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The ATLAS and CMS experiments did not find evidence for Supersymmetry using close to 5/fb of published LHC data at a center-of-mass energy of 7 TeV. We combine these LHC data with data on B_s -> mu mu (LHCb experiment), the relic density…

High Energy Physics - Phenomenology · Physics 2012-10-08 C. Beskidt , W. de Boer , D. I. Kazakov , F. Ratnikov

The DEAP-3600 experiment is a single-phase detector that uses 3600 Kg of liquid argon to search for Dark Matter at SNOLAB, Sudbury, Canada, 6800 ft. underground. The projected sensitivity to the spin-independent WIMP-nucleon cross-section…

Instrumentation and Detectors · Physics 2017-06-19 P. Giampa

We present the latest results from the search for light dark matter particle interactions with the DarkSide-50 dual-phase liquid argon time projection chamber. This analysis, based on the ionization signal only, improves the existing limits…

High Energy Physics - Experiment · Physics 2024-07-18 D. Franco

New Experiments With Spheres-Gas (NEWS-G) is a direct dark matter detection experiment using Spherical Proportional Counters (SPCs) with light noble gases to search for low-mass Weakly Interacting Massive Particles (WIMPs). We report the…

Critical probes of dark matter come from tests of its elastic scattering with nuclei. The results are typically assumed to be model-independent, meaning that the form of the potential need not be specified and that the cross sections on…

High Energy Physics - Phenomenology · Physics 2023-01-02 Matthew C. Digman , Christopher V. Cappiello , John F. Beacom , Christopher M. Hirata , Annika H. G. Peter

Direct detection experiments aim at the detection of dark matter in the form of weakly interacting massive particles (WIMPs) by searching for signals from elastic dark matter nucleus scattering. Additionally, inelastic scattering in which…

High Energy Physics - Phenomenology · Physics 2020-01-08 G. Arcadi , C. Döring , C. Hasterok , S. Vogl

The dark matter in the Universe might be composed of superheavy particles (mass >~ 10^10 GeV). These particles can be detected via nuclear recoils produced in elastic scatterings from nuclei. We estimate the observable rate of strongly…

Astrophysics · Physics 2009-11-07 Ivone F. M. Albuquerque , Laura Baudis

The PICASSO dark matter search experiment operated an array of 32 superheated droplet detectors containing 3.0 kg of C$_{4}$F$_{10}$ and collected an exposure of 231.4 kgd at SNOLAB between March 2012 and January 2014. We report on the…

We study scenarios where Dark Matter is a weakly interacting particle (WIMP) embedded in an ElectroWeak multiplet. In particular, we consider real SU(2) representations with zero hypercharge, that automatically avoid direct detection…

High Energy Physics - Phenomenology · Physics 2022-01-19 Salvatore Bottaro , Dario Buttazzo , Marco Costa , Roberto Franceschini , Paolo Panci , Diego Redigolo , Ludovico Vittorio

The p-type point-contact germanium detectors are novel techniques offering kg-scale radiation sensors with sub-keV sensitivities. They have been used for light Dark Matter WIMPs searches and may have potential applications in neutrino…

Instrumentation and Detectors · Physics 2014-03-14 H. B. Li , the TEXONO Collaboration

We study the reach of direct detection experiments for large bound states (containing $10^4$ or more dark nucleons) of Asymmetric Dark Matter. We consider ordinary nuclear recoils, excitation of collective modes (phonons), and electronic…

High Energy Physics - Phenomenology · Physics 2019-09-04 Ahmet Coskuner , Dorota M. Grabowska , Simon Knapen , Kathryn M. Zurek

We review various issues related to the direct detection of constituents of dark matter, which are assumed to be Weakly Interacting Massive Particles (WIMPs). We specifically consider heavy WIMPs such as: 1) The lightest supersymmetric…

Nuclear Theory · Physics 2017-08-23 J. D. Vergados

Dark matter particles with masses in the sub-GeV range have escaped severe constraints from direct detection experiments such as LUX, PANDAX-II and XENON100 as the corresponding recoil energies are, largely, lower than the detector…

High Energy Physics - Phenomenology · Physics 2019-10-16 Debajyoti Choudhury , Divya Sachdeva

In the recent years, many low-threshold dark matter (DM) direct detection experiments have reported the observation of unexplained excesses of events at low energies. Exemplary for these, the experiment CRESST has detected unidentified…

High Energy Physics - Phenomenology · Physics 2022-02-23 Riccardo Catena , Vanessa Zema

We compute the projected sensitivity to dark matter (DM) particles in the sub-GeV mass range of future direct detection experiments using germanium and silicon semiconductor targets. We perform this calculation within the dark photon model…

High Energy Physics - Phenomenology · Physics 2020-06-03 Erik Andersson , Alex Bökmark , Riccardo Catena , Timon Emken , Henrik Klein Moberg , Emil Åstrand

The LUX-ZEPLIN experiment is a dark matter detector centered on a dual-phase xenon time projection chamber operating at the Sanford Underground Research Facility in Lead, South Dakota, USA. This Letter reports results from LUX-ZEPLIN's…

High Energy Physics - Experiment · Physics 2023-08-07 J. Aalbers , D. S. Akerib , C. W. Akerlof , A. K. Al Musalhi , F. Alder , A. Alqahtani , S. K. Alsum , C. S. Amarasinghe , A. Ames , T. J. Anderson , N. Angelides , H. M. Araújo , J. E. Armstrong , M. Arthurs , S. Azadi , A. J. Bailey , A. Baker , J. Balajthy , S. Balashov , J. Bang , J. W. Bargemann , M. J. Barry , J. Barthel , D. Bauer , A. Baxter , K. Beattie , J. Belle , P. Beltrame , J. Bensinger , T. Benson , E. P. Bernard , A. Bhatti , A. Biekert , T. P. Biesiadzinski , H. J. Birch , B. Birrittella , G. M. Blockinger , K. E. Boast , B. Boxer , R. Bramante , C. A. J. Brew , P. Brás , J. H. Buckley , V. V. Bugaev , S. Burdin , J. K. Busenitz , M. Buuck , R. Cabrita , C. Carels , D. L. Carlsmith , B. Carlson , M. C. Carmona-Benitez , M. Cascella , C. Chan , A. Chawla , H. Chen , J. J. Cherwinka , N. I. Chott , A. Cole , J. Coleman , M. V. Converse , A. Cottle , G. Cox , W. W. Craddock , O. Creaner , D. Curran , A. Currie , J. E. Cutter , C. E. Dahl , A. David , J. Davis , T. J. R. Davison , J. Delgaudio , S. Dey , L. de Viveiros , A. Dobi , J. E. Y. Dobson , E. Druszkiewicz , A. Dushkin , T. K. Edberg , W. R. Edwards , M. M. Elnimr , W. T. Emmet , S. R. Eriksen , C. H. Faham , A. Fan , S. Fayer , N. M. Fearon , S. Fiorucci , H. Flaecher , P. Ford , V. B. Francis , E. D. Fraser , T. Fruth , R. J. Gaitskell , N. J. Gantos , D. Garcia , A. Geffre , V. M. Gehman , J. Genovesi , C. Ghag , R. Gibbons , E. Gibson , M. G. D. Gilchriese , S. Gokhale , B. Gomber , J. Green , A. Greenall , S. Greenwood , M. G. D. van der Grinten , C. B. Gwilliam , C. R. Hall , S. Hans , K. Hanzel , A. Harrison , E. Hartigan-O'Connor , S. J. Haselschwardt , S. A. Hertel , G. Heuermann , C. Hjemfelt , M. D. Hoff , E. Holtom , J. Y-K. Hor , M. Horn , D. Q. Huang , D. Hunt , C. M. Ignarra , R. G. Jacobsen , O. Jahangir , R. S. James , S. N. Jeffery , W. Ji , J. Johnson , A. C. Kaboth , A. C. Kamaha , K. Kamdin , V. Kasey , K. Kazkaz , J. Keefner , D. Khaitan , M. Khaleeq , A. Khazov , I. Khurana , Y. D. Kim , C. D. Kocher , D. Kodroff , L. Korley , E. V. Korolkova , J. Kras , H. Kraus , S. Kravitz , H. J. Krebs , L. Kreczko , B. Krikler , V. A. Kudryavtsev , S. Kyre , B. Landerud , E. A. Leason , C. Lee , J. Lee , D. S. Leonard , R. Leonard , K. T. Lesko , C. Levy , J. Li , F. -T. Liao , J. Liao , J. Lin , A. Lindote , R. Linehan , W. H. Lippincott , R. Liu , X. Liu , Y. Liu , C. Loniewski , M. I. Lopes , E. Lopez Asamar , B. López Paredes , W. Lorenzon , D. Lucero , S. Luitz , J. M. Lyle , P. A. Majewski , J. Makkinje , D. C. Malling , A. Manalaysay , L. Manenti , R. L. Mannino , N. Marangou , M. F. Marzioni , C. Maupin , M. E. McCarthy , C. T. McConnell , D. N. McKinsey , J. McLaughlin , Y. Meng , J. Migneault , E. H. Miller , E. Mizrachi , J. A. Mock , A. Monte , M. E. Monzani , J. A. Morad , J. D. Morales Mendoza , E. Morrison , B. J. Mount , M. Murdy , A. St. J. Murphy , D. Naim , A. Naylor , C. Nedlik , C. Nehrkorn , F. Neves , A. Nguyen , J. A. Nikoleyczik , A. Nilima , J. O'Dell , F. G. O'Neill , K. O'Sullivan , I. Olcina , M. A. Olevitch , K. C. Oliver-Mallory , J. Orpwood , D. Pagenkopf , S. Pal , K. J. Palladino , J. Palmer , M. Pangilinan , N. Parveen , S. J. Patton , E. K. Pease , B. Penning , C. Pereira , G. Pereira , E. Perry , T. Pershing , I. B. Peterson , A. Piepke , J. Podczerwinski , D. Porzio , S. Powell , R. M. Preece , K. Pushkin , Y. Qie , B. N. Ratcliff , J. Reichenbacher , L. Reichhart , C. A. Rhyne , A. Richards , Q. Riffard , G. R. C. Rischbieter , J. P. Rodrigues , A. Rodriguez , H. J. Rose , R. Rosero , P. Rossiter , T. Rushton , G. Rutherford , D. Rynders , J. S. Saba , D. Santone , A. B. M. R. Sazzad , R. W. Schnee , P. R. Scovell , D. Seymour , S. Shaw , T. Shutt , J. J. Silk , C. Silva , G. Sinev , K. Skarpaas , W. Skulski , R. Smith , M. Solmaz , V. N. Solovov , P. Sorensen , J. Soria , I. Stancu , M. R. Stark , A. Stevens , T. M. Stiegler , K. Stifter , R. Studley , B. Suerfu , T. J. Sumner , P. Sutcliffe , N. Swanson , M. Szydagis , M. Tan , D. J. Taylor , R. Taylor , W. C. Taylor , D. J. Temples , B. P. Tennyson , P. A. Terman , K. J. Thomas , D. R. Tiedt , M. Timalsina , W. H. To , A. Tomás , Z. Tong , D. R. Tovey , J. Tranter , M. Trask , M. Tripathi , D. R. Tronstad , C. E. Tull , W. Turner , L. Tvrznikova , U. Utku , J. Va'vra , A. Vacheret , A. C. Vaitkus , J. R. Verbus , E. Voirin , W. L. Waldron , A. Wang , B. Wang , J. J. Wang , W. Wang , Y. Wang , J. R. Watson , R. C. Webb , A. White , D. T. White , J. T. White , R. G. White , T. J. Whitis , M. Williams , W. J. Wisniewski , M. S. Witherell , F. L. H. Wolfs , J. D. Wolfs , S. Woodford , D. Woodward , S. D. Worm , C. J. Wright , Q. Xia , X. Xiang , Q. Xiao , J. Xu , M. Yeh , J. Yin , I. Young , P. Zarzhitsky , A. Zuckerman , E. A. Zweig

We report the results of an experimental search for ultralight axion-like dark matter in the mass range 162 neV to 166 neV. The detection scheme of our Cosmic Axion Spin Precession Experiment (CASPEr) is based on a precision measurement of…

Dark matter pair production at high energy colliders may leave observable signatures in the energy and momentum spectra of the objects recoiling against the dark matter. We use LEP data on mono-photon events with large missing energy to…

High Energy Physics - Phenomenology · Physics 2011-08-09 Patrick J. Fox , Roni Harnik , Joachim Kopp , Yuhsin Tsai

We show that dark matter with a per-nucleon scattering cross section $\gtrsim 10^{-28}~{\rm cm^2}$ could be discovered by liquid scintillator neutrino detectors like BOREXINO, SNO+, and JUNO. Due to the large dark matter fluxes admitted,…

High Energy Physics - Phenomenology · Physics 2019-04-24 Joseph Bramante , Benjamin Broerman , Jason Kumar , Rafael F. Lang , Maxim Pospelov , Nirmal Raj

Various WIMP dark matter searches using the full data set of XMASS-I, a single-phase liquid xenon detector, are reported in this paper. Stable XMASS-I data taking accumulated a total live time of 1590.9 days between November 20, 2013 and…

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