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The EDELWEISS II experiment is devoted to the search for Weakly Interacting Massive Particles (WIMP) that would constitute the Dark Matter halo of our Galaxy. For this purpose, the experiment uses cryogenic germanium detectors, cooled down…

Cosmology and Nongalactic Astrophysics · Physics 2014-11-20 Veronique Sanglard

Dark matter (DM) particles with mass in the sub-GeV range are an attractive alternative to heavier weakly-interacting massive particles, but direct detection of such light particles is challenging. If however DM-nucleus scattering leads to…

High Energy Physics - Phenomenology · Physics 2018-09-12 Matthew J. Dolan , Felix Kahlhoefer , Christopher McCabe

The Korea Invisible Mass Search(KIMS) experiment presents new limits on WIMP-nucleon cross section using the data from an exposure of 3409 kgd taken with low background CsI(Tl) crystals at Yangyang underground laboratory. The most stringent…

The Heidelberg Dark Matter Search Experiment (HDMS) is a new ionization Germanium experiment in a special design. Two concentric Ge crystals are housed by one cryostat system, the outer detector acting as an effective shield against…

Astrophysics · Physics 2008-11-26 L. Baudis , A. Dietz , B. Majorovits , F. Schwamm , H. Strecker , H. V. Klapdor-Kleingrothaus

The lack of an unambiguous signal for thermally produced dark matter particles in direct detection, indirect detection, and collider searches calls for broadening the search strategies by probing a wider range of dark matter masses with…

Instrumentation and Detectors · Physics 2024-09-09 Margarita Kaznacheeva , Karoline Schäffner

Line intensity mapping (LIM) can provide a powerful means to constrain the theory of gravity and the nature of dark energy at low and high redshifts by mapping the large-scale structure (LSS) over many redshift epochs. In this paper, we…

Cosmology and Nongalactic Astrophysics · Physics 2023-04-18 Azadeh Moradinezhad Dizgah , Emilio Bellini , Garrett K. Keating

We investigate the possibility of using the cosmic gravitational focusing (CGF) to probe the minor light dark matter (DM) component whose mass is in the range of $(0.1 \sim 100)$\,eV. Being a purely gravitational effect, the CGF offers a…

High Energy Physics - Phenomenology · Physics 2025-09-26 Shao-Feng Ge , Liang Tan

We present a comprehensive survey of CII* absorption detections toward stars within 100 pc in order to measure the distribution of electron densities present in the local interstellar medium (LISM). Using high spectral resolution…

Astrophysics · Physics 2009-11-13 Seth Redfield , Ross E. Falcon

Searches for weakly interacting massive particles(WIMP) can be based on the dete ction of nuclear recoil energy in CsI(Tl) crystals. We demonstrate that low energy gamma rays down to few keV is detected with CsI(Tl) crystal detector. A…

Instrumentation and Detectors · Physics 2019-08-17 H. J. Kim , H. J. Ahn , S. K. Kim , E. Won , T. Y. Kim , Y. D. Kim , M. H. Lee , J. S. Chai , J. H. Ha

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

Dark Matter experiments are recently focusing their detection techniques in low-mass WIMPs, which requires the use of light elements and low energy threshold. In this context, we present the TREX-DM experiment, a low background…

Understanding the ability to measure and discriminate particle events at the lowest possible energy is an essential requirement in developing new experiments to search for weakly interacting massive particle (WIMP) dark matter. In this…

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

A new design of a cryogenic germanium detector for dark matter search is presented, taking advantage of the coplanar grid technique of event localisation for improved background discrimination. Experiments performed with prototype devices…

We make a systematic and comparative study for the LHC and ILC for the electroweakino searches in the Minimal Supersymmetric Standard Model. We adopt a general bottom-up approach and scan over the parameter regions for all the three cases…

High Energy Physics - Phenomenology · Physics 2013-10-01 Mikael Berggren , Tao Han , Jenny List , Sanjay Padhi , Shufang Su , Tomohiko Tanabe

A search for dark matter using an underground single-phase liquid xenon detector was conducted at the Kamioka Observatory in Japan, particularly for Weakly Interacting Massive Particles (WIMPs). We have used 705.9 live days of data in a…

SuperCDMS SNOLAB will be a next-generation experiment aimed at directly detecting low-mass (< 10 GeV/c$^2$) particles that may constitute dark matter by using cryogenic detectors of two types (HV and iZIP) and two target materials…

Particle detectors that use liquid xenon (LXe) as detection medium are among the leading technologies in the search for dark matter weakly interacting massive particles (WIMPs). A key enabling element has been the low-energy detection…

In the cosmological paradigm, cold dark matter (DM) dominates the mass content of the Universe and is present at every scale. Candidates for DM include many extensions of the standard model, with a weakly interacting massive particle (WIMP)…

High Energy Astrophysical Phenomena · Physics 2019-08-14 B. Zitzer