26 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.
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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
DUNE Offline Computing Conceptual Design Report
- Author
- Abed Abud Adam
- Abi Babak
- Acciarri Roberto
- Acero Mario
- Adames Marcio
- Adamov George
- Adamowski Mark
- Adams David
- Adinolfi Marco
- Adriano Cris
- Aduszkiewicz Antoni
- Aguilar Jessica
- Ahmad Zubayer
- Ahmed Jhanzeb
- Aimard Benjamin
- Akbar Faiza
- Allison Kyle
- Alonso Monsalve Saul
- Alrashed Munera
- Alt Christoph
- Alton Andrew
- Alvarez Rodrigo
- Amedo Pablo
- Anderson John
- Andrade Aldana Diego
- Andreopoulos Costas
- Andreotti Mirco
- Andrews Michael P.
- Andrianala Fenompanirina
- Andringa Sofia
- Anfimov Nikolay
- Anicézio Campanelli Wallison Luiz
- Ankowski Artur
- Antoniassi Marcelo
- Antonova Maria
- Antoshkin Alexander
- Antusch Stefan
- Aranda-Fernandez Alfredo
- Arellano Luciano
- Arnold Lukas
- Arroyave Manuel
- Asaadi Jonathan
- Asquith Lily
- Aurisano Adam
- Aushev Vladimir
- Autiero Dario
- Ayala-Torres Marco Alberto
- Azfar Farrukh
- Back Ashley
- Back Henning
- Back J.J.
- Bagaturia Iuri
- Bagby Linda
- Balashov Nikita
- Balasubramanian Supraja
- Baldi Pierre
- Baller Bruce
- Bambah Bindu
- Barao Fernando
- Barenboim Gabriela
- Barker G.J.
- Barkhouse Wayne
- Barnes Christopher
- Barr Giles
- Barranco Monarca Juan
- Barros Adilson
- Barros Nuno
- Barrow Joshua
- Basharina-Freshville Anastasia
- Bashyal Amit
- Basque Vincent
- Batchelor Charlie
- Battat James
- Battisti Federico
- Bay Fatih
- Bazetto Maria
- Bazo Alba José Luis
- Beacom J.F.
- Bechetoille Edouard
- Behera Biswaranjan
- Belchior Ewerton
- Bellantoni Leo
- Bellettini Giorgio
- Bellini Vincenzo
- Beltramello Olga
- Benekos Nektarios
- Benitez Montiel Carlos
- Benjamin Douglas
- Bento Neves Francisco
- Berger Joshua
- Berkman Sophie
- Bernardini Paolo
- Berner Roman
- Bersani Andrea
- Bertolucci Sergio
- Betancourt Minerba
- Betancur Rodríguez Amalia
- Bevan Adrian
- Bezawada Yashwanth
- Bezerra Anibal
- Bezerra Thiago
- Bhambure Jay
- Bhardwaj Akhil
- Bhatnagar Vipin
- Bhattacharjee Maharnab
- Bhattarai Devesh
- Bhuller Shyam
- Bhuyan Bipul
- Biagi Simone
- Bian Jianming
- Biassoni Matteo
- Biery Kurt
- Bilki Burak
- Bishai Mary
- Bisignani Valeria
- Bitadze Alexander
- Blake Andrew
- Blaszczyk F.D.
- Blazey Gerald
- Blend Dylan
- Blucher Edward
- Bobyshev Andrey
- Boissevain Jan
- Bolognesi Sara
- Bolton Timothy
- Bomben Luca
- Bonesini Maurizio
- Bonilla-Diaz Cesar
- Bonini Filiberto
- Booth Alexander
- Boran Fatma
- Bordoni Stefania
- Borkum Aran
- Bostan Nilay
- Bour Petr
- Boyden Daniel
- Bracinik Juraj
- Braga Davide
- Brailsford Dominic
- Branca Antonio
- Brandt Andrew
- Bremer Johan
- Brew Christopher
- Brice Stephen
- Brizzolari Claudia
- Bromberg Carl
- Brooke Jim
- Bross Alan
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- Brunetti Maria
- Buchanan Norman
- Budd Howard
- Buergi Jonas
- Caceres Vera Gian
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- Calabrese Roberto
- Calafiura Paolo
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- Chalifour Michel
- Chappell Andrew
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- Cicero Valentina
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- Copello Simone
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- Crisler Michael
- Cristaldo Esteban
- Crnkovic Jason
- Cross Ryan
- Cudd Andrew
- Cuesta Clara
- Cui Yanou
- Cussans David
- da Motta Helio
- da Silva Peres Leonardo
- Dalager Olivia
- Dallavalle Ricardo
- Dar Zubair
- David Claire
- David Quentin
- Davies Gavin
- Davini Stefano
- Dawson Jaime
- de Bonis Isabelle
- de Gouvea Andre
- de Holanda Pedro
- de Icaza Astiz I.L.
- de Jong Paul
- de la Torre Andres
- de Leo Veronica
- de Lurgio Patrick
- de Mello Neto J.R.
- de Roeck Albert
- de Romeri Valentina
- de Souza Greg
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- Decowski M. Patrick
- Deisting Alexander
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- Detje J.P.
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- Gomez Fajardo L.S.
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- Harris Deborah
- Hartnell Jeffrey
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- Hatfield Kaleb
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- He Muyuan
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- Henry Sarah
- Hernandez Morquecho Miguel Angel
- Herner Kenneth
- Hewes V.
- Hilgenberg Christopher
- Hill Tony
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- Weatherly Pierce
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- Weber Michele
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- Weinstein Amanda
- Wenman Dan
- Wetstein Matthew
- Whilhelmi James
- White A.
- White A.
- White Brandon
- White Stephen
- Whitehead Leigh
- Whittington Denver
- Wilking Michael
- Wilkinson Alexander
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- Williams Zachary
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- Wilson Robert
- Wisniewski William
- Wolcott Jeremy
- Wolfs Jean
- Wongjirad Taritree
- Wood Anthony
- Wood Kevin
- Worcester Elizabeth
- Worcester Matthew
- Wospakrik Marianette
- Wresilo Karolina
- Wret Clarence
- Wu Shaowei
- Wu Wanwei
- Wu Wenjie
- Xiao Yiwen
- Xiotidis Ioannis
- Yaeggy Barbara
- Yandel Erin
- Yang Guang
- Yang Kang
- Yang Tingjun
- Yankelevich Alejandro
- Yershov Nikolai
- Yonehara Katsuya
- Yoon Young Soo
- Young Tim
- Yu B.
- Yu H.
- Yu H.
- Yu Jae
- Yu Yiding
- Yuan Wenlong
- Zaki Rowan
- Zalesak Jaroslav
- Zambelli Laura
- Zamorano Bruno
- Zani Andrea
- Zazueta Luis
- Zeller Geralyn
- Zennamo Joseph
- Zeug Kyle
- Zhang Chao
- Zhang Shuaixiang
- Zhang Yuze
- Zhao Manhong
- Zhivun Elena
- Zimmerman E.D.
- Zucchelli Stefano
- Zuklin Josef
- Zutshi Vishnu
- Zwaska Robert
- Publication venue
- HAL CCSD
- Publication date
- 10/11/2022
- Field of study
This document describes Offline Software and Computing for the Deep Underground Neutrino Experiment (DUNE) experiment, in particular, the conceptual design of the offline computing needed to accomplish its physics goals. Our emphasis in this document is the development of the computing infrastructure needed to acquire, catalog, reconstruct, simulate and analyze the data from the DUNE experiment and its prototypes. In this effort, we concentrate on developing the tools and systems thatfacilitate the development and deployment of advanced algorithms. Rather than prescribing particular algorithms, our goal is to provide resources that are flexible and accessible enough to support creative software solutions as HEP computing evolves and to provide computing that achieves the physics goals of the DUNE experiment
Snowmass Neutrino Frontier: DUNE Physics Summary
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- Wret C.
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- Wu W.
- Xiao Y.
- Xie F.
- Yaeggy B.
- Yandel E.
- Yang G.
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- Yankelevich A.
- Yershov N.
- Yonehara K.
- Yoon Y.S.
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- Yu B.
- Yu H.
- Yu H.
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- Yu Y.
- Yuan W.
- Zaki R.
- Zalesak J.
- Zambelli L.
- Zamorano B.
- Zani A.
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- Zeller G.P.
- Zennamo J.
- Zetina L.M. Montaño
- Zeug K.
- Zhang C.
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- 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
DUNE Offline Computing Conceptual Design Report
- Author
- Abed Abud Adam
- Abi Babak
- Acciarri Roberto
- Acero Mario
- Adames Marcio
- Adamov George
- Adamowski Mark
- Adams David
- Adinolfi Marco
- Adriano Cris
- Aduszkiewicz Antoni
- Aguilar Jessica
- Ahmad Zubayer
- Ahmed Jhanzeb
- Aimard Benjamin
- Akbar Faiza
- Allison Kyle
- Alonso Monsalve Saul
- Alrashed Munera
- Alt Christoph
- Alton Andrew
- Alvarez Rodrigo
- Amedo Pablo
- Anderson John
- Andrade Aldana Diego
- Andreopoulos Costas
- Andreotti Mirco
- Andrews Michael P.
- Andrianala Fenompanirina
- Andringa Sofia
- Anfimov Nikolay
- Anicézio Campanelli Wallison Luiz
- Ankowski Artur
- Antoniassi Marcelo
- Antonova Maria
- Antoshkin Alexander
- Antusch Stefan
- Aranda-Fernandez Alfredo
- Arellano Luciano
- Arnold Lukas
- Arroyave Manuel
- Asaadi Jonathan
- Asquith Lily
- Aurisano Adam
- Aushev Vladimir
- Autiero Dario
- Ayala-Torres Marco Alberto
- Azfar Farrukh
- Back Ashley
- Back Henning
- Back J.J.
- Bagaturia Iuri
- Bagby Linda
- Balashov Nikita
- Balasubramanian Supraja
- Baldi Pierre
- Baller Bruce
- Bambah Bindu
- Barao Fernando
- Barenboim Gabriela
- Barker G.J.
- Barkhouse Wayne
- Barnes Christopher
- Barr Giles
- Barranco Monarca Juan
- Barros Adilson
- Barros Nuno
- Barrow Joshua
- Basharina-Freshville Anastasia
- Bashyal Amit
- Basque Vincent
- Batchelor Charlie
- Battat James
- Battisti Federico
- Bay Fatih
- Bazetto Maria
- Bazo Alba José Luis
- Beacom J.F.
- Bechetoille Edouard
- Behera Biswaranjan
- Belchior Ewerton
- Bellantoni Leo
- Bellettini Giorgio
- Bellini Vincenzo
- Beltramello Olga
- Benekos Nektarios
- Benitez Montiel Carlos
- Benjamin Douglas
- Bento Neves Francisco
- Berger Joshua
- Berkman Sophie
- Bernardini Paolo
- Berner Roman
- Bersani Andrea
- Bertolucci Sergio
- Betancourt Minerba
- Betancur Rodríguez Amalia
- Bevan Adrian
- Bezawada Yashwanth
- Bezerra Anibal
- Bezerra Thiago
- Bhambure Jay
- Bhardwaj Akhil
- Bhatnagar Vipin
- Bhattacharjee Maharnab
- Bhattarai Devesh
- Bhuller Shyam
- Bhuyan Bipul
- Biagi Simone
- Bian Jianming
- Biassoni Matteo
- Biery Kurt
- Bilki Burak
- Bishai Mary
- Bisignani Valeria
- Bitadze Alexander
- Blake Andrew
- Blaszczyk F.D.
- Blazey Gerald
- Blend Dylan
- Blucher Edward
- Bobyshev Andrey
- Boissevain Jan
- Bolognesi Sara
- Bolton Timothy
- Bomben Luca
- Bonesini Maurizio
- Bonilla-Diaz Cesar
- Bonini Filiberto
- Booth Alexander
- Boran Fatma
- Bordoni Stefania
- Borkum Aran
- Bostan Nilay
- Bour Petr
- Boyden Daniel
- Bracinik Juraj
- Braga Davide
- Brailsford Dominic
- Branca Antonio
- Brandt Andrew
- Bremer Johan
- Brew Christopher
- Brice Stephen
- Brizzolari Claudia
- Bromberg Carl
- Brooke Jim
- Bross Alan
- Brunetti Giulia
- Brunetti Maria
- Buchanan Norman
- Budd Howard
- Buergi Jonas
- Caceres Vera Gian
- Cagnoli Irene
- Cai Tejin
- Caiulo Davide
- Calabrese Roberto
- Calafiura Paolo
- Calcutt Jacob
- Calin Marius
- Calivers Livio
- Calvez Steven
- Calvo Enrique
- Caminata Alessio
- Caratelli David
- Carber Daniel
- Carceller J.C.
- Carini Gabriella
- Carlus Bruno
- Carneiro Mateus
- Carniti Paolo
- Caro Terrazas Ivan
- Carranza Hector
- Carrara Nicholas
- Carroll Lauren
- Carroll Thomas
- Castaño Forero Javier
- Castillo Andrés
- Catano-Mur Erika
- Cattadori Carla
- Cavalier Fabien
- Cavallaro Giuseppe
- Cavanna Flavio
- Centro Sandro
- Cerati Giuseppe
- Cervelli Alberto
- Cervera Villanueva Anselmo
- Chakraborty Kaustav
- Chalifour Michel
- Chappell Andrew
- Chardonnet Etienne
- Charitonidis Nikolas
- Chatterjee Animesh
- Chattopadhyay Subhasish
- Chen Hucheng
- Chen Mu-Chun
- Chen Yifan
- Chen Zheyang
- Chen-Wishart Zachary
- Cheon Yoolim
- Cherdack Daniel
- Chi Cheng-Yi
- Childress Sam
- Chirco Robert
- Chiriacescu Ana
- Chitirasreemadam Namitha
- Cho Kihyeon
- Choate Sarah
- Chokheli David
- Chong P.S.
- Chowdhury Barnali
- Christensen Anne
- Christian David
- Christodoulou Georgios
- Chukanov Artem
- Chung Moses
- Church Eric
- Cicero Valentina
- Clarke Peter
- Cline Gordon
- Coan Thomas
- Cocco Alfredo
- Coelho Joao
- Collot Johann
- Conley Erin
- Conrad Janet M.
- Convery Mark
- Copello Simone
- Cova Paolo
- Cremaldi Lucien
- Cremonesi Linda
- Crespo-Anadón J.I.
- Crisler Michael
- Cristaldo Esteban
- Crnkovic Jason
- Cross Ryan
- Cudd Andrew
- Cuesta Clara
- Cui Yanou
- Cussans David
- da Motta Helio
- da Silva Peres Leonardo
- Dalager Olivia
- Dallavalle Ricardo
- Dar Zubair
- David Claire
- David Quentin
- Davies Gavin
- Davini Stefano
- Dawson Jaime
- de Bonis Isabelle
- de Gouvea Andre
- de Holanda Pedro
- de Icaza Astiz I.L.
- de Jong Paul
- de la Torre Andres
- de Leo Veronica
- de Lurgio Patrick
- de Mello Neto J.R.
- de Roeck Albert
- de Romeri Valentina
- de Souza Greg
- De Kaushik
- De Shruti
- Debbins Paul
- Decowski M. Patrick
- Deisting Alexander
- Delbart Alain
- Delepine David
- Delgado Maritza
- Dell'Acqua Andrea
- Delmonte Nicola
- Demar Philip
- Demuth David
- Dennis Steve
- Densham Chris
- Deptuch Grzegorz
- Detje J.P.
- Devi Ritu
- Dharmapalan Ranjan
- Di Capua Francesco
- Di Domenico Antonio
- Di Domizio Sergio
- Di Giulio Letizia
- Di Noto Lea
- Dias Marco
- Diaz Jorge S.
- Ding Pengfei
- Distefano Carla
- Diurba Richard
- Diwan Milind
- Djurcic Zelimir
- Doering Dionisio
- Dolan Stephen
- Dolek Furkan
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- Vagins M.R.
- Vahle Patricia
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- Vallazza Erik
- Valle J.W.
- Vallecorsa Sofia
- van Berg Rick
- van de Water Richard
- Vanegas Forero David
- Vannerom David
- Varanini Filippo
- Vargas Oliva Danaisis
- Varner Gary
- Vasina Svetlana
- Vaughan Noah
- Vaziri Kamran
- Vega Juan
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- Verdugo Antonio
- Vergani Stefano
- Vermeulen M.A.
- Verzocchi Marco
- Vicenzi Matteo
- Vieira de Souza Henrique
- Vignoli Chiara
- Vilela Cristovao
- Viren Brett
- Vrba Tomas
- Vuong Quynh
- Wachala Tomasz
- Wagner Alexander
- Waldron Abigail
- Wallbank Michael
- Walton Tammy
- Wang Hanguo
- Wang Jingbo
- Wang L.
- Wang Michael
- Wang Xiaoran
- Wang Y.
- Wang Y.
- Warburton Karl
- Warner David
- Wascko Morgan
- Waters David
- Watson Alan
- Wawrowska Klaudia
- Weatherly Pierce
- Weber Alfons
- Weber Michele
- Wei Hanyu
- Weinstein Amanda
- Wenman Dan
- Wetstein Matthew
- Whilhelmi James
- White A.
- White A.
- White Brandon
- White Stephen
- Whitehead Leigh
- Whittington Denver
- Wilking Michael
- Wilkinson Alexander
- Wilkinson Callum
- Williams Zachary
- Wilson Fergus
- Wilson Robert
- Wisniewski William
- Wolcott Jeremy
- Wolfs Jean
- Wongjirad Taritree
- Wood Anthony
- Wood Kevin
- Worcester Elizabeth
- Worcester Matthew
- Wospakrik Marianette
- Wresilo Karolina
- Wret Clarence
- Wu Shaowei
- Wu Wanwei
- Wu Wenjie
- Xiao Yiwen
- Xiotidis Ioannis
- Yaeggy Barbara
- Yandel Erin
- Yang Guang
- Yang Kang
- Yang Tingjun
- Yankelevich Alejandro
- Yershov Nikolai
- Yonehara Katsuya
- Yoon Young Soo
- Young Tim
- Yu B.
- Yu H.
- Yu H.
- Yu Jae
- Yu Yiding
- Yuan Wenlong
- Zaki Rowan
- Zalesak Jaroslav
- Zambelli Laura
- Zamorano Bruno
- Zani Andrea
- Zazueta Luis
- Zeller Geralyn
- Zennamo Joseph
- Zeug Kyle
- Zhang Chao
- Zhang Shuaixiang
- Zhang Yuze
- Zhao Manhong
- Zhivun Elena
- Zimmerman E.D.
- Zucchelli Stefano
- Zuklin Josef
- Zutshi Vishnu
- Zwaska Robert
- Publication venue
- HAL CCSD
- Publication date
- 10/11/2022
- Field of study
This document describes Offline Software and Computing for the Deep Underground Neutrino Experiment (DUNE) experiment, in particular, the conceptual design of the offline computing needed to accomplish its physics goals. Our emphasis in this document is the development of the computing infrastructure needed to acquire, catalog, reconstruct, simulate and analyze the data from the DUNE experiment and its prototypes. In this effort, we concentrate on developing the tools and systems thatfacilitate the development and deployment of advanced algorithms. Rather than prescribing particular algorithms, our goal is to provide resources that are flexible and accessible enough to support creative software solutions as HEP computing evolves and to provide computing that achieves the physics goals of the DUNE experiment
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.
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- 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
A Gaseous Argon-Based Near Detector to Enhance the Physics Capabilities of DUNE
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- Publication venue
- HAL CCSD
- Publication date
- 26/07/2022
- Field of study
This document presents the concept and physics case for a magnetized gaseous argon-based detector system (ND-GAr) for the Deep Underground Neutrino Experiment (DUNE) Near Detector. This detector system is required in order for DUNE to reach its full physics potential in the measurement of CP violation and in delivering precision measurements of oscillation parameters. In addition to its critical role in the long-baseline oscillation program, ND-GAr will extend the overall physics program of DUNE. The LBNF high-intensity proton beam will provide a large flux of neutrinos that is sampled by ND-GAr, enabling DUNE to discover new particles and search for new interactions and symmetries beyond those predicted in the Standard Model
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
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- 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
A Gaseous Argon-Based Near Detector to Enhance the Physics Capabilities of DUNE
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- Abi B.
- Abud A. Abed
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- HAL CCSD
- Publication date
- 26/07/2022
- Field of study
This document presents the concept and physics case for a magnetized gaseous argon-based detector system (ND-GAr) for the Deep Underground Neutrino Experiment (DUNE) Near Detector. This detector system is required in order for DUNE to reach its full physics potential in the measurement of CP violation and in delivering precision measurements of oscillation parameters. In addition to its critical role in the long-baseline oscillation program, ND-GAr will extend the overall physics program of DUNE. The LBNF high-intensity proton beam will provide a large flux of neutrinos that is sampled by ND-GAr, enabling DUNE to discover new particles and search for new interactions and symmetries beyond those predicted in the Standard Model
Doping Liquid Argon with Xenon in ProtoDUNE Single-Phase: Effects on Scintillation Light
- Author
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- Abi B
- Acciarri R
- Acero M.A
- Adames M.R
- Adamov G
- Adamowski M
- Adams D
- Adinolfi M
- Adriano C
- Aduszkiewicz A
- Aguilar J
- Aimard B
- Akbar F
- Allison K
- Alonso Monsalve S
- Alonso M.J. Rodriguez
- Alrashed M
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- Anderson J
- Andrade D.A
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- Zhang C
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- Zhao M
- Zhivun E
- 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