English
Related papers

Related papers: Backgrounds in the DEAP-3600 Dark Matter Experimen…

200 papers

We report a first search for weakly interacting massive particles (WIMPs) using the background rejection capabilities of SuperCDMS. An exposure of 577 kg-days was analyzed for WIMPs with mass < 30 GeV/c2, with the signal region blinded.…

The NEWS-G direct dark matter search experiment uses spherical proportional counters (SPC) with light noble gases to explore low WIMP masses. The first results obtained with an SPC prototype operated with Ne gas at the Laboratoire…

Instrumentation and Detectors · Physics 2022-03-02 Daniel Durnford , Marie-Cécile Piro

The Search for Hidden Particles (SHiP) Collaboration has proposed a general-purpose experimental facility operating in beam-dump mode at the CERN SPS accelerator to search for light, feebly interacting particles. The SHiP experiment…

Instrumentation and Detectors · Physics 2022-05-23 SHIP Collaboration

The DAMIC (Dark Matter in CCDs) experiment at the SNOLAB underground laboratory uses fully depleted, high resistivity CCDs to search for dark matter particles with masses below 10 GeV/c$^2$. An upgrade of the detector using an array of…

Instrumentation and Methods for Astrophysics · Physics 2018-07-01 Mariangela Settimo

Experiments that use liquid noble gasses as target materials, such as argon and xenon, play a significant role in direct detection searches for WIMP(-like) dark matter. As these experiments grow in size, they will soon encounter a new…

High Energy Physics - Phenomenology · Physics 2023-05-05 Andrea Gaspert , Pietro Giampa , David E. Morrissey

We present limits on spin-independent inelastic weakly interacting massive particles (WIMP)-nucleus scattering using the 737.1 kg$\cdot$day dataset from the CDEX-1B experiment. Expected nuclear recoil spectra for various inelastic WIMP…

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

The WIMP proposed here yields the observed abundance of dark matter, and is consistent with the current limits from direct detection, indirect detection, and collider experiments, if its mass is $\sim 72$ GeV/$c^2$. It is also consistent…

High Energy Physics - Phenomenology · Physics 2021-08-02 Reagan Thornberry , Maxwell Throm , Gabriel Frohaug , John Killough , Dylan Blend , Michael Erickson , Brian Sun , Brett Bays , Roland E. Allen

We propose a new beam-dump experiment, SHADOWS, to search for a large variety of feebly-interacting particles possibly produced in the interactions of a 400 GeV proton beam with a high-Z material dump. SHADOWS will use the 400 GeV primary…

In experiments for direct dark matter searches, neutrinos coherently scattering off nuclei can produce similar events as Weakly Interacting Massive Particles (WIMPs). To reach sensitivities better than about 10^-10 pb for the elastic WIMP…

The SABRE (Sodium iodide with Active Background REjection) experiment aims to detect an annual rate modulation from dark matter interactions in ultra-high purity NaI(Tl) crystals which will provide a model independent test of the signal…

High Energy Physics - Experiment · Physics 2025-11-21 L. J. Milligan

An energy threshold of (220$\pm$10) eV was achieved at an efficiency of 50% with a four-channel ultra-low-energy germanium detector each with an active mass of 5 g\cite{wimppaper}. This provides a unique probe to WIMP dark matter with mass…

Astrophysics · Physics 2019-08-13 Shin-Ted Lin , H. T. Wong

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 2015-09-08 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

The Cryogenic Dark Matter Search experiment uses low-temperature solid-state detectors to seek Weakly Interacting Massive Particles (WIMPs) and has the world's best exclusion limit on the spin-independent WIMP-nucleon cross section. The…

High Energy Physics - Experiment · Physics 2019-08-13 Oleg Kamaev

We present direct detection constraints on the absorption of hidden-photon dark matter with particle masses in the range 1.2-30 eV$c^{-2}$ with the DAMIC experiment at SNOLAB. Under the assumption that the local dark matter is entirely…

In this paper, we investigate the possibility of testing the weakly interacting massive particle (WIMP) dark matter (DM) models by applying the simplest phenomenological model which introduces an interaction term between dark energy (DE)…

Cosmology and Nongalactic Astrophysics · Physics 2021-09-15 Wei Cheng , Yuan He , Jin-Wang Diao , Yu Pan , Jun Zeng , Jia-Wei Zhang

Measurements with a bare p-type high purity germanium diode (HPGe) submerged in a 19 kg liquid argon (LAr) scintillation detector at MPIK Heidelberg are reported. The liquid argon--germanium system (LArGe) is operated as a 4$\pi$…

Instrumentation and Detectors · Physics 2008-11-26 M. Di Marco , P. Peiffer , S. Schönert

An energy threshold of (220+-10) eV was achieved at an efficiency of 50% with a four-channel ultra-low-energy germanium detector each with an active mass of 5 g. This provides a unique probe to WIMP dark matter with mass below 10 GeV. With…

High Energy Physics - Experiment · Physics 2009-03-24 TEXONO Collaboration , S. T. Lin

New data are reported from the operation of the PICO-60 dark matter detector, a bubble chamber filled with 36.8 kg of CF$_3$I and located in the SNOLAB underground laboratory. PICO-60 is the largest bubble chamber to search for dark matter…

Unveiling the nature of cosmic dark matter (DM) is an urgent issue in cosmology. Here we make use of a strategy based on the search for the imprints left on the cosmic microwave background temperature and polarization spectra by the energy…

Cosmology and Nongalactic Astrophysics · Physics 2015-06-11 Carmelo Evoli , Stefania Pandolfi , Andrea Ferrara