English
Related papers

Related papers: Data Acquisition and Readout System for the LUX Da…

200 papers

The current status of the QUAX R\&D program is presented. QUAX is a feasibility study for a detection of axion as dark matter based on the coupling to the electrons. The relevant signal is a magnetization change of a magnetic material…

LUX-ZEPLIN (LZ) is a second-generation direct dark matter experiment with spin-independent WIMP-nucleon scattering sensitivity above $1.4 \times 10^{-48}$ cm$^{2}$ for a WIMP mass of 40 GeV/c$^{2}$ and a 1000 d exposure. LZ achieves this…

Instrumentation and Detectors · Physics 2022-03-02 D. S. Akerib , C. W. Akerlof , D. Yu. Akimov , A. Alquahtani , S. K. Alsum , T. J. Anderson , N. Angelides , H. M. Araújo , A. Arbuckle , J. E. Armstrong , M. Arthurs , H. Auyeung , S. Aviles , X. Bai , A. J. Bailey , J. Balajthy , S. Balashov , J. Bang , M. J. Barry , D. Bauer , P. Bauer , A. Baxter , J. Belle , P. Beltrame , J. Bensinger , T. Benson , E. P. Bernard , A. Bernstein , A. Bhatti , A. Biekert , T. P. Biesiadzinski , H. J. Birch , B. Birrittella , K. E. Boast , A. I. Bolozdynya , E. M. Boulton , B. Boxer , R. Bramante , S. Branson , P. Brás , M. Breidenbach , C. A. J. Brew , J. H. Buckley , V. V. Bugaev , R. Bunker , S. Burdin , J. K. Busenitz , R. Cabrita , J. S. Campbell , C. Carels , D. L. Carlsmith , B. Carlson , M. C. Carmona-Benitez , M. Cascella , C. Chan , J. J. Cherwinka , A. A. Chiller , C. Chiller , N. I. Chott , A. Cole , J. Coleman , D. Colling , R. A. Conley , A. Cottle , R. Coughlen , G. Cox , W. W. Craddock , D. Curran , A. Currie , J. E. Cutter , J. P. da Cunhaw , C. E. Dahl , S. Dardin , S. Dasu , J. Davis , T. J. R. Davison , L. de Viveiros , N. Decheine , A. Dobi , J. E. Y. Dobson , E. Druszkiewicz , A. Dushkin , T. K. Edberg , W. R. Edwards , B. N. Edwards , J. Edwards , M. M. Elnimr , W. T. Emmet , S. R. Eriksen , C. H. Faham , A. Fan , S. Fayer , S. Fiorucci , H. Flaecher , I. M. Fogarty Florang , P. Ford , V. B. Francis , E. D. Fraser , F. Froborg , T. Fruth , R. J. Gaitskell , N. J. Gantos , D. Garcia , V. M. Gehman , R. Gelfand , J. Genovesi , R. M. Gerhard , C. Ghag , E. Gibson , M. G. D. Gilchriese , S. Gokhale , B. Gomber , T. G. Gonda , A. Greenall , S. Greenwood , G. Gregerson , M. G. D. van der Grinten , C. B. Gwilliam , C. R. Hall , D. Hamilton , S. Hans , K. Hanzel , T. Harrington , A. Harrison , J. Harrison , C. Hasselkus , S. J. Haselschwardt , D. Hemer , S. A. Hertel , J. Heise , S. Hillbrand , O. Hitchcock , C. Hjemfelt , M. D. Hoff , B. Holbrook , E. Holtom , J. Y-K. Hor , M. Horn , D. Q. Huang , T. W. Hurteau , C. M. Ignarra , M. N. Irving , R. G. Jacobsen , O. Jahangir , S. N. Jeffery , W. Ji , M. Johnson , J. Johnson , P. Johnson , W. G. Jones , A. C. Kaboth , A. Kamaha , K. Kamdin , V. Kasey , K. Kazkaz , J. Keefner , D. Khaitan , M. Khaleeq , A. Khazov , A. V. Khromov , I. Khurana , Y. D. Kim , W. T. Kim , C. D. Kocher , D. Kodroff , A. M. Konovalov , L. Korley , E. V. Korolkova , M. Koyuncu , J. Kras , H. Kraus , S. W. Kravitz , H. J. Krebs , L. Kreczko , B. Krikler , V. A. Kudryavtsev , A. V. Kumpan , S. Kyre , A. R. Lambert , B. Landerud , N. A. Larsen , A. Laundrie , E. A. Leason , H. S. Lee , J. Lee , C. Lee , B. G. Lenardo , D. S. Leonard , R. Leonard , K. T. Lesko , C. Levy , J. Li , Y. Liu , J. Liao , F. -T. Liao , J. Lin , A. Lindote , R. Linehan , W. H. Lippincott , R. Liu , X. Liu , C. Loniewski , M. I. Lopes , E. Lopez-Asamar , B. López Paredes , W. Lorenzon , D. Lucero , S. Luitz , J. M. Lyle , C. Lynch , P. A. Majewski , J. Makkinje , D. C. Malling , A. Manalaysay , L. Manenti , R. L. Mannino , N. Marangou , D. J. Markley , P. MarrLaundrie , T. J. Martin , M. F. Marzioni , C. Maupin , C. T. McConnell , D. N. McKinsey , J. McLaughlin , D. -M. Mei , Y. Meng , E. H. Miller , Z. J. Minaker , E. Mizrachi , J. Mock , D. Molash , A. Monte , M. E. Monzani , J. A. Morad , E. Morrison , B. J. Mount , A. St. J. Murphy , D. Naim , A. Naylor , C. Nedlik , C. Nehrkorn , H. N. Nelson , J. Nesbit , F. Neves , J. A. Nikkel , J. A. Nikoleyczik , A. Nilima , J. O'Dell , H. Oh , F. G. O'Neill , K. O'Sullivan , I. Olcina , M. A. Olevitch , K. C. Oliver-Mallory , L. Oxborough , A. Pagac , D. Pagenkopf , S. Pal , K. J. Palladino , V. M. Palmaccio , J. Palmer , M. Pangilinan , N. Parveen , S. J. Patton , E. K. Pease , B. P. Penning , G. Pereira , C. Pereira , I. B. Peterson , A. Piepke , S. Pierson , S. Powell , R. M. Preece , K. Pushkin , Y. Qie , M. Racine , B. N. Ratcliff , J. Reichenbacher , L. Reichhart , C. A. Rhyne , A. Richards , Q. Riffard , G. R. C. Rischbieter , J. P. Rodrigues , H. J. Rose , R. Rosero , P. Rossiter , R. Rucinski , G. Rutherford , J. S. Saba , L. Sabarots , D. Santone , M. Sarychev , A. B. M. R. Sazzad , R. W. Schnee , M. Schubnell , P. R. Scovell , M. Severson , D. Seymour , S. Shaw , G. W. Shutt , T. A. Shutt , J. J. Silk , C. Silva , K. Skarpaas , W. Skulski , A. R. Smith , R. J. Smith , R. E. Smith , J. So , M. Solmaz , V. N. Solovov , P. Sorensen , V. V. Sosnovtsev , I. Stancu , M. R. Stark , S. Stephenson , N. Stern , A. Stevens , T. M. Stiegler , K. Stifter , R. Studley , T. J. Sumner , K. Sundarnath , P. Sutcliffe , N. Swanson , M. Szydagis , M. Tan , W. C. Taylor , R. Taylor , D. J. Taylor , D. Temples , B. P. Tennyson , P. A. Terman , K. J. Thomas , J. A. Thomson , D. R. Tiedt , M. Timalsina , W. H. To , A. Tomás , T. E. Tope , M. Tripathi , D. R. Tronstad , C. E. Tull , W. Turner , L. Tvrznikova , M. Utes , U. Utku , S. Uvarov , J. Va'vra , A. Vacheret , A. Vaitkus , J. R. Verbus , T. Vietanen , E. Voirin , C. O. Vuosalo , S. Walcott , W. L. Waldron , K. Walker , J. J. Wang , R. Wang , L. Wang , W. Wang , Y. Wang , J. R. Watson , J. Migneault , S. Weatherly , R. C. Webb , W. -Z. Wei , M. While , R. G. White , J. T. White , D. T. White , T. J. Whitis , W. J. Wisniewski , K. Wilson , M. S. Witherell , F. L. H. Wolfs , J. D. Wolfs , D. Woodward , S. D. Worm , X. Xiang , Q. Xiao , J. Xu , M. Yeh , J. Yin , I. Young , C. Zhang , P. Zarzhitsky

The LHC trigger and data acquisition systems will need significant modifications to operate at the HL-LHC. Due to the increased occupancy of each crossing, Level-1 trigger systems would experience degraded performance of the LHC algorithms…

Instrumentation and Detectors · Physics 2013-07-03 Wesley H. Smith

Axions are a well-motivated candidate for dark matter. The preeminent method to search for axion dark matter is known as the axion haloscope, which makes use of the conversion of axions to photons in a large magnetic field. Due to the weak…

Experimental efforts searching for dark matter particles over the last few decades have ruled out many candidates led by the new generation of tonne-scale liquid xenon. For light dark matter, hydrogen could be a better target than xenon as…

The RFX-mod2 Nuclear Fusion experiment is an upgrade of RFX-mod, shutdown in 2016. Among the other improvements in the machine structure and diagnostics, a larger number of electromagnetic probes (EMs) is foreseen to provide more…

We present a comprehensive analysis of electronic recoil vs. nuclear recoil discrimination in liquid/gas xenon time projection chambers, using calibration data from the 2013 and 2014-16 runs of the Large Underground Xenon (LUX) experiment.…

The Deep Underground Neutrino Experiment (DUNE) is a next-generation neutrino experiment that will probe the properties of these elusive particles with unparalleled precision. It will also act as an observatory for neutrino bursts caused by…

Instrumentation and Detectors · Physics 2024-05-30 Eric L. Flumerfelt

The LUXE experiment (Laser Und XFEL Experiment) is a new experiment in planning at DESY Hamburg using the electron beam of the European XFEL (Eu.XFEL). LUXE is intended to study collisions between a high-intensity optical laser and up to…

Instrumentation and Detectors · Physics 2021-12-16 Yan Benhammou

In the past decade, dual-phase xenon time projection chambers (Xe-TPCs) have emerged as some of the most powerful detectors in the fields of astroparticle physics and rare-event searches. Developed primarily towards the direct detection of…

Instrumentation and Detectors · Physics 2024-02-05 Laura Baudis

We are building an experiment to search for dark matter in the form of dark photons in the nano- to milli-eV mass range. This experiment is the electromagnetic dual of magnetic detector dark radio experiments. It is also a frequency-time…

Searching for dark matter (DM) at colliders is one of the biggest challenges in high-energy physics today. Significant efforts have been made to detect DM within the mass range of 1-10,000 GeV at the Large Hadron Collider and other…

High Energy Physics - Experiment · Physics 2025-11-17 Tamas Almos Vami

We extend the study of the performance of a prototype two-phase liquid xenon WIMP dark matter detector to recoil energies below 20 keV. We demonstrate a new method for obtaining the best estimate of the energies of events using a calibrated…

Astrophysics · Physics 2008-11-26 T. Shutt , C. E. Dahl , J. Kwong , A. Bolozdynya , P. Brusov

Axions are a promising cold dark matter candidate. Haloscopes, which use the conversion of axions to photons in the presence of a magnetic field to detect axions, are the basis of microwave cavity searches such as the Axion Dark Matter…

Cosmology and Nongalactic Astrophysics · Physics 2020-07-01 N. Crisosto , G. Rybka , P. Sikivie , N. S. Sullivan , D. B. Tanner , J. Yang

The WaveDAQ is a newly-designed digitization Trigger and Data AcQuisition system (TDAQ) allowing Multi-gigasample waveform recording on a large amount of channels (up to 16384) by using the DRS4 analog switched capacitor array as…

A new data acquisition system for the high resolution magnetic spectrometer Lintott at the superconducting Darmstadt electron linear accelerator S-DALINAC was developed. It allows inclusive and coincidence electron scattering experiments…

Instrumentation and Detectors · Physics 2022-04-27 M. Singer , U. Bonnes , A. D'Alessio , M. Hilcker , P. von Neumann-Cosel , N. Pietralla

The Argon Dark Matter experiment is a ton-scale double phase argon Time Projection Chamber designed for direct Dark Matter searches. It combines the detection of scintillation light together with the ionisation charge in order to…

The AGATA tracking detector array represents a significant improvement over previous Compton suppressed arrays. The construction of AGATA led to numerous technological breakthroughs in order to meet the requirements and the challenges of…

An optical quantum sensor (OQS) based on lasers and alkali-metal atoms is a sensitive ambient-temperature magnetometer that can be used in axion dark matter search with an inductor-capacitor (LC) circuit at kHz and MHz frequencies. We have…

Instrumentation and Detectors · Physics 2023-10-30 Young Jin Kim , Leanne Duffy , Igor Savukov , Ping-Han Chu

KLOE, a new state of the art detector recently commissioned for physics operation at DAFNE, has many innovative interesting features, especially in the DAQ and Trigger areas. Custom electronics assert a trigger in a 2 microseconds decision…

High Energy Physics - Experiment · Physics 2012-08-27 The KLOE Collaboration