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We discuss the use of atom interferometry as a tool to search for Dark Matter (DM) composed of ultra-light scalar fields. Previous work on ultra-light DM detection using accelerometers has considered the possibility of equivalence principle…

Atomic Physics · Physics 2016-12-28 Andrew A. Geraci , Andrei Derevianko

The readout electronics upgrade for the ATLAS Liquid Argon Calorimeters at the CERN Large Hadron Collider requires a radiation-hard ADC. The design of a radiation-hard dual-channel 12-bit 40 MS/s pipeline ADC for this use is presented. The…

Instrumentation and Detectors · Physics 2017-06-07 Jayanth Kuppambatti , Jaroslav Ban , Timothy Andeen , Rex Brown , Ryne Carbone , Peter Kinget , Gustaaf Brooilmans , William Sippach

A new method of searching for dark matter in the form of weakly interacting massive particles (WIMP) has been developed with the direct detection of the low energy nuclear recoils observed in a massive target (ultimately many tons) of ultra…

Noble element detectors using argon or xenon as the detection medium are widely used in the searches for rare neutrino and dark matter interactions. Xenon doping in liquid argon can preserve attractive properties of an argon target while…

The Gamma-Ray and AntiMatter Survey (GRAMS) project is a proposed next-generation balloon/satellite mission targeting both MeV gamma-ray observations and antimatter-based dark matter searches. A cost-effective, large-scale Liquid Argon Time…

The Light Dark Matter eXperiment (LDMX) is a proposed fixed-target missing momentum search for sub-GeV thermal relic dark matter. LDMX aims to probe thermal dark matter targets with 1016 electrons on target. Such an approach requires a…

The Scintillating Bubble Chamber (SBC) Collaboration is designing a new generation of low background, noble liquid bubble chamber experiments with sub-keV nuclear recoil threshold. These experiments combine the electronic recoil blindness…

This paper reports the first results of a direct dark matter search with the DEAP-3600 single-phase liquid argon (LAr) detector. The experiment was performed 2 km underground at SNOLAB (Sudbury, Canada) utilizing a large target mass, with…

This paper will discuss a new method of signal read-out from photon detectors in ultra-large, underground liquid argon time projection chambers. In this design, the signal from the light collection system is coupled via capacitive plates to…

Instrumentation and Detectors · Physics 2016-04-13 Z. Moss , M. Toups , L. Bugel , G. H. Collin , J. M. Conrad

The Aria cryogenic distillation plant, located in Sardinia, Italy, is a key component of the DarkSide-20k experimental program for WIMP dark matter searches at the INFN Laboratori Nazionali del Gran Sasso, Italy. Aria is designed to purify…

Instrumentation and Detectors · Physics 2024-05-17 20k Collaboration

This paper reports on laser-induced multiphoton ionization at 266 nm of liquid argon in a time projection chamber (LAr TPC) detector. The electron signal produced by the laser beam is a formidable tool for the calibration and monitoring of…

Instrumentation and Detectors · Physics 2010-12-21 I. Badhrees , A. Ereditato , I. Kreslo , M. Messina , U. Moser , B. Rossi , M. S. Weber , M. Zeller , C. Altucci , S. Amoruso , R. Bruzzese , R. Velotta

This paper describes the concept and the beginning of an experimental investigation of whether it is possible to directly detect dark energy density on earth using atom interferometry. The concept is to null out the gravitational force…

Instrumentation and Methods for Astrophysics · Physics 2022-03-02 Martin L. Perl

A new scheme for detecting wave-like dark matter (DM) using Rydberg atoms is proposed. Recent advances in trapping and manipulating Rydberg atoms make it possible to use Rydberg atoms trapped in optical tweezer arrays for DM detection. We…

High Energy Physics - Phenomenology · Physics 2026-05-15 So Chigusa , Taiyo Kasamaki , Toshi Kusano , Takeo Moroi , Kazunori Nakayama , Naoya Ozawa , Yoshiro Takahashi , Atsuhiro Umemoto , Amar Vutha

This Letter details a measurement of the ionization yield ($Q_y$) of 6.7 keV $^{40}Ar$ atoms stopping in a liquid argon detector. The $Q_y$ of 3.6-6.3 detected $e^{-}/\mbox{keV}$, for applied electric fields in the range 240--2130 V/cm, is…

Coherent scattering is a flavor-blind, high-rate, as yet undetected neutrino interaction predicted by the Standard Model. We propose to use a compact (kg-scale), two-phase (liquid-gas) argon ionization detector to measure coherent neutrino…

Nuclear Experiment · Physics 2009-11-10 Chris Hagmann , Adam Bernstein

The XENON1T experiment at the Laboratori Nazionali del Gran Sasso (LNGS) is the first WIMP dark matter detector operating with a liquid xenon target mass above the ton-scale. Out of its 3.2t liquid xenon inventory, 2.0t constitute the…

Instrumentation and Methods for Astrophysics · Physics 2018-06-13 XENON Collaboration , E. Aprile , J. Aalbers , F. Agostini , M. Alfonsi , F. D. Amaro , M. Anthony , B. Antunes , F. Arneodo , M. Balata , P. Barrow , L. Baudis , B. Bauermeister , M. L. Benabderrahmane , T. Berger , A. Breskin , P. A. Breur , A. Brown , E. Brown , S. Bruenner , G. Bruno , R. Budnik , L. Bütikofer , J. Calvén , J. M. R. Cardoso , M. Cervantes , A. Chiarini , D. Cichon , D. Coderre , A. P. Colijn , J. Conrad , R. Corrieri , J. P. Cussonneau , M. P. Decowski , P. de Perio , P. Di Gangi , A. Di Giovanni , S. Diglio , J. -M. Disdier , M. Doets , E. Duchovni , G. Eurin , J. Fei , A. D. Ferella , A. Fieguth , D. Florin , D. Front , W. Fulgione , A. Gallo Rosso , M. Galloway , F. Gao , M. Garbini , C. Geis , K. -L. Giboni , L. W. Goetzke , L. Grandi , Z. Greene , C. Grignon , C. Hasterok , E. Hogenbirk , C. Huhmann , R. Itay , A. James , B. Kaminsky , S. Kazama , G. Kessler , A. Kish , H. Landsman , R. F. Lang , D. Lellouch , L. Levinson , Q. Lin , S. Lindemann , M. Lindner , F. Lombardi , J. A. M. Lopes , R. Maier , A. Manfredini , I. Maris , T. Marrodán Undagoitia , J. Masbou , F. V. Massoli , D. Masson , D. Mayani , M. Messina , K. Micheneau , A. Molinario , K. Morå , M. Murra , J. Naganoma , K. Ni , U. Oberlack , D. Orlandi , R. Othegraven , P. Pakarha , S. Parlati , B. Pelssers , R. Persiani , F. Piastra , J. Pienaar , V. Pizzella , M. -C. Piro , G. Plante , N. Priel , D. Ramírez García , L. Rauch , S. Reichard , C. Reuter , A. Rizzo , S. Rosendahl , N. Rupp , J. M. F. dos Santos , R. Saldahna , G. Sartorelli , M. Scheibelhut , S. Schindler , J. Schreiner , M. Schumann , L. Scotto Lavina , M. Selvi , P. Shagin , E. Shockley , M. Silva , H. Simgen , M. v. Sivers , M. Stern , A. Stein , D. Tatananni , L. Tatananni , D. Thers , A. Tiseni , G. Trinchero , C. Tunnell , N. Upole , M. Vargas , O. Wack , R. Walet , H. Wang , Z. Wang , Y. Wei , C. Weinheimer , C. Wittweg , J. Wulf , J. Ye , Y. Zhang

The LArIAT liquid argon time projection chamber, placed in a tertiary beam of charged particles at the Fermilab Test Beam Facility, has collected large samples of pions, muons, electrons, protons, and kaons in the momentum range 300-1400…

Instrumentation and Detectors · Physics 2020-06-17 LArIAT Collaboration , R. Acciarri , C. J. Adams , J. Asaadi , M. Backfish , W. Badgett , B. Baller , O. Benevides Rodrigues , F. d. M. Blaszczyk , R. Bouabid , C. Bromberg , R. Carey , R. Castillo Fernandez , F. Cavanna , J. I. Cevallos Aleman , A. Chatterjee , P. Dedin Neto , M. V. Dos Santos , S. Dytman , D. Edmunds , M. Elkins , C. O. Escobar , J. Esquivel , J. Evans , A. Falcone , A. Farbin , W. Flanagan , B. Fleming , W. Foreman , D. Garcia-Gamez , D. Gastler , T. Ghosh , R. A. Gomes , E. Gramellini , R. Gran , P. Guzowski , A. Habig , A. Hahn , P. Hamilton , C. Hill , J. Ho , A. Holin , J. Hugon , E. Iwai , D. Jensen , R. A. Johnson , H. Jostlein , H. Kawai , E. Kearns , E. Kemp , M. Kirby , T. Kobilarcik , M. Kordosky , P. Kryczynski , K. Lang , R. Linehan , S. Lockwitz , X. Luo , A. A. B. Machado , A. Marchionni , T. Maruyama , L. Mendes Santos , W. Metcalf , C. A. Moura , R. Nichol , I. Nutini , A. Olivier , O. Palamara , J. Paley , I. Parmaksiz , B. Passarelli Gelli , L. Paulucci , D. Phan , G. Pulliam , J. L. Raaf , B. Rebel , M. Reggiani Guzzo , M. Ross-Lonergan , D. Schmitz , D. Sessumes , S. Shahsavarani , D. Shooltz , E. Segreto , D. Smith , M. Soares Nunes , M. Soderberg , B. Soubasis , F. Spagliardi , J. M. St. John , M. Stancari , D. Stefan , M. Stephens , R. Sulej , A. Szelc , M. Tabata , D. Totani , M. Tzanov , G. Valdiviesso , D. Walker , H. Wenzel , Z. Williams , T. Yang , J. Yu , G. Zeller , S. Zhang , J. Zhu

In liquid argon TPCs for dark matter search and neutrino detection experiments, primary scintillation light is used as a prompt signal of particle scattering, being intensively produced in the vacuum ultraviolet (VUV) due to excimer…

Instrumentation and Detectors · Physics 2022-09-09 A. Bondar , E. Borisova , A. Buzulutskov , E. Frolov , V. Nosov , V. Oleynikov , A. Sokolov