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The XENON100 experiment, located at the Laboratori Nazionali del Gran Sasso (LNGS), aims to directly detect dark matter in the form of Weakly Interacting Massive Particles (WIMPs) via their elastic scattering off xenon nuclei. We present a…

Direction sensitivity could provide robust evidence for the direct detection of weakly interacting massive particles constituting dark matter. However, the sensitivity of this method remains low due to the radioactive backgrounds. The…

Diverse searches for direct dark matter (DM) in effective electromagnetic and leptophilic interactions resulting from new physics, as well as Weakly Interacting Massive Particles (WIMPs) with unconventional electronic recoils, are…

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…

A Resistive Plate Chamber using Diamond-Like Carbon electrodes (DLC-RPC) has been developed as a background tagging detector in the MEG$~$II experiment. The DLC-RPC is planned to be installed in a high-intensity and low-momentum muon beam.…

Instrumentation and Detectors · Physics 2025-06-13 Masato Takahashi , Sei Ban , Weiyuan Li , Atsuhiko Ochi , Wataru Ootani , Atsushi Oya , Hiromu Suzuki , Kensuke Yamamoto

The Weakly Interacting Massive Particles(WIMPs) have long been the favored CDM candidate in the standard $\Lambda$CDM model. However, owing to great improvement in the experimental sensitivity in the past decade, some parameter space of the…

Cosmology and Nongalactic Astrophysics · Physics 2023-11-15 Abineet Parichha , Shiv Sethi

This report presents an overview of the unconventional use of charge-coupled devices (CCDs) to search for Dark Matter (DM). The DArk Matter In CCDs (DAMIC Experiment) employs the bulk silicon of thick, fully-depleted CCDs as a target for…

Instrumentation and Detectors · Physics 2020-01-14 N. Castello-Mor , DAMIC-M Collaboration

Next-generation dark matter (DM) detectors searching for weakly interacting massive particles (WIMPs) will be sensitive to coherent scattering from solar neutrinos, demanding an efficient background-signal discrimination tool. Directional…

Now that conventional weakly interacting massive particle (WIMP) dark matter searches are approaching the neutrino floor, there has been a resurgence of interest in detectors with sensitivity to nuclear recoil directions. A large-scale…

Recent computational results suggest that directional dark matter detectors have potential to probe for WIMP dark matter particles below the neutrino floor. The DRIFT-IId detector used in this work is a leading directional WIMP search time…

The CDMS II experiment uses Z-dependent Ionization Phonon (ZIP) detectors made of Germanium and Silicon to identify nuclear recoils from Weakly Interacting Massive Particles (WIMPs) with near complete event-by-event rejection of various…

Astrophysics · Physics 2007-05-23 Samuel Leclercq

The Weakly Interacting Massive Particles (WIMPs) are among the main candidates for the relic dark matter (DM). The idea of the direct DM detection relies on elastic in-dependent (SD) and spin-independent (SI) interaction of WIMPs with…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. A. Bednyakov , F. Simkovic , I. V. Titkova

We report on the results of a search for a Weakly Interacting Massive Particle (WIMP) signal in low-energy data of the Cryogenic Dark Matter Search (CDMS~II) experiment using a maximum likelihood analysis. A background model is constructed…

Low-pressure gaseous TPCs are well suited detectors to correlate the directions of nuclear recoils to the galactic Dark Matter (DM) halo. Indeed, in addition to providing a measure of the energy deposition due to the elastic scattering of a…

Instrumentation and Methods for Astrophysics · Physics 2017-12-06 C. Couturier , Q. Riffard , N. Sauzet , O. Guillaudin , F. Naraghi , D. Santos

The DAMIC (Dark Matter in CCDs) experiment searches for the interactions of dark matter particles with the nuclei and the electrons in the silicon bulk of thick fully depleted charge-coupled devices (CCDs). Because of the low noise and low…

High Energy Physics - Experiment · Physics 2020-04-02 Mariangela Settimo

Weakly Interacting Massive Particles (WIMPs) are one of the leading candidates for Dark Matter. Currently, the most promising method to detect WIMPs is the direct detection of the recoil energy deposited in a low-background laboratory…

Astrophysics · Physics 2011-11-10 Chung-Lin Shan

Building on the successful experience in operating the DarkSide-50 detector, the DarkSide Collaboration is going to construct DarkSide-20k, a direct WIMP search detector using a two-phase Liquid Argon Time Projection Chamber (LArTPC) with…

Instrumentation and Detectors · Physics 2018-08-09 C. E. Aalseth , F. Acerbi , P. Agnes , I. F. M. Albuquerque , T. Alexander , A. Alici , A. K. Alton , P. Antonioli , S. Arcelli , R. Ardito , I. J. Arnquist , D. M. Asner , M. Ave , H. O. Back , A. I. Barrado Olmedo , G. Batignani , E. Bertoldo , S. Bettarini , M. G. Bisogni , V. Bocci , A. Bondar , G. Bonfini , W. Bonivento , M. Bossa , B. Bottino , M. Boulay , R. Bunker , S. Bussino , A. Buzulutskov , M. Cadeddu , M. Cadoni , A. Caminata , N. Canci , A. Candela , C. Cantini , M. Caravati , M. Cariello , M. Carlini , M. Carpinelli , A. Castellani , S. Catalanotti , V. Cataudella , P. Cavalcante , S. Cavuoti , R. Cereseto , A. Chepurnov , C. Cicalò , L. Cifarelli , M. Citterio , A. G. Cocco , M. Colocci , S. Corgiolu , G. Covone , P. Crivelli , I. D'Antone , M. D'Incecco , D. D'Urso , M. D. Da Rocha Rolo , M. Daniel , S. Davini , A. de Candia , S. De Cecco , M. De Deo , G. De Filippis , G. De Guido , G. De Rosa , G. Dellacasa , M. Della Valle , P. Demontis , A. Derbin , A. Devoto , F. Di Eusanio , G. Di Pietro , C. Dionisi , A. Dolgov , I. Dormia , S. Dussoni , A. Empl , M. Fernandez Diaz , A. Ferri , C. Filip , G. Fiorillo , K. Fomenko , D. Franco , G. E. Froudakis , F. Gabriele , A. Gabrieli , C. Galbiati , P. Garcia Abia , A. Gendotti , A. Ghisi , S. Giagu , P. Giampa , G. Gibertoni , C. Giganti , M. A. Giorgi , G. K. Giovanetti , M. L. Gligan , A. Gola , O. Gorchakov , A. M. Goretti , F. Granato , M. Grassi , J. W. Grate , G. Y. Grigoriev , M. Gromov , M. Guan , M. B. B. Guerra , M. Guerzoni , M. Gulino , R. K. Haaland , A. Hallin , B. Harrop , E. W. Hoppe , S. Horikawa , B. Hosseini , D. Hughes , P. Humble , E. V. Hungerford , An. Ianni , C. Jillings , T. N. Johnson , K. Keeter , C. L. Kendziora , S. Kim , G. Koh , D. Korablev , G. Korga , A. Kubankin , M. Kuss , M. Kuźniak , B. Lehnert , X. Li , M. Lissia , G. U. Lodi , B. Loer , G. Longo , P. Loverre , R. Lussana , L. Luzzi , Y. Ma , A. A. Machado , I. N. Machulin , A. Mandarano , L. Mapelli , M. Marcante , A. Margotti , S. M. Mari , M. Mariani , J. Maricic , C. J. Martoff , M. Mascia , M. Mayer , A. B. McDonald , A. Messina , P. D. Meyers , R. Milincic , A. Moggi , S. Moioli , J. Monroe , A. Monte , M. Morrocchi , B. J. Mount , W. Mu , V. N. Muratova , S. Murphy , P. Musico , R. Nania , A. Navrer Agasson , I. Nikulin , V. Nosov , A. O. Nozdrina , N. N. Nurakhov , A. Oleinik , V. Oleynikov , M. Orsini , F. Ortica , L. Pagani , M. Pallavicini , S. Palmas , L. Pandola , E. Pantic , E. Paoloni , G. Paternoster , V. Pavletcov , F. Pazzona , S. Peeters , K. Pelczar , L. A. Pellegrini , N. Pelliccia , F. Perotti , R. Perruzza , V. Pesudo Fortes , C. Piemonte , F. Pilo , A. Pocar , T. Pollmann , D. Portaluppi , D. A. Pugachev , H. Qian , B. Radics , F. Raffaelli , F. Ragusa , M. Razeti , A. Razeto , V. Regazzoni , C. Regenfus , B. Reinhold , A. L. Renshaw , M. Rescigno , F. Retière , Q. Riffard , A. Rivetti , S. Rizzardini , A. Romani , L. Romero , B. Rossi , N. Rossi , A. Rubbia , D. Sablone , P. Salatino , O. Samoylov , E. Sánchez García , W. Sands , M. Sant , R. Santorelli , C. Savarese , E. Scapparone , B. Schlitzer , G. Scioli , E. Segreto , A. Seifert , D. A. Semenov , A. Shchagin , L. Shekhtman , E. Shemyakina , A. Sheshukov , M. Simeone , P. N. Singh , P. Skensved , M. D. Skorokhvatov , O. Smirnov , G. Sobrero , A. Sokolov , A. Sotnikov , F. Speziale , R. Stainforth , C. Stanford , G. B. Suffritti , Y. Suvorov , R. Tartaglia , G. Testera , A. Tonazzo , A. Tosi , P. Trinchese , E. V. Unzhakov , A. Vacca , E. Vázquez-Jáuregui , M. Verducci , T. Viant , F. Villa , A. Vishneva , B. Vogelaar , M. Wada , J. Wahl , J. Walding , S. Walker , H. Wang , Y. Wang , A. W. Watson , S. Westerdale , R. Williams , M. M. Wojcik , S. Wu , X. Xiang , X. Xiao , C. Yang , Z. Ye , A. Yllera de Llano , F. Zappa , G. Zappalà , C. Zhu , A. Zichichi , M. Zullo , A. Zullo

If the dark matter particle has spin 0, only two types of WIMP-nucleon interaction can arise from the non-relativistic reduction of renormalisable single-mediator models for dark matter-quark interactions. Based on this crucial observation,…

High Energy Physics - Phenomenology · Physics 2018-01-17 Riccardo Catena , Jan Conrad , Christian Döring , Alfredo Davide Ferella , Martin B. Krauss

The Cryogenic Dark Matter search experiment (CDMS) employs low-temperature Ge and Si detectors to detect WIMPs via their elastic scattering of target nuclei. The last analysis with an germanium exposure of 397.8 kg-days resulted in zero…

Instrumentation and Methods for Astrophysics · Physics 2019-08-13 T. Bruch

Measurement of the direction of the elastic nuclear recoil track and ionization charge distribution along it, gives unique possibility for unambiguous detection of the dark matter WIMP particle. Within current radiation detection…

Instrumentation and Detectors · Physics 2017-08-23 N. J. C. Spooner , P. Majewski
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