataris

The COHERENT collaboration measured coherent elastic neutrino-nucleus scattering (CEvNS) for the first time at the Spallation Neutron Source at Oak Ridge National Laboratory, using a CsI[Na] detector. Here we discuss the nature of the CEvNS…

High Energy Physics - Experiment · Physics 2018-01-18 Kate Scholberg

We discuss a small-scale experiment, called $\nu$-cleus, for the first detection of coherent neutrino-nucleus scattering by probing nuclear-recoil energies down to the 10 eV-regime. The detector consists of low-threshold CaWO$_4$ and…

The new generation of dedicated Engineering Strain Scanners at neutron facilities such as ENGIN-X at ISIS and SMARTS at LANSCE offer considerable increases in both the throughput of samples and the density of measurements which are feasible…

Materials Science · Physics 2007-05-23 J. A. James , J. R. Santistiban , M. R. Daymond , L. Edwards

HEIMDAL is a thermal powder diffractometer designed to operate at the European Spallation Source, world's most intense neutron source. The detailed design of the instrument, which is expected to enter user operation in 2024/2025, assumes…

Instrumentation and Detectors · Physics 2020-01-29 I. Stefanescu , M. Christensen , R. Hall-Wilton , S. Holm-Dahlin , K. Iversen , M. Klein , D. Mannix , J. Schefer , C. J. Schmidt , W. Schweika , U. Stuhr

The European Spallation Source is being constructed in Lund, Sweden and is planned to be the world's brightest pulsed spallation neutron source for cold and thermal neutron beams ($\le$ 1 eV). The facility uses a 2 GeV proton beam to…

Instrumentation and Detectors · Physics 2018-07-04 V. Santoro , D. D. DiJulio , S. Ansell , N. Cherkashyna , G. Muhrer , P. M. Bentley

During 2014 the second experimental area EAR2 was completed at the n-TOF neutron beam facility at CERN. As the neutrons are produced via spallation, by means of a high-intensity 20 GeV pulsed proton beam impinging on a thick target, the…

Instrumentation and Detectors · Physics 2019-08-14 L. Cosentino , A. Musumarra , M. Barbagallo , N. Colonna , L. Damone , A. Pappalardo , M. Piscopo , P. Finocchiaro

Back-n is a white neutron experimental facility at China Spallation Neutron Source (CSNS). The time structure of the primary proton beam make it fully applicable to use TOF (time-of-flight) method for neutron energy measuring. We implement…

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