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200 papers

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

A small liquid argon Time Projection Chamber (LAr TPC) was operated for the first time in a magnetic field of 0.55 Tesla. The imaging properties of the detector were not affected by the magnetic field. In a test run with cosmic rays a…

Instrumentation and Detectors · Physics 2008-11-26 A. Badertscher , M. Laffranchi , A. Meregaglia , A. Mueller , A. Rubbia

The three-dimensional (3-D) reconstruction of nuclear recoils is of interest for directional detection of fast neutrons and for direction-sensitive searches for weakly interacting massive particles(WIMPs), which may constitute the Dark…

Instrumentation and Detectors · Physics 2015-12-09 S. E. Vahsen , M. T. Hedges , I. Jaegle , S. J. Ross , I. S. Seong , T. N. Thorpe , J. Yamaoka , J. A. Kadyk , M. Garcia-Sciveres

The existence of dark matter as evidenced by numerous indirect observations is one of the most important indications that there must be physics beyond the Standard Model of particle physics. This article reviews the concepts of direct…

Cosmology and Nongalactic Astrophysics · Physics 2019-11-26 Marc Schumann

To increase the light yield of a liquid Ar (LAr) detector, we optimized the evaporation technique of tetraphenyl butadiene (TPB) on the detector surface and tested the operability of a silicon photomultiplier (SiPM), namely, the multi-pixel…

Instrumentation and Detectors · Physics 2022-05-04 Kazutaka Aoyama , Masashi Tanaka , Masato Kimura , Kohei Yorita

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

This paper describes the results of a study on the general lines, main construction criteria, crucial points, parameters and required preliminary R&D activities for the construction of a LAr (liquid argon) imaging detector with active mass…

Astrophysics · Physics 2007-05-23 D. B. Cline , F. Sergiampietri

The DEAP-3600 experiment is located 2 km underground at SNOLAB, in Sudbury, Ontario. It is a single-phase detector that searches for dark matter particle interactions within a 1000-kg fiducial mass target of liquid argon. A first generation…

The GammaTPC is an MeV-scale single-phase liquid argon time-projection-chamber gamma-ray telescope concept with a novel dual-scale pixel-based charge-readout system. It promises to enable a significant improvement in sensitivity to…

Instrumentation and Methods for Astrophysics · Physics 2023-01-25 M. Buuck , A. Mishra , E. Charles , N. Di Lalla , O. Hitchcock , M. E. Monzani , N. Omodei , T. Shutt

The XENON1T experiment uses a time projection chamber (TPC) with liquid Xenon to search for Weakly Interacting Massive Particles (WIMPs), a proposed Dark Matter particle, via direct detection. As this experiment relies on capturing rare…

High Energy Physics - Phenomenology · Physics 2020-08-03 Charanjit K. Khosa , Lucy Mars , Joel Richards , Veronica Sanz

The DarkSide-50 experiment at the Laboratori Nazionali del Gran Sasso is a search for dark matter using a dual phase time projection chamber with 50 kg of low radioactivity argon as target. Light signals from interactions in the argon are…

Instrumentation and Detectors · Physics 2018-01-17 DarkSide Collaboration , P. Agnes , I. F. M. Albuquerque , T. Alexander , A. K. Alton , K. Arisaka , D. M. Asner , M. Ave , H. O. Back , B. Baldin , K. Biery , V. Bocci , G. Bonfini , W. Bonivento , M. Bossa , B. Bottino , A. Brigatti , J. Brodsky , F. Budano , S. Bussino , M. Cadeddu , M. Cadoni , F. Calaprice , N. Canci , A. Candela , H. Cao , M. Caravati , M. Cariello , M. Carlini , S. Catalanotti , V. Cataudella , P. Cavalcante , A. Chepurnov , C. Cicaló , A. G. Cocco , G. Covone , L. Crippa , D. D'Angelo , M. D'Incecco , S. Davini , A. deCandia , S. DeCecco , M. DeDeo , G. DeFilippis , G. DeRosa , M. DeVincenzi , A. Derbin , A. Devoto , F. DiEusanio , C. Dionisi , G. DiPietro , E. Edkins , A. Empl , A. Fan , G. Fiorillo , K. Fomenko , G. Forster , D. Franco , F. Gabriele , C. Galbiat , S. Giagu , C. Giganti , G. K. Giovanetti , A. M. Goretti , F. Granato , L. Grandi , M. Gromov , M. Guan , Y. Guardincerri , B. R. Hackett , K. R. Herner , D. Hughes , P. Humble , E. V. Hungerford , Aldo Ianni , Andrea Ianni , I. James , T. N. Johnson , K. Keeter , C. L. Kendziora , V. Kobychev , G. Koh , D. Korablev , G. Korga , A. Kubankin , X. Li , M. Lissia , B. Loer , P. Lombardi , G. Longo , S. Luitz , Y. Ma , A. Machado , I. N. Machulin , A. Mandarano , S. M. Mari , J. Maricic , L. Marini , C. J. Martoff , P. D. Meyers , T. Miletic , R. Milincic , D. Montanari , A. Monte , M. Montuschi , M. E. Monzani , P. Mosteiro , B. J. Mount , V. N. Muratova , P. Musico , A. NavrerAgasson , A. Nelson , S. Odrowsk , A. Oleinik , M. Orsini , F. Ortica , L. Pagani , M. Pallavicini , E. Pantic , S. Parmeggiano , K. Pelczar , N. Pelliccia , A. Pocar , S. Pordes , D. A. Pugachev , H. Qian , K. Randle , G. Ranucci , M. Razeti , A. Razeto , B. Reinhold , A. L. Renshaw , M. Rescigno , Q. Riffard , A. Romani , B. Rossi , N. Rossi , S. D. Rountree , D. Sablone , P. Saggese , R. Saldanha , W. Sands , S. Sangiorgio , C. Savarese , B. Schlitzer , E. Segreto , D. A. Semenov , E. Shields , P. N. Singh , M. D. Skorokhvatov , O. Smirno , A. Sotnikov , C. Stanford , Y. Suvorov , R. Tartaglia , J. Tatarowicz , G. Testera , A. Tonazzo , P. Trinchese , E. V. Unzhakov , M. Verducci , A. Vishneva , R. B. Vogelaar , M. Wada , S. Walker , H. Wang , Y. Wang , A. W. Watson , S. Westerdale , M. M. Wojcik , X. Xiang , X. Xiao , J. Xu , C. Yang , J. Yoo , S. Zavatarelli , A. Zec , W. Zhong , C. Zhu , G. Zuzel

The status and plans of a research program on the development of ultra-low-energy germanium detectors with sub-keV sensitivities are reported. We survey the scientific goals which include the observation of neutrino-nucleus coherent…

High Energy Physics - Experiment · Physics 2008-11-26 Henry T. Wong

A chamber for direct detection of WIMPs with masses < 10 GeV/c2 and solar axions is developed. The chamber is filled with a gas mixture of H2 +3ppm TMAE (1,5,10 bar), or D2 + 3ppm TMAE. These gas fillings make it possible to suppress an…

Instrumentation and Detectors · Physics 2016-03-21 B. M. Ovchinnikov , V. V. Parusov

Liquid argon time projection chambers (TPC) are widely used in neutrino oscillation and dark matter experiments. Detection of scintillation light in liquid argon TPC's is challenging because of its short wavelength, in the VUV range, and…

We study the sensitivity of multi ton-scale time projection chambers using a liquid xenon target, e.g., the proposed DARWIN instrument, to spin-independent and spin-dependent WIMP-nucleon scattering interactions. Taking into account…

Instrumentation and Detectors · Physics 2015-10-14 Marc Schumann , Laura Baudis , Lukas Bütikofer , Alexander Kish , Marco Selvi

The Liquid Argon Time Projection Chamber (LArTPC) is an advanced neutrino detector technology widely used in recent and upcoming accelerator neutrino experiments. It features a low energy threshold and high spatial resolution that allow for…

Instrumentation and Detectors · Physics 2021-03-24 Haiwang Yu , Mary Bishai , Wenqiang Gu , Meifeng Lin , Xin Qian , Yihui Ren , Andrea Scarpelli , Brett Viren , Hanyu Wei , Hongzhao Yu , Kwang Min Yu , Chao Zhang

DARWIN is a design-study for a next-to-next generation experiment to directly detect WIMP dark matter in a detector based on a liquid xenon/liquid argon two-phase time projection chamber. This article describes the project, its goals and…

Instrumentation and Methods for Astrophysics · Physics 2011-11-29 Marc Schumann

The GAPS experiment is foreseen to carry out a dark matter search by measuring low-energy cosmic-ray antideuterons and antiprotons with a novel detection approach. It will provide a new avenue to access a wide range of different dark matter…

Instrumentation and Methods for Astrophysics · Physics 2015-08-14 P. von Doetinchem , T. Aramaki , S. Boggs , H. Fuke , C. J. Hailey , S. I. Mognet , R. A. Ong , K. Perez , J. Zweerink

There are several proposals and projects today for building LXe Time Projection Chambers (TPCs) for dark matter search. An important element of these TPCs are the photomultipliers operating either inside LXe or in vapors above the liquid.…

Instrumentation and Detectors · Physics 2008-11-26 L. Periale , V. Peskov , C. Iacobaeus , B. Lund-Jensen , P. Picchi , F. Pietropaolo , Rodionov