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Two new facilities have recently been proposed to measure low energy neutrino-nucleus cross sections, the nu-SNS (Spallation Neutron Source) and low energy beta beams. The former produces neutrinos by pion decay at rest, while the latter…

Nuclear Theory · Physics 2009-11-10 G. C. McLaughlin

The proposed Mitchell Institute Neutrino Experiment at Reactor (MINER) experiment at the Nuclear Science Center at Texas A&M University will search for coherent elastic neutrino-nucleus scattering within close proximity (about 2 meters) of…

Presently, there are several experimental setups dedicated to rare event searches, such as dark matter interactions or double beta decay, in the building or commissioning phases. These experiments often use large mass detectors and have…

High Energy Astrophysical Phenomena · Physics 2012-11-08 Carlos Martinez Amaya , Matteo Biassoni

The COHERENT collaboration reports the most precise measurement of the coherent elastic neutrino-nucleus scattering cross section to date. This measurement was performed with COHERENT's germanium detector array, Ge-Mini, at the Spallation…

The first eight years of operation of the Cold Neutron Chopper Spectrometer (CNCS) at the Spallation Neutron Source in Oak Ridge is being reviewed. The instrument has been part of the facility user program since 2009, and more than 250…

Instrumentation and Detectors · Physics 2016-10-12 Georg Ehlers , Andrey A. Podlesnyak , Alexander I. Kolesnikov

Several proposals for studying neutrinos with large detectors are currently under discussion. We suggest that they could provide a precise measurement of the electroweak mixing angle as well as a probe for new physics, such as non-standard…

High Energy Physics - Phenomenology · Physics 2013-05-30 E. A. Garces , O. G. Miranda , M. A. Tortola , J. W. F. Valle

The success of current and future-generation neutrinoless double beta decay experiments relies on the ability to eliminate or reduce extraneous backgrounds. In addition to constructing experiments using radiopure materials and handling in…

Instrumentation and Detectors · Physics 2026-02-09 G. Othman , C. Wiseman , T. H. Burritt , J. A. Detwiler , M. P. Held , R. Henning , T. Mathew , D. Peterson , W. Pettus , G. Song , T. D. Van Wechel

The first generation of solar neutrino experiments narrowed the allowed flavor mixing and mass parameter solutions (for nu_e <-> nu_x) to a few isolated regions of sin^2*2*theta - delta M^2 parameter space. Recently, the Small Mixing Angle…

High Energy Physics - Experiment · Physics 2007-05-23 S. A. Dazeley

We present the yield and spectra of stable secondary particles (gamma, e^+/-, nu_e, nubar_e, nu_mu, and nubar_mu) of p-p interaction in parameterized formulae to facilitate calculations involving them in astronomical environments. The…

Astrophysics · Physics 2009-11-11 Tuneyoshi Kamae , Niklas Karlsson , Tsunefumi Mizuno , Toshinori Abe , Tatsumi Koi

The Low Energy Modular Array (LEMA) is one of three instruments that compose the STROBE-X mission concept. The LEMA is a large effective-area, high throughput, non-imaging pointed instrument based on the X-ray Timing Instrument of the…

Instrumentation and Methods for Astrophysics · Physics 2024-10-14 Keith C. Gendreau , Dominic Maes , Ronald A. Remillard , Paul S. Ray , Zaven Arzoumanian , Craig Markwardt , Takashi Okajima

The KATRIN experiment will probe the neutrino mass by measuring the beta-electron energy spectrum near the endpoint of tritium beta-decay. An integral energy analysis will be performed by an electro-static spectrometer (Main Spectrometer),…

Instrumentation and Detectors · Physics 2016-05-04 M. Arenz , M. Babutzka , M. Bahr , J. P. Barrett , S. Bauer , M. Beck , A. Beglarian , J. Behrens , T. Bergmann , U. Besserer , J. Blümer , L. I. Bodine , K. Bokeloh , J. Bonn , B. Bornschein , L. Bornschein , S. Büsch , T. H. Burritt , S. Chilingaryan , T. J. Corona , L. De Viveiros , P. J. Doe , O. Dragoun , G. Drexlin , S. Dyba , S. Ebenhöch , K. Eitel , E. Ellinger , S. Enomoto , M. Erhard , D. Eversheim , M. Fedkevych , A. Felden , S. Fischer , J. A. Formaggio , F. Fränkle , D. Furse , M. Ghilea , W. Gil , F. Glück , A. Gonzalez Urena , S. Görhardt , S. Groh , S. Grohmann , R. Grössle , R. Gumbsheimer , M. Hackenjos , V. Hannen , F. Harms , N. Hauÿmann , F. Heizmann , K. Helbing , W. Herz , S. Hickford , D. Hilk , B. Hillen , T. Höhn , B. Holzapfel , M. Hötzel , M. A. Howe , A. Huber , A. Jansen , N. Kernert , L. Kippenbrock , M. Kleesiek , M. Klein , A. Kopmann , A. Kosmider , A. Kovalík , B. Krasch , M. Kraus , H. Krause , M. Krause , L. Kuckert , B. Kuffner , L. La Cascio , O. Lebeda , B. Leiber , J. Letnev , V. M. Lobashev , A. Lokhov , E. Malcherek , M. Mark , E. L. Martin , S. Mertens , S. Mirz , B. Monreal , K. Müller , M. Neuberger , H. Neumann , S. Niemes , M. Noe , N. S. Oblath , A. Off , H. -W. Ortjohann , A. Osipowicz , E. Otten , D. S. Parno , P. Plischke , A. W. P. Poon , M. Prall , F. Priester , P. C. -O. Ranitzsch , J. Reich , O. Rest , R. G. H. Robertson , M. Röllig , S. Rosendahl , S. Rupp , M. Rysavy , K. Schlösser , M. Schlösser , K. Schönung , M. Schrank , J. Schwarz , W. Seiler , H. Seitz-Moskaliuk , J. Sentkerestiova , A. Skasyrskaya , M. Slezak , A. Spalek , M. Steidl , N. Steinbrink , M. Sturm , M. Suesser , H. H. Telle , T. Thümmler , N. Titov , I. Tkachev , N. Trost , A. Unru , K. Valerius , D. Venos , R. Vianden , S. Vöcking , B. L. Wall , N. Wandkowsky , M. Weber , C. Weinheimer , C. Weiss , S. Welte , J. Wendel , K. L. Wierman , J. F. Wilkerson , D. Winzen , J. Wolf , S. Wüstling , M. Zacher , S. Zadoroghny , M. Zboril

NEXT (Neutrino Experiment with a Xenon TPC) aims to observe the neutrinoless double beta decay of \ensuremath{{}^{136}\rm Xe} in a high-pressure gas xenon Time Projection Chamber using electroluminescence to amplify the signal from…

Instrumentation and Detectors · Physics 2019-08-14 Paola Ferrario

This paper presents a quantum efficiency measurement setup based on a 2D motorized stage, a wide spectrum xenon lamp, a beam splitter system, and two calibrated photo-diodes for measuring the quantum efficiency (QE) of photomultiplier tubes…

Quantum Physics · Physics 2023-12-18 P. Migliozzi , C. M. Mollo , A. Simonelli

The MEDLEY setup based at The Svedberg Laboratory (TSL), Uppsala, Sweden has previously been used to measure double-differential cross-sections for elastic nd scattering, as well as light ion production reactions for various nuclei in the…

Nuclear Experiment · Physics 2008-04-16 P. -A. Söderström

The MEG II experiment at Paul Scherrer Institut in Switzerland will search for the lepton flavour violating muon decay, $\mu^+\to e^+\gamma$, with a sensitivity of $4\times10^{-14}$ improving the existing limit of an order of magnitude. In…

The PADME experiment, at the Laboratori Nazionali di Frascati (LNF), in Italy, will search for invisible decays of the hypothetical dark photon via the process $e^+e^-\rightarrow \gamma A'$, where the $A'$ escapes detection. The dark photon…

A new thermal neutron detector with the domestically produced THGEM (THick Gas Electron Multiplier) was developed as an alternative to 3He to meet the needs of the next generation of neutron facilities. One type of Au-coated THGEM was…

Instrumentation and Detectors · Physics 2014-08-06 Yang Lei , Zhou Jian-Rong , Sun Zhi-Jia , Zhang Ying , Huang Chao-Qiang , Sun Guang-Ai , Wang Yan-Feng , Yang Gui-An , Xu Hong , Xie Yu-Guang , Chen Yuan-Bo

To study thermodynamic properties and dynamic phase space behavior of hydrogen isotopologues (Q$_2$) at cryogenic temperatures and at high density, the Tritium Absorption InfraRed Spectroscopy 2 (T$_2$ApIR) experiment has been set up and…

We describe a concept for a NASA SMEX Mission in which Gas Electron Multiplier (GEM) detectors, developed at CERN, are adapted for use in X-ray astronomy. These detectors can be used to obtain moderately large detector area and…

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