33 research outputs found
Highly-parallelized simulation of a pixelated LArTPC on a GPU
- Author
- Abed Abud A.
- Abi B.
- Acciarri R.
- Acero M.A.
- Adames M.R.
- Adamov G.
- Adamowski M.
- Adams D.
- Adinolfi M.
- Adriano C.
- Aduszkiewicz A.
- Aguilar J.
- Ahmad Z.
- Ahmed J.
- Aimard B.
- Akbar F.
- Allison K.
- Alonso Monsalve S.
- Alrashed M.
- Alt C.
- Alton A.
- Alvarez R.
- Amedo P.
- Anderson J.
- Andrade D.A.
- Andreopoulos C.
- Andreotti M.
- Andrews M.P.
- Andrianala F.
- Andringa S.
- Anfimov N.
- Anicézio Campanelli W.L.
- Ankowski A.
- Antoniassi M.
- Antonova M.
- Antoshkin A.
- Antusch S.
- Aranda-Fernandez A.
- Arellano L.
- Arnold L.O.
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2023
- Field of study
The rapid development of general-purpose computing on graphics processing units (GPGPU) is allowing the implementation of highly-parallelized Monte Carlo simulation chains for particle physics experiments. This technique is particularly suitable for the simulation of a pixelated charge readout for time projection chambers, given the large number of channels that this technology employs. Here we present the first implementation of a full microphysical simulator of a liquid argon time projection chamber (LArTPC) equipped with light readout and pixelated charge readout, developed for the DUNE Near Detector. The software is implemented with an end-to-end set of GPU-optimized algorithms. The algorithms have been written in Python and translated into CUDA kernels using Numba, a just-in-time compiler for a subset of Python and NumPy instructions. The GPU implementation achieves a speed up of four orders of magnitude compared with the equivalent CPU version. The simulation of the current induced on 10^3 pixels takes around 1 ms on the GPU, compared with approximately 10 s on the CPU. The results of the simulation are compared against data from a pixel-readout LArTPC prototype
Polymeric Membranes Containing Phosphorus in the Chain for Solid Polymer Electrolytes
- Author
- Publication venue
- 'Informa UK Limited'
- Publication date
- Field of study
Dual Atrioventricular Nodal Pathways: A Reappraisal
- Author
- Agha A.S.
- Amat-y-Leon F.
- Anderson R.H.
- Asinger RW
- Bauerfeind RA.
- Becker A.E
- Bigger J.T.
- Bisset JK
- Brechenmacher C
- Capelle FJL.
- Coumel P.
- Curry P.V.L
- Denes P
- Denes P
- Denes P.
- Denes P.
- Dopirak MR
- Drury A.N.
- Ferrier GR
- Gallavardin L.
- Gettes L.S.
- Goldreyer B.N.
- Goldreyer B.N.
- Hunt N.C.
- Iliescu G.C.
- Janse M.J.
- Janse MJ
- Josephson ME.
- Klein H.O.
- Lister J.W.
- Mendez C
- Mendez C
- Mines GR.
- Moe G.K.
- Moe GK.
- Motte P.G
- Narula O.S.
- Neuss H
- Rinkenberger R.L.
- Rosenblueth A.
- Satake S
- Scherlag BJ
- Schuilenburg R.M.
- Schuilenburg RM
- Schuilenburg RM
- Schuilenburg RM.
- Sclarovsky S
- Spurrell R.A.J
- Strasberg B
- Sung R.J
- Sung RJ
- Thapar M.K.
- Touboul P
- Waxman MB.
- Wellens H.J.J
- Wellens H.J.J
- Wellens HJJ
- White P.D.
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- Wit AL.
- Wu D
- Wu D
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- Zipes D.P.
- Publication venue
- 'Wiley'
- Publication date
- Field of study
Long-baseline neutrino oscillation physics potential of the DUNE experiment: DUNE Collaboration
- Publication venue
- Publication date
- 01/01/2020
- Field of study
The sensitivity of the Deep Underground Neutrino Experiment (DUNE) to neutrino oscillation is determined, based on a full simulation, reconstruction, and event selection of the far detector and a full simulation and parameterized analysis of the near detector. Detailed uncertainties due to the flux prediction, neutrino interaction model, and detector effects are included. DUNE will resolve the neutrino mass ordering to a precision of 5σ, for all δCP values, after 2 years of running with the nominal detector design and beam configuration. It has the potential to observe charge-parity violation in the neutrino sector to a precision of 3σ (5σ) after an exposure of 5 (10) years, for 50% of all δCP values. It will also make precise measurements of other parameters governing long-baseline neutrino oscillation, and after an exposure of 15 years will achieve a similar sensitivity to sin 22 θ13 to current reactor experiments. © 2020, The Author(s)
Supernova neutrino burst detection with the deep underground neutrino experiment: DUNE Collaboration
- Publication venue
- Publication date
- 01/01/2021
- Field of study
The deep underground neutrino experiment (DUNE), a 40-kton underground liquid argon time projection chamber experiment, will be sensitive to the electron-neutrino flavor component of the burst of neutrinos expected from the next Galactic core-collapse supernova. Such an observation will bring unique insight into the astrophysics of core collapse as well as into the properties of neutrinos. The general capabilities of DUNE for neutrino detection in the relevant few- to few-tens-of-MeV neutrino energy range will be described. As an example, DUNE’s ability to constrain the νe spectral parameters of the neutrino burst will be considered. © 2021, The Author(s)
First results on ProtoDUNE-SP liquid argon time projection chamber performance from a beam test at the CERN Neutrino Platform
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- Publication venue
- HAL CCSD
- Publication date
- 01/01/2020
- Field of study
International audienceThe ProtoDUNE-SP detector is a single-phase liquid argon time projection chamber with an active volume of 7.2× 6.1× 7.0 m3. It is installed at the CERN Neutrino Platform in a specially-constructed beam that delivers charged pions, kaons, protons, muons and electrons with momenta in the range 0.3 GeV/c to 7 GeV/c. Beam line instrumentation provides accurate momentum measurements and particle identification. The ProtoDUNE-SP detector is a prototype for the first far detector module of the Deep Underground Neutrino Experiment, and it incorporates full-size components as designed for that module. This paper describes the beam line, the time projection chamber, the photon detectors, the cosmic-ray tagger, the signal processing and particle reconstruction. It presents the first results on ProtoDUNE-SP's performance, including noise and gain measurements, dE/dx calibration for muons, protons, pions and electrons, drift electron lifetime measurements, and photon detector noise, signal sensitivity and time resolution measurements. The measured values meet or exceed the specifications for the DUNE far detector, in several cases by large margins. ProtoDUNE-SP's successful operation starting in 2018 and its production of large samples of high-quality data demonstrate the effectiveness of the single-phase far detector design
Deep underground neutrino experiment (DUNE) near detector conceptual design report
- Publication venue
- Publication date
- 01/01/2021
- Field of study
The Deep Underground Neutrino Experiment (DUNE) is an international, world-class experiment aimed at exploring fundamental questions about the universe that are at the forefront of astrophysics and particle physics research. DUNE will study questions pertaining to the preponderance of matter over antimatter in the early universe, the dynamics of supernovae, the subtleties of neutrino interaction physics, and a number of beyond the Standard Model topics accessible in a powerful neutrino beam. A critical component of the DUNE physics program involves the study of changes in a powerful beam of neutrinos, i.e., neutrino oscillations, as the neutrinos propagate a long distance. The experiment consists of a near detector, sited close to the source of the beam, and a far detector, sited along the beam at a large distance. This document, the DUNE Near Detector Conceptual Design Report (CDR), describes the design of the DUNE near detector and the science program that drives the design and technology choices. The goals and requirements underlying the design, along with projected performance are given. It serves as a starting point for a more detailed design that will be described in future documents. © 2021 by the authors. Licensee MDPI, Basel, Switzerland
Snowmass Neutrino Frontier: DUNE Physics Summary
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- Zucchelli S.
- Zuklin J.
- Zutshi V.
- Zwaska R.
- Publication venue
- HAL CCSD
- Publication date
- 26/07/2022
- Field of study
The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino oscillation experiment with a primary physics goal of observing neutrino and antineutrino oscillation patterns to precisely measure the parameters governing long-baseline neutrino oscillation in a single experiment, and to test the three-flavor paradigm. DUNE's design has been developed by a large, international collaboration of scientists and engineers to have unique capability to measure neutrino oscillation as a function of energy in a broadband beam, to resolve degeneracy among oscillation parameters, and to control systematic uncertainty using the exquisite imaging capability of massive LArTPC far detector modules and an argon-based near detector. DUNE's neutrino oscillation measurements will unambiguously resolve the neutrino mass ordering and provide the sensitivity to discover CP violation in neutrinos for a wide range of possible values of δCP. DUNE is also uniquely sensitive to electron neutrinos from a galactic supernova burst, and to a broad range of physics beyond the Standard Model (BSM), including nucleon decays. DUNE is anticipated to begin collecting physics data with Phase I, an initial experiment configuration consisting of two far detector modules and a minimal suite of near detector components, with a 1.2 MW proton beam. To realize its extensive, world-leading physics potential requires the full scope of DUNE be completed in Phase II. The three Phase II upgrades are all necessary to achieve DUNE's physics goals: (1) addition of far detector modules three and four for a total FD fiducial mass of at least 40 kt, (2) upgrade of the proton beam power from 1.2 MW to 2.4 MW, and (3) replacement of the near detector's temporary muon spectrometer with a magnetized, high-pressure gaseous argon TPC and calorimeter
Doping Liquid Argon with Xenon in ProtoDUNE Single-Phase: Effects on Scintillation Light
- Author
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- Abi B
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- Zimmerman E.D
- Zucchelli S
- Zuklin J
- Zutshi V
- Publication venue
- HAL CCSD
- Publication date
- 08/02/2024
- Field of study
International audienceDoping of liquid argon TPCs (LArTPCs) with a small concentration of xenon is a technique for light-shifting and facilitates the detection of the liquid argon scintillation light. In this paper, we present the results of the first doping test ever performed in a kiloton-scale LArTPC. From February to May 2020, we carried out this special run in the single-phase DUNE Far Detector prototype (ProtoDUNE-SP) at CERN, featuring 770 t of total liquid argon mass with 410 t of fiducial mass. The goal of the run was to measure the light and charge response of the detector to the addition of xenon, up to a concentration of 18.8 ppm. The main purpose was to test the possibility for reduction of non-uniformities in light collection, caused by deployment of photon detectors only within the anode planes. Light collection was analysed as a function of the xenon concentration, by using the pre-existing photon detection system (PDS) of ProtoDUNE-SP and an additional smaller set-up installed specifically for this run. In this paper we first summarize our current understanding of the argon-xenon energy transfer process and the impact of the presence of nitrogen in argon with and without xenon dopant. We then describe the key elements of ProtoDUNE-SP and the injection method deployed. Two dedicated photon detectors were able to collect the light produced by xenon and the total light. The ratio of these components was measured to be about 0.65 as 18.8 ppm of xenon were injected. We performed studies of the collection efficiency as a function of the distance between tracks and light detectors, demonstrating enhanced uniformity of response for the anode-mounted PDS. We also show that xenon doping can substantially recover light losses due to contamination of the liquid argon by nitrogen
Snowmass Neutrino Frontier: DUNE Physics Summary
- Author
- Abed Abud A.
- Abi B.
- Acciarri R.
- Acero M.A.
- Adames M.R.
- Adamov G.
- Adamowski M.
- Adams D.
- Adinolfi M.
- Adriano C.
- Aduszkiewicz A.
- Aguilar J.
- Ahmad Z.
- Ahmed J.
- Aimard B.
- Akbar F.
- Alba J.L. Bazo
- Ali-Mohammadzadeh B.
- Alion T.
- Allison K.
- Alonso M.J. Rodriguez
- Alrashed M.
- Alt C.
- Alton A.
- Alvarez R.
- Amedo P.
- Anderson J.
- Andreopoulos C.
- Andreotti M.
- Andrews M.P.
- Andrianala F.
- Andringa S.
- Anfimov N.
- Ankowski A.
- Antoniassi M.
- Antonova M.
- Antoshkin A.
- Antusch S.
- Aranda-Fernandez A.
- Arellano L.
- Arnold L.O.
- Arroyave M.A.
- Asaadi J.
- Asquith L.
- Aurisano A.
- Aushev V.
- Autiero D.
- Ayala-Torres M.
- Azfar F.
- Back A.
- Back H.
- Back J.J.
- Backhouse C.
- Bagaturia I.
- Bagby L.
- Balashov N.
- Balasubramanian S.
- Baldi P.
- Baller B.
- Bambah B.
- Barao F.
- Barenboim G.
- Barker G.J.
- Barkhouse W.
- Barnes C.
- Barr G.
- Barrios J. Hoyos
- Barros A.
- Barros N.
- Barrow J.L.
- Basharina-Freshville A.
- Bashyal A.
- Basque V.
- Batchelor C.
- Battat J.B.R.
- Battisti F.
- Bay F.
- Bazetto M.C.Q.
- Beacom J.F.
- Bechetoille E.
- Behera B.
- Beigbeder C.
- Belchior E.
- Bellantoni L.
- Bellettini G.
- Bellini V.
- Beltramello O.
- Benekos N.
- Berger J.
- Berkman S.
- Bermeo L.V. Gomez
- Bernardini P.
- Berner R.M.
- Bersani A.
- Bertolucci S.
- Betancourt M.
- Bevan A.
- Bezawada Y.
- Bezerra A.T.
- Bezerra T.J.C.
- Bhardwaj A.
- Bhatnagar V.
- Bhattacharjee M.
- Bhattarai D.
- Bhuller S.
- Bhuyan B.
- Biagi S.
- Bian J.
- Biassoni M.
- Biery K.
- Bilki B.
- Bishai M.
- Bitadze A.
- Blake A.
- Blaszczyk F.D.M.
- Blazey G.C.
- Blucher E.
- Boissevain J.
- Bolognesi S.
- Bolton T.
- Bomben L.
- Bonesini M.
- Bongrand M.
- Bonilla-Diaz C.
- Bonini F.
- Booth A.
- Boran F.
- Bordoni S.
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- Wang J.
- Wang L.
- Wang M.H.L.S.
- Wang X.
- Wang Y.
- Wang Y.
- Warburton K.
- Warner D.
- Wascko M.O.
- Waters D.
- Watson A.
- Wawrowska K.
- Weatherly P.
- Weber A.
- Weber M.
- Wei H.
- Weinstein A.
- Wenman D.
- Wetstein M.
- White A.
- Whitehead L.H.
- Whittington D.
- Wilking M.J.
- Wilkinson A.
- Wilkinson C.
- Williams Z.
- Wilson F.
- Wilson R.J.
- Wisniewski W.
- Wolcott J.
- Wongjirad T.
- Wood A.
- Wood K.
- Worcester E.
- Worcester M.
- Wresilo K.
- Wret C.
- Wu W.
- Wu W.
- Xiao Y.
- Xie F.
- Yaeggy B.
- Yandel E.
- Yang G.
- Yang K.
- Yang T.
- Yankelevich A.
- Yershov N.
- Yonehara K.
- Yoon Y.S.
- Young T.
- Yu B.
- Yu H.
- Yu H.
- Yu J.
- Yu Y.
- Yuan W.
- Zaki R.
- Zalesak J.
- Zambelli L.
- Zamorano B.
- Zani A.
- Zazueta L.
- Zeller G.P.
- Zennamo J.
- Zetina L.M. Montaño
- Zeug K.
- Zhang C.
- Zhang S.
- Zhang Y.
- Zhao M.
- Zhivun E.
- Zhu G.
- Zimmerman E.D.
- Zucchelli S.
- Zuklin J.
- Zutshi V.
- Zwaska R.
- Publication venue
- HAL CCSD
- Publication date
- 26/07/2022
- Field of study
The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino oscillation experiment with a primary physics goal of observing neutrino and antineutrino oscillation patterns to precisely measure the parameters governing long-baseline neutrino oscillation in a single experiment, and to test the three-flavor paradigm. DUNE's design has been developed by a large, international collaboration of scientists and engineers to have unique capability to measure neutrino oscillation as a function of energy in a broadband beam, to resolve degeneracy among oscillation parameters, and to control systematic uncertainty using the exquisite imaging capability of massive LArTPC far detector modules and an argon-based near detector. DUNE's neutrino oscillation measurements will unambiguously resolve the neutrino mass ordering and provide the sensitivity to discover CP violation in neutrinos for a wide range of possible values of δCP. DUNE is also uniquely sensitive to electron neutrinos from a galactic supernova burst, and to a broad range of physics beyond the Standard Model (BSM), including nucleon decays. DUNE is anticipated to begin collecting physics data with Phase I, an initial experiment configuration consisting of two far detector modules and a minimal suite of near detector components, with a 1.2 MW proton beam. To realize its extensive, world-leading physics potential requires the full scope of DUNE be completed in Phase II. The three Phase II upgrades are all necessary to achieve DUNE's physics goals: (1) addition of far detector modules three and four for a total FD fiducial mass of at least 40 kt, (2) upgrade of the proton beam power from 1.2 MW to 2.4 MW, and (3) replacement of the near detector's temporary muon spectrometer with a magnetized, high-pressure gaseous argon TPC and calorimeter