Related papers: The real-time data processing and acquisition syst…

Status of the Project 8 Phase II

The Project 8 collaboration aims to measure the absolute neutrino mass scale using cyclotron radiation emission spectroscopy on the beta decay of tritium. The second phase of the project will measure a continuous spectrum of molecular…

Instrumentation and Detectors · Physics 2019-08-14 Mathieu Guigue

A high dynamic range data acquisition system for a solid-state electron Electric Dipole Moment experiment

We have built a high precision (24-bit) data acquisition (DAQ) system with eight simultaneously sampling input channels for the measurement of the electric dipole moment (EDM) of the electron. The DAQ system consists of two main components,…

Instrumentation and Detectors · Physics 2015-05-28 Young Jin Kim , Brandon Kunkler , Chen-Yu Liu , Gerard Visser

Project 8: Using Radio-Frequency Techniques to Measure Neutrino Mass

The Project 8 experiment aims to measure the neutrino mass using tritium beta decays. Beta-decay electron energies will be measured with a novel technique: as the electrons travel in a uniform magnetic field their cyclotron radiation will…

Instrumentation and Detectors · Physics 2019-08-14 N. S. Oblath

Results from the Project 8 phase-1 cyclotron radiation emission spectroscopy detector

The Project 8 collaboration seeks to measure the absolute neutrino mass scale by means of precision spectroscopy of the beta decay of tritium. Our technique, cyclotron radiation emission spectroscopy, measures the frequency of the radiation…

Instrumentation and Detectors · Physics 2017-10-06 A Ashtari Esfahani , S Böser , C Claessens , L de Viveiros , P J Doe , S Doeleman , M Fertl , E C Finn , J A Formaggio , M Guigue , K M Heeger , A M Jones , K Kazkaz , B H LaRoque , E Machado , B Monreal , J A Nikkel , N S Oblath , R G H Robertson , L J Rosenberg , G Rybka , L Saldaña , P L Slocum , J R Tedeschi , T Thümmler , B A Vandevender , M Wachtendonk , J Weintroub , A Young , E Zayas

The Triggerless Data Acquisition System of the XENONnT Experiment

The XENONnT detector uses the latest and largest liquid xenon-based time projection chamber (TPC) operated by the XENON Collaboration, aimed at detecting Weakly Interacting Massive Particles and conducting other rare event searches. The…

Instrumentation and Detectors · Physics 2023-08-09 E. Aprile , J. Aalbers , K. Abe , F. Agostini , S. Ahmed Maouloud , L. Althueser , B. Andrieu , E. Angelino , J. R. Angevaare , V. C. Antochi , D. Antón Martin , F. Arneodo , L. Baudis , A. L. Baxter , L. Bellagamba , R. Biondi , A. Bismark , E. J. Brookes , A. Brown , S. Bruenner , G. Bruno , R. Budnik , T. K. Bui , C. Cai , J. M. R. Cardoso , D. Cichon , A. P. Cimental Chavez , D. Coderre , A. P. Colijn , J. Conrad , J. J. Cuenca-García , J. P. Cussonneau , V. D'Andrea , M. P. Decowski , P. Di Gangi , S. Di Pede , S. Diglio , K. Eitel , A. Elykov , S. Farrell , A. D. Ferella , C. Ferrari , H. Fischer , M. Flierman , W. Fulgione , C. Fuselli , P. Gaemers , R. Gaior , A. Gallo Rosso , M. Galloway , F. Gao , R. Glade-Beucke , L. Grandi , J. Grigat , M. Guida , R. Hammann , A. Higuera , C. Hils , L. Hoetzsch , N. F. Hood , J. Howlett , M. Iacovacci , Y. Itow , J. Jakob , F. Joerg , A. Joy , N. Kato , M. Kara , P. Kavrigin , S. Kazama , M. Kobayashi , G. Koltman , A. Kopec , F. Kuger , H. Landsman , R. F. Lang , L. Levinson , I. Li , S. Li , S. Liang , S. Lindemann , M. Lindner , K. Liu , J. Loizeau , F. Lombardi , J. Long , J. A. M. Lopes , Y. Ma , C. Macolino , J. Mahlstedt , A. Mancuso , L. Manenti , F. Marignetti , T. Marrodán Undagoitia , K. Martens , J. Masbou , D. Masson , E. Masson , S. Mastroianni , M. Messina , K. Miuchi , K. Mizukoshi , A. Molinario , S. Moriyama , K. Morå , Y. Mosbacher , M. Murra , J. Müller , K. Ni , U. Oberlack , B. Paetsch , J. Palacio , R. Peres , C. Peters , J. Pienaar , M. Pierre , V. Pizzella , G. Plante , J. Qi , J. Qin , D. Ramírez García , A. Rocchetti , L. Sanchez , P. Sanchez-Lucas , J. M. F. dos Santos , I. Sarnoff , G. Sartorelli , J. Schreiner , D. Schulte , P. Schulte , H. Schulze Eißing , M. Schumann , L. Scotto Lavina , M. Selvi , F. Semeria , P. Shagin , S. Shi , E. Shockley , M. Silva , H. Simgen , A. Takeda , P. -L. Tan , A. Terliuk , D. Thers , F. Toschi , G. Trinchero , C. Tunnell , F. Tönnies , K. Valerius , G. Volta , C. Weinheimer , M. Weiss , D. Wenz , C. Wittweg , T. Wolf , D. Xu , Z. Xu , M. Yamashita , L. Yang , J. Ye , L. Yuan , G. Zavattini , S. Zerbo , M. Zhong , T. Zhu

The Data Acquisition System of the LZ Dark Matter Detector: FADR

The Data Acquisition System (DAQ) for the LUX-ZEPLIN (LZ) dark matter detector is described. The signals from 745 PMTs, distributed across three subsystems, are sampled with 100-MHz 32-channel digitizers (DDC-32s). A basic waveform analysis…

Instrumentation and Detectors · Physics 2024-08-20 J. Aalbers , D. S. Akerib , A. K. Al Musalhi , F. Alder , C. S. Amarasinghe , A. Ames , T. J. Anderson , N. Angelides , H. M. Araújo , J. E. Armstrong , M. Arthurs , A. Baker , S. Balashov , J. Bang , E. E. Barillier , J. W. Bargemann , K. Beattie , T. Benson , A. Bhatti , A. Biekert , T. P. Biesiadzinski , H. J. Birch , E. Bishop , G. M. Blockinger , B. Boxer , C. A. J. Brew , P. Brás , J. H. Buckley , S. Burdin , M. Buuck , M. C. Carmona-Benitez , M. Carter , A. Chawla , H. Chen , J. J. Cherwinka , Y. T. Chin , N. I. Chott , M. V. Converse , A. Cottle , G. Cox , D. Curran , C. E. Dahl , A. David , J. Delgaudio , S. Dey , L. de Viveiros , L. Di Felice , T. Dimino , C. Ding , J. E. Y. Dobson , E. Druszkiewicz , S. R. Eriksen , A. Fan , N. M. Fearon , N. Fieldhouse , S. Fiorucci , H. Flaecher , E. D. Fraser , T. M. A. Fruth , R. J. Gaitskell , A. Geffre , R. Gelfand , J. Genovesi , C. Ghag , R. Gibbons , S. Gokhale , J. Green , M. G. D. van der Grinten , J. J. Haiston , C. R. Hall , S. Han , E. Hartigan-O'Connor , S. J. Haselschwardt , M. A. Hernandez , S. A. Hertel , G. Heuermann , G. J. Homenides , M. Horn , D. Q. Huang , D. Hunt , E. Jacquet , R. S. James , J. Johnson , A. C. Kaboth , A. C. Kamaha , M. Kannichankandy , D. Khaitan , A. Khazov , I. Khurana , J. Kim , Y. D. Kim , J. Kingston , R. Kirk , D. Kodroff , L. Korley , E. V. Korolkova , M. Koyuncu , H. Kraus , S. Kravitz , L. Kreczko , V. A. Kudryavtsev , D. S. Leonard , K. T. Lesko , C. Levy , J. Lin , A. Lindote , R. Linehan , W. H. Lippincott , C. Loniewski , M. I. Lopes , W. Lorenzon , C. Lu , S. Luitz , P. A. Majewski , A. Manalaysay , R. L. Mannino , C. Maupin , M. E. McCarthy , G. McDowell , D. N. McKinsey , J. McLaughlin , J. B. Mclaughlin , R. McMonigle , E. H. Miller , E. Mizrachi , A. Monte , M. E. Monzani , M. Moongweluwan , J. D. Morales Mendoza , E. Morrison , B. J. Mount , M. Murdy , A. St. J. Murphy , A. Naylor , H. N. Nelson , F. Neves , A. Nguyen , J. A. Nikoleyczik , H. Oh , I. Olcina , M. A. Olevitch , K. C. Oliver-Mallory , J. Orpwood , K. J. Palladino , J. Palmer , N. J. Pannifer , N. Parveen , S. J. Patton , B. Penning , G. Pereira , E. Perry , T. Pershing , A. Piepke , Y. Qie , J. Reichenbacher , C. A. Rhyne , Q. Riffard , G. R. C. Rischbieter , H. S. Riyat , R. Rosero , T. Rushton , D. Rynders , D. Santone , R. Sarkis , A. B. M. R. Sazzad , R. W. Schnee , S. Shaw , T. Shutt , J. J. Silk , C. Silva , G. Sinev , J. Siniscalco , W. Skulski , R. Smith , V. N. Solovov , P. Sorensen , J. Soria , I. Stancu , A. Stevens , K. Stifter , B. Suerfu , T. J. Sumner , M. Szydagis , W. C. Taylor , D. R. Tiedt , M. Timalsina , Z. Tong , D. R. Tovey , J. Tranter , M. Trask , M. Tripathi , D. R. Tronstad , A. Vacheret , A. C. Vaitkus , J. Vaitkus , O. Valentino , V. Velan , A. Wang , J. J. Wang , Y. Wang , J. R. Watson , R. C. Webb , L. Weeldreyer , T. J. Whitis , M. Williams , W. J. Wisniewski , F. L. H. Wolfs , J. D. Wolfs , S. Woodford , D. Woodward , C. J. Wright , Q. Xia , X. Xiang , J. Xu , M. Yeh , J. Yin

Data Acquisition and Readout System for the LUX Dark Matter Experiment

LUX is a two-phase (liquid/gas) xenon time projection chamber designed to detect nuclear recoils from interactions with dark matter particles. Signals from the LUX detector are processed by custom-built analog electronics which provide…

Instrumentation and Methods for Astrophysics · Physics 2015-05-30 D. S. Akerib , X. Bai , S. Bedikian , E. Bernard , A. Bernstein , A. Bradley , S. B. Cahn , M. C. Carmona-Benitez , D. Carr , J. J. Chapman , K. Clark , T. Classen , T. Coffey , A. Curioni , S. Dazeley , L. deViveiros , M. Dragowsky , E. Druszkiewicz , C. H. Faham , S. Fiorucci , R. J. Gaitskell , K. R. Gibson , C. Hall , M. Hanhardt , B. Holbrook , M. Ihm , R. G. Jacobsen , L. Kastens , K. Kazkaz , R. Lander , N. Larsen , C. Lee , D. Leonard , K. Lesko , A. Lyashenko , D. C. Malling , R. Mannino , D. N. McKinsey , D. Mei , J. Mock , M. Morii , H. Nelson , J. A. Nikkel , M. Pangilinan , P. Phelps , T. Shutt , W. Skulski , P. Sorensen , J. Spaans , T. Stiegler , R. Svoboda , M. Sweany , M. Szydagis , J. Thomson , M. Tripathi , J. R. Verbus , N. Walsh , R. Webb , J. T. White , M. Wlasenko , F. L. H. Wolfs , M. Woods , C. Zhang

The Data Acquisition System for LZ

The Data Acquisition System of the LZ experiment, the 10-tonne dark matter detector to be installed at the Sanford Underground Research Facility (SURF), will collect signals from 788 photomultiplier tubes (PMTs). Because the signals from…

Instrumentation and Detectors · Physics 2015-11-30 Eryk Druszkiewicz

The XENON1T Data Acquisition System

The XENON1T liquid xenon time projection chamber is the most sensitive detector built to date for the measurement of direct interactions of weakly interacting massive particles with normal matter. The data acquisition system (DAQ) is…

Instrumentation and Detectors · Physics 2019-08-08 E. Aprile , J. Aalbers , F. Agostini , M. Alfonsi , L. Althueser , F. D. Amaro , V. C. Antochi , F. Arneodo , D. Barge , L. Baudis , B. Bauermeister , L. Bellagamba , M. L. Benabderrahmane , T. Berger , P. A. Breur , A. Brown , E. Brown , S. Bruenner , G. Bruno , R. Budnik , L. Bütikofer , C. Capelli , J. M. R. Cardoso , D. Cichon , D. Coderre , A. P. Colijn , J. Conrad , J. P. Cussonneau , M. P. Decowski , P. de Perio , P. Di Gangi , A. Di Giovanni , S. Diglio , A. Elykov , G. Eurin , J. Fei , A. D. Ferella , A. Fieguth , W. Fulgione , P. Gaemers , A. Gallo Rosso , M. Galloway , F. Gao , M. Garbini , L. Grandi , Z. Greene , C. Hasterok , E. Hogenbirk , J. Howlett , M. Iacovacci , R. Itay , F. Joerg , S. Kazama , A. Kish , M. Kobayashi , G. Koltman , A. Kopec , H. Landsman , R. F. Lang , L. Levinson , Q. Lin , S. Lindemann , M. Lindner , F. Lombardi , J. A. M. Lopes , E. López Fune , C. Macolino , J. Mahlstedt , A. Manfredini , F. Marignetti , T. Marrodán Undagoitia , J. Masbou , D. Masson , S. Mastroianni , M. Messina , K. Micheneau , K. Miller , A. Molinario , K. Morå , Y. Mosbacher , M. Murra , J. Naganoma , K. Ni , U. Oberlack , K. Odgers , B. Pelssers , R. Peres , F. Piastra , J. Pienaar , V. Pizzella , G. Plante , R. Podviianiuk , H. Qiu , D. Ramírez García , S. Reichard , B. Riedel , A. Rocchetti , N. Rupp , J. M. F. dos Santos , G. Sartorelli , N. Šarčević , M. Scheibelhut , S. Schindler , J. Schreiner , D. Schulte , M. Schumann , L. Scotto Lavina , M. Selvi , P. Shagin , E. Shockley , M. Silva , H. Simgen , C. Therreau , D. Thers , F. Toschi , G. Trinchero , C. D. Tunnell , N. Upole , M. Vargas , G. Volta , O. Wack , H. Wang , Y. Wei , C. Weinheimer , D. Wenz , C. Wittweg , J. Wulf , J. Ye , Y. Zhang , T. Zhu , J. P. Zopounidis , M. Pieracci , C. Tintori

Project 8: Determining neutrino mass from tritium beta decay using a frequency-based method

A general description is given of Project 8, a new approach to measuring the neutrino mass scale via the beta decay of tritium. In Project 8, the energy of electrons emitted in beta decay is determined from the frequency of cyclotron…

Nuclear Experiment · Physics 2013-09-30 P. J. Doe , J. Kofron , E. L. McBride , R. G. H. Robertson , L. J Rosenberg , G. Rybka , S. Doelman , A. Rogers , J. A. Formaggio , D. Furse , N. S. Oblath , B. H. LaRoque , M. Leber , B. Monreal , M. Bahr , D. M. Asner , A. M. Jones , J. Fernandes , B. A. VanDevender , R. Patterson , R. Bradley , T. Thuemmler

Project 8 Apparatus for Cyclotron Radiation Emission Spectroscopy with $^\mathrm{83m}$Kr and Tritium

Cyclotron Radiation Emission Spectroscopy (CRES) is a novel technique for the precise measurement of relativistic electron energy. This technique is being employed by the Project~8 collaboration for measuring a high-precision tritium beta…

Instrumentation and Detectors · Physics 2025-03-13 A. Ashtari Esfahani , D. M. Asner , S. Böser , N. Buzinsky , R. Cervantes , C. Claessens , L. de Viveiros , P. J. Doe , J. L. Fernandes , M. Fertl , J. A. Formaggio , D. Furse , L. Gladstone , M. Guigue , J. Hartse , K. M. Heeger , X. Huyan , A. M. Jones , J. A. Kofron , B. H. LaRoque , A. Lindman , E. Machado , E. L. McBride , P. Mohanmurthy , R. Mohiuddin , B. Monreal , E. C. Morrison , J. A. Nikkel , E. Novitski , N. S. Oblath , M. Ottiger , W. Pettus , R. Reimann , R. G. H. Robertson , G. Rybka , D. Rysewyk , L. Saldaña , P. L. Slocum , M. G. Sternberg , Y. H. Sun , P. T. Surukuchi , J. R. Tedeschi , A. B. Telles , F. Thomas , M. Thomas , T. Thümmler , L. Tvrznikova , B. A. VanDevender , M. Wachtendonk , M. Walter , J. Weintroub , T. E. Weiss , T. Wendler , N. L. Woods , E. Zayas , A. Ziegler

Project 8 detector upgrades for a tritium beta decay spectrum using cyclotron radiation

Following the successful observation of single conversion electrons from $^{83m}$Kr using Cyclotron Radiation Emission Spectroscopy (CRES), Project 8 is now advancing its focus toward a tritium beta decay spectrum. A tritium spectrum will…

Instrumentation and Detectors · Physics 2017-03-20 A Ashtari Esfahani , S Böser , C Claessens , L de Viveiros , P J Doe , S Doeleman , M Fertl , E C Finn , J A Formaggio , M Guigue , K M Heeger , A M Jones , K Kazkaz , B H LaRoque , E Machado , B Monreal , J A Nikkel , N S Oblath , R G H Robertson , L J Rosenberg , G Rybka , L Saldaña , P L Slocum , J R Tedeschi , T Thümmler , B A Vandevender , M Wachtendonk , J Weintroub , A Young , E Zayas

Development of an FPGA-based realtime DAQ system for axion haloscope experiments

A real-time Data Acquisition (DAQ) system for the CULTASK axion haloscope experiment was constructed and tested. The CULTASK is an experiment to search for cosmic axions using resonant cavities, to detect photons from axion conversion…

Instrumentation and Detectors · Physics 2021-11-30 MyeongJae Lee , ByeongRok Ko , Saebyeok Ahn

Data acquisition system in Run-0a for the J-PARC E16 experiment

J-PARC E16 is an experiment to examine the origin of hadron mass through a systematic measurement of spectral changes of vector mesons in nuclei. The measurement of $e^{+}e^{-}$ pairs from the decay of vector mesons will provide the…

Instrumentation and Detectors · Physics 2020-11-03 Tomonori Takahashi , Kazuya Aoki , Sakiko Ashikaga , Wen-Chen Chang , Eitaro Hamada , Ryotaro Honda , Masaya Ichikawa , Masahiro Ikeno , Shunsuke Kajikawa , Koki Kanno , Daisuke Kawama , Takehito Kondo , Che-Sheng Lin , Chih-Hsun Lin , Yuhei Morino , Tomoki Murakami , Wataru Nakai , Satomi Nakasuga , Megumi Naruki , Yuki Obara , Kyoichiro Ozawa , Hiroyuki Sako , Susumu Sato , Hiroshi Sendai , Kazuki Suzuki , Yudai Takaura , Manobu Tanaka , Tomohisa Uchida , Satoshi Yokkaichi

The Remote Analog to Digital Conversion DAQ System for the TRISTAN Detector Upgrade

The TRISTAN detector is an upgrade to the KATRIN experiment to enable a differential measurement of the tritium $\beta$-decay spectrum to search for the experimental signature of keV scale sterile neutrinos. The TRISTAN detector upgrade…

Instrumentation and Detectors · Physics 2026-04-27 Andrew S. Gavin , Matthias Balzer , Suren Chilingaryan , Reyco Henning , Andreas Kopmann , Susanne Mertens , Jalal Mostafa , Frank Simon , Nicholas Tan Jerome , Denis Tcherniakhovski , Korbinian Urban , John F. Wilkerson , Sascha Wüstling

Overview of Project 8 and Progress Towards Tritium Operation

Project 8 is a tritium endpoint neutrino mass experiment utilizing a phased program to achieve sensitivity to the range of neutrino masses allowed by the inverted mass hierarchy. The Cyclotron Radiation Emission Spectroscopy (CRES)…

Instrumentation and Detectors · Physics 2019-08-14 Walter C. Pettus

Scalable DAQ system operating the CHIPS-5 neutrino detector

The CHIPS R&D project focuses on development of low-cost water Cherenkov neutrino detectors through novel design strategies and resourceful engineering. This work presents an end-to-end DAQ solution intended for a recent 5 kt CHIPS…

Instrumentation and Detectors · Physics 2024-08-21 Belén Alonso Rancurel , Son Cao , Thomas J. Carroll , Rhys Castellan , Erika Catano-Mur , John P. Cesar , João A. B. Coelho , Patrick Dills , Thomas Dodwell , Jack Edmondson , Daan van Eijk , Quinn Fetterly , Zoé Garbal , Stefano Germani , Thomas Gilpin , Anthony Giraudo , Alec Habig , Daniel Hanuska , Harry Hausner , Wilson Y. Hernandez , Anna Holin , Junting Huang , Sebastian B. Jones , Albrecht Karle , George Kileff , Kai R. Jenkins , Paul Kooijman , Arthur Kreymer , Gabe M. LaFond , Karol Lang , Jeffrey P. Lazar , Rui Li , Kexin Liu , David A. Loving , Petr Mánek , Marvin L. Marshak , Jerry R. Meier , William Miller , Jeffrey K. Nelson , Christopher Ng , Ryan J. Nichol , Vittorio Paolone , Andrew Perch , Maciej M. Pfützner , Alexander Radovic , Katherine Rawlins , Patrick Roedl , Lucas Rogers , Ibrahim Safa , Alexandre Sousa , Josh Tingey , Jennifer Thomas , Jozef Trokan-Tenorio , Patricia Vahle , Richard Wade , Christopher Wendt , Daniel Wendt , Leigh H. Whitehead , Samuel Wolcott , Tianlu Yuan

A multi-channel DAQ system based on FPGA for long-distance transmission in nuclear physics experiments

As the development of electronic science and technology, electronic data acquisition (DAQ) system is more and more widely applied to nuclear physics experiments. Workstations are often utilized for data storage, data display, data…

Instrumentation and Detectors · Physics 2018-06-26 Hongwei Yu , Kezhu Song , Junfeng Yang , Kehan Li , Tengfei Chen , Shiyu Luo , Cheng Tang , Han Yu

Overview of the data acquisition system architecture for the DarkSide-20k experiment

The DarkSide-20k (DS-20k) detector is designed to directly search for dark matter by detecting weakly interacting massive particles (WIMPs) scattering off nuclei in a 20 tonnes target of low radioactivity Argon from underground sources, in…

Instrumentation and Detectors · Physics 2025-02-24 Maria Adriana Sabia

Data Acquisition Software for CMS HCAL Testbeams

Although CMS will not start operation for several years, many subdetector groups have active testbeam programs involving final or near-final electronics. The high-bandwidth electronics require the development of new DAQ systems including…

Instrumentation and Detectors · Physics 2007-05-23 J. Mans , W. Fisher