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Related papers: Detector development for the CRESST experiment

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Direction-sensitive WIMP dark matter searches may help overcome the challenges faced by direct dark matter detection experiments. In particular, directional detectors should be able to clearly differentiate a dark matter signal from…

Instrumentation and Detectors · Physics 2014-02-04 Steven Ross

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

The hunt for dark matter remains one of the principal objectives of modern physics and cosmology. Searches for dark matter in the form of axions are proposed or underway across a range of experimental collaborations. As we look to the next…

High Energy Physics - Phenomenology · Physics 2022-05-04 J. I. McDonald

Models for light dark matter particles with masses below 1 GeV/c$^2$ are a natural and well-motivated alternative to so-far unobserved weakly interacting massive particles. Gram-scale cryogenic calorimeters provide the required detector…

Much like ordinary matter, dark matter might consist of elementary particles, and weakly interacting massive particles are one of the prime suspects. During the past decade, the sensitivity of experiments trying to directly detect them has…

Cosmology and Nongalactic Astrophysics · Physics 2017-09-05 Jianglai Liu , Xun Chen , Xiangdong Ji

The CRESST experiment aims for a detection of dark matter in the form of WIMPs. These particles are expected to scatter elastically off the nuclei of a target material, thereby depositing energy on the recoiling nucleus. CRESST uses…

Recently, the CDMS/Si experiment has observed a low energy excess of events in their dark matter search. In light of this new result we update the mirror dark matter explanation of the direction detection experiments. We find that the DAMA,…

Cosmology and Nongalactic Astrophysics · Physics 2015-06-16 R. Foot

The CRESST experiment (Cryogenic Rare Event Search with Superconducting Thermometers) searches for dark matter via the phonon and light signals of elastic scattering processes in scintillating crystals. The discrimination between a possible…

We report on recent progress in the search for dark matter particles with masses from 1 MeV to 1 GeV. Several dark matter candidates in this mass range are expected to generate measurable electronic-recoil signals in direct-detection…

Cosmology and Nongalactic Astrophysics · Physics 2023-01-02 Alvaro E. Chavarria

Cryogenic detectors are at the forefront of rare-event search experiments, including direct detection of dark matter, coherent elastic neutrino-nucleus scattering, neutrinoless double-beta decay, and searches for fractionally charged…

High Energy Physics - Experiment · Physics 2025-12-03 S. Das , R. Dey , V. K. S. Kashyap , B. Mohanty , D. Mondal , S. Banik , M. Chaudhuri , V. Iyer

In the past decades, numerous experiments have emerged to unveil the nature of dark matter, one of the most discussed open questions in modern particle physics. Among them, the CRESST experiment, located at the Laboratori Nazionali del Gran…

CRESST II is an experiment for direct WIMP search, using cryogenic detectors. The ratio of the two signals (temperature rise and scintillation light) measured for each interaction is an excellent parameter for discrimination of radioactive…

High Energy Physics - Experiment · Physics 2007-05-23 H. Wulandari , F. von Feilitzsch , M. Huber , Th. Jagemann , J. Jochum , T. Lachenmaier , J. -C. Lanfranchi , W. Potzel , W. Rau , M. Stark , S. Waller

Many low-threshold experiments observe sharply rising event rates of yet unknown origins below a few hundred eV, and larger than expected from known backgrounds. Due to the significant impact of this excess on the dark matter or neutrino…

Instrumentation and Methods for Astrophysics · Physics 2022-09-07 P. Adari , A. Aguilar-Arevalo , D. Amidei , G. Angloher , E. Armengaud , C. Augier , L. Balogh , S. Banik , D. Baxter , C. Beaufort , G. Beaulieu , V. Belov , Y. Ben Gal , G. Benato , A. Benoît , A. Bento , L. Bergé , A. Bertolini , R. Bhattacharyya , J. Billard , I. M. Bloch , A. Botti , R. Breier , G. Bres , J-. L. Bret , A. Broniatowski , A. Brossard , C. Bucci , R. Bunker , M. Cababie , M. Calvo , P. Camus , G. Cancelo , L. Canonica , F. Cappella , L. Cardani , J. -F. Caron , N. Casali , G. del Castello , A. Cazes , R. Cerulli , B. A. Cervantes Vergara , D. Chaize , M. Chapellier , L. Chaplinsky , F. Charlieux , M. Chaudhuri , A. E. Chavarria , G. Chemin , R. Chen , H. Chen , F. Chierchie , I. Colantoni , J. Colas , J. Cooley , J. -M. Coquillat , E. C. Corcoran , S. Crawford , M. Crisler , A. Cruciani , P. Cushman , A. D'Addabbo , J. C. D'Olivo , A. Dastgheibi-Fard , M. De Jésus , Y. Deng , J. B. Dent , E. L. Depaoli , K. Dering , S. Dharani , S. Di Lorenzo , A. Drlica-Wagner , L. Dumoulin , D. Durnford , B. Dutta , L. Einfalt , A. Erb , A. Erhart , R. Essig , J. Estrada , E. Etzion , O. Exshaw , F. Favela-Perez , F. v. Feilitzsch , G. Fernandez Moroni , N. Ferreiro Iachellini , S. Ferriol , S. Fichtinger , E. Figueroa-Feliciano , J. -B. Filippini , D. Filosofov , J. A. Formaggio , M. Friedl , S. Fuard , D. Fuchs , A. Fuss , R. Gaïor , A. Garai , C. Garrah , J. Gascon , G. Gerbier , M. Ghaith , V. M. Ghete , D. Gift , I. Giomataris , G. Giroux , A. Giuliani , P. Gorel , P. Gorla , C. Goupy , J. Goupy , C. Goy , M. Gros , P. Gros , Y. Guardincerri , C. Guerin , V. Guidi , O. Guillaudin , S. Gupta , E. Guy , P. Harrington , D. Hauff , S. T. Heine , S. A. Hertel , S. E. Holland , Z. Hong , E. W. Hoppe , T. W. Hossbach , J. -C. Ianigro , V. Iyer , A. Jastram , M. Ješkovský , Y. Jin , J. Jochum , J. P. Johnston , A. Juillard , D. Karaivanov , V. Kashyap , I. Katsioulas , S. Kazarcev , M. Kaznacheeva , F. Kelly , B. Kilminster , A. Kinast , L. Klinkenberg , H. Kluck , P. Knights , Y. Korn , H. Kraus , B. von Krosigk , A. Kubik , N. A. Kurinsky , J. Lamblin , A. Langenkämper , S. Langrock , T. Lasserre , H. Lattaud , P. Lautridou , I. Lawson , S. J. Lee , M. Lee , A. Letessier-Selvon , D. Lhuillier , M. Li , Y. -T. Lin , A. Lubashevskiy , R. Mahapatra , S. Maludze , M. Mancuso , I. Manthos , L. Marini , S. Marnieros , R. D. Martin , A. Matalon , J. Matthews , B. Mauri , D. W. Mayer , A. Mazzolari , E. Mazzucato , H. Meyer zu Theenhausen , E. Michielin , J. Minet , N. Mirabolfathi , K. v. Mirbach , D. Misiak , P. Mitra , J-. L. Mocellin , B. Mohanty , V. Mokina , J. -P. Mols , A. Monfardini , F. Mounier , S. Munagavalasa , J. -F. Muraz , X. -F. Navick , T. Neep , H. Neog , H. Neyrial , K. Nikolopoulos , A. Nilima , C. Nones , V. Novati , P. O'Brien , L. Oberauer , E. Olivieri , M. Olmi , A. Onillon , C. Oriol , A. Orly , J. L. Orrell , T. Ortmann , C. T. Overman , C. Pagliarone , V. Palušová , P. Pari , P. K. Patel , L. Pattavina , F. Petricca , A. Piers , H. D. Pinckney , M. -C. Piro , M. Platt , D. Poda , D. Ponomarev , W. Potzel , P. Povinec , F. Pröbst , P. Privitera , F. Pucci , K. Ramanathan , J. -S. Real , T. Redon , F. Reindl , R. Ren , A. Robert , J. Da Rocha , D. Rodrigues , R. Rogly , J. Rothe , N. Rowe , S. Rozov , I. Rozova , T. Saab , N. Saffold , T. Salagnac , J. Sander , V. Sanglard , D. Santos , Y. Sarkis , V. Savu , G. Savvidis , I. Savvidis , S. Schönert , K. Schäffner , N. Schermer , J. Schieck , B. Schmidt , D. Schmiedmayer , C. Schwertner , L. Scola , M. Settimo , Ye. Shevchik , V. Sibille , I. Sidelnik , A. Singal , R. Smida , M. Sofo Haro , T. Soldner , J. Stachurska , M. Stahlberg , L. Stefanazzi , L. Stodolsky , C. Strandhagen , R. Strauss , A. Stutz , R. Thomas , A. Thompson , J. Tiffenberg , C. Tomei , M. Traina , S. Uemura , I. Usherov , L. Vagneron , W. Van De Pontseele , F. A. Vazquez de Sola Fernandez , M. Vidal , M. Vignati , A. L. Virto , M. Vivier , T. Volansky , V. Wagner , F. Wagner , J. Walker , R. Ward , S. L. Watkins , A. Wex , M. Willers , M. J. Wilson , L. Winslow , E. Yakushev , T. -T. Yu , M. Zampaolo , A. Zaytsev , V. Zema , D. Zinatulina , A. Zolotarova

CRESST is one of the most prominent direct detection experiments for dark matter particles with sub-GeV/c$^2$ mass. One of the advantages of the CRESST experiment is the possibility to include a large variety of nuclides in the target…

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 describe the TREX-DM experiment, a low background…

Instrumentation and Detectors · Physics 2016-06-22 F. J. Iguaz , J. G. Garza , F. Aznar , J. F. Castel , S. Cebrian , T. Dafni , J. A. Garcia , I. G. Irastorza , A. Lagraba , G. Luzon , A. Peiro

We review the status and future of direct searches for light dark matter. We start by answering the question: `Whatever happened to the light dark matter anomalies?' i.e. the fate of the potential dark matter signals observed by the CoGeNT,…

High Energy Physics - Phenomenology · Physics 2015-06-15 Jonathan H. Davis

Driven by the null results in the searches for dark matter, the field of direct dark matter detection is constantly evolving to push new frontiers. Ultimately, a vast parameter space for dark matter masses below a few GeV is yet to be…

High Energy Physics - Experiment · Physics 2025-12-18 Melih Solmaz

The majority of the matter in the universe is still unidentified and under investigation by both direct and indirect means. Many experiments searching for the recoil of dark-matter particles off target nuclei in underground laboratories…

High Energy Physics - Phenomenology · Physics 2015-10-28 Michael Klasen , Martin Pohl , Günter Sigl

Dark matter is poorly constrained by direct detection experiments at masses below 1 MeV. This is an important target for the next generation of experiments, and several methods have been proposed to probe this mass range. One class of such…

High Energy Physics - Phenomenology · Physics 2020-07-31 Benjamin V. Lehmann , Stefano Profumo

A direct dark matter search is performed using fully-depleted high-resistivity CCD detectors . Due to their low electronic readout noise (RMS ~ 7 eV) these devices operate with a very low detection threshold of 40 eV, making the search for…

Instrumentation and Methods for Astrophysics · Physics 2015-05-28 J. Barreto , H. Cease , H. T. Diehl , J. Estrada , B. Flaugher , N. Harrison , J. Jones , B. Kilminster , J. Molina , J. Smith , T. Schwarz , A. Sonnenschein