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Microprocessors in physics experiments at SLAC
- Author
- Publication venue
- Stanford Linear Accelerator Center
- Publication date
- 01/04/1981
- Field of study
The increasing size and complexity of high energy physics experiments is changing the way data are collected. To implement a trigger or event filter requires complex logic which may have to be modified as the experiment proceeds. Simply to monitor a detector, large amounts of data must be processed on line. The use of microprocessors or other programmable devices can help to achieve these ends flexibly and economically. At SLAC, a number of microprocessor-based systems have been built and are in use in experimental setups, and others are now being developed. This talk is a review of existing systems and their use in experiments, and of developments in progress and future plans
The Long-Baseline Neutrino Experiment: Exploring Fundamental Symmetries of the Universe
- Author
- Adams Corey
- Adams David
- Akiri Tarek
- Alion Tyler
- Anderson Kris
- Andreopoulos Costas
- Andrews Mike
- Anghel Ioana
- Anjos JoĂŁo Carlos Costa dos
- Antonello Maddalena
- Arrieta-Diaz Enrique
- Artuso Marina
- Asaadi Jonathan
- Bai Xinhua
- Baibussinov Bagdat
- Baird Michael
- Balantekin Baha
- Baller Bruce
- Baptista Brian
- Barker D'Ann
- Barker Gary
- Barletta William A.
- Barr Giles
- Bartoszek Larry
- Bashyal Amit
- Bass Matt
- Bellini Vincenzo
- Benetti Pietro Angelo
- Berger Bruce E.
- Bergevin Marc
- Berman Eileen
- Berns Hans-Gerd
- Bernstein Adam
- Bernstein Robert
- Bhandari Babu
- Bhatnagar Vipin
- Bhuyan Bipul
- Bian Jianming
- Bishai Mary
- Blake Andrew
- Blaszczyk Flor
- Blaufuss Erik
- Bleakley Bruce
- Blucher Edward
- Blusk Steve
- Bocean Virgil
- Boffelli F.
- Boissevain Jan
- Bolton Timothy
- Bonesini Maurizio
- Boyd Steve
- Brandt Andrew
- Breedon Richard
- Bromberg Carl
- Brown Ralph
- Brunetti Giullia
- Buchanan Norman
- Bugg Bill
- Busenitz Jerome
- Calligarich E.
- Camilleri Leslie
- Carminati Giada
- Carr Rachel
- Castromonte Cesar
- Cavanna Flavio
- Centro Sandro
- Chen Alex
- Chen Hucheng
- Chen Kai
- Cherdack Daniel
- Chi Cheng-Yi
- Childress Sam
- Choudhary Brajesh Chandra
- Christodoulou Georgios
- Christofferson Cabot-Ann
- Church Eric
- Cline David
- Coan Thomas
- Cocco Alfredo
- Coelho Joao
- Coleman Stephen
- Conrad Janet M.
- Convery Mark
- Corey Robert
- Corwin Luke
- Cranshaw Jack
- Cronin-Hennessy Daniel
- Curioni A.
- da Motta Helio
- Davenne Tristan
- Davies Gavin S.
- Dazeley Steven
- de Geronimo Gianluigi
- de Gouvea Andre
- de Jong Jeffrey K.
- De Kaushik
- Demuth David
- Densham Chris
- Diwan Milind
- Djurcic Zelimir
- Dolfini R.
- Dolph Jeffrey
- Drake Gary
- Dye Stephen
- Dyuang Hongue
- Edmunds Daniel
- Elliott Steven
- Elnimr Muhammad
- Eno Sarah
- Enomoto Sanshiro
- Escobar Carlos O.
- Evans Justin
- Falcone A.
- Falk Lisa
- Farbin Amir
- Farnese Christian
- Fava Angela
- Felde John
- Fernandes S.
- Ferroni Fernando
- Feyzi Farshid
- Fields Laura
- Finch Alex
- Fitton Mike
- Fleming Bonnie
- Fowler Jack
- Fox Walt
- Friedland Alex
- Fuess Stu
- Fujikawa Brian
- Gallagher Hugh
- Gandhi Raj
- Garvey Gerald
- Gehman Victor M.
- Gibin Daniele
- Gill Ronald
- Gomes Ricardo A.
- Goodman Maury C.
- Goon Jason
- Graf Nicholas
- Graham Mathew
- Gran Rik
- Grant Christopher
- Grant Nick
- Greenlee Herbert
- Greenler Leland
- Grullon Sean
- Guardincerri Elena
- Guarino Victor
- Guarnaccia Evan
- Guedes Germano
- Guenette Roxanne
- Guglielmi Alberto
- Guzzo Marcelo M.
- Habig Alec T.
- Hackenburg Robert W.
- Hadavand Haleh
- Hahn Alan
- Haigh Martin
- Haines Todd
- Handler Thomas
- Hans Sunej
- Hartnell Jeff
- Harton John
- Hatcher Robert
- Hatzikoutelis Athans
- Hays Steven
- Hazen Eric
- Headley Mike
- Heavey Anne
- Heeger Karsten
- Heise Jaret
- Hellauer Robert
- Hewes Jeremy
- Himmel Alexander
- Hogan Matthew
- Holanda Pedro
- Holin Anna
- Horton-Smith Glenn
- Howell Joe
- Hurh Patrick
- Huston Joey
- Hylen James
- Imlay Richard
- Insler Jonathan
- Introzzi G.
- Isvan Zeynep
- Jackson Chris
- Jacobsen John
- Jaffe David E.
- James Cat
- Jen Chun-Min
- Johnson Marvin
- Johnson Randy
- Johnson Robert
- Johnson Scott
- Johnston William
- Johnstone John
- Jones Ben J. P.
- Jostlein H.
- Junk Thomas
- Kadel Richard
- Kaess Karl
- Karagiorgi Georgia
- Kaspar Jarek
- Katori Teppei
- Kayser Boris
- Kearns Edward
- Keener Paul
- Kemp Ernesto
- Kettell Steve H.
- Kirby Mike
- Klein Joshua
- Koizumi Gordon
- Kopp Sacha
- Kormos Laura
- Kropp William
- Kudryavtsev Vitaly A.
- Kumar Ashok
- Kumar Jason
- Kutter Thomas
- La Zia Franco
- Lande Kenneth
- Lane Charles
- Lang Karol
- Lanni Francesco
- Lanza Richard
- Latorre Tony
- LBNE Collaboration
- Learned John
- Lee David
- Lee Kevin
- Li Qizhong
- Li Shaorui
- Li Yichen
- Li Zepeng
- Libo Jiang
- Linden Steve
- Ling Jiajie
- Link Jonathan
- Littenberg Laurence
- Liu Hu
- Liu Qiuguang
- Liu Tiankuan
- Losecco John
- Louis William
- Lundberg Byron
- Lundin Tracy
- Lundy Jay
- Machado Ana Amelia
- Maesano Cara
- Magill Steve
- Mahler George
- Malon David
- Malys Stephen
- Mammoliti Francesco
- Mandal Samit Kumar
- Mann Anthony
- Mantsch Paul
- Marchionni Alberto
- Marciano William
- Mariani Camillo
- Maricic Jelena
- Marino Alysia
- Marshak Marvin
- Marshall John
- Matsuno Shiegenobu
- Mauger Christopher
- Mavrokoridis Konstantinos
- Mayer Nate
- McCauley Neil
- McCluskey Elaine
- McDonald Kirk
- McFarland Kevin
- McKee David
- McKeown Robert
- McTaggart Robert
- Mehdiyev Rashid
- Mei Dongming
- Menegolli A.
- Meng Guang
- Meng Yixiong
- Mertins David
- Messier Mark
- Metcalf William
- Milincic Radovan
- Miller William
- Mills Geoff
- Mishra Sanjib R.
- Mokhov Nikolai
- Montanari Claudio
- Montanari David
- Moore Craig
- Morfin Jorge
- Morgan Ben
- Morse William
- Moss Zander
- Moura CĂ©lio A.
- Mufson Stuart
- Muller David
- Musser Jim
- Naples Donna
- Napolitano Jim
- Newcomer Mitch
- Nichol Ryan
- Nicholls Tim
- Niner Evan
- Norris Barry
- Nowak Jaroslaw
- O'Keeffe Helen
- Oliveira Roberto
- Olson Travis
- Page Brian
- Pakvasa Sandip
- Palamara Ornella
- Paley Jon
- Paolone Vittorio
- Papadimitriou Vaia
- Park Seongtae
- Parsa Zohreh
- Partyka Kinga
- Paulos Bob
- Pavlovic Zarko
- Peeters Simon
- Perch Andy
- Perkin Jon D.
- Petti Roberto
- Petukhov Andre
- Pietropaolo Francesco
- Plunkett Robert
- Polly Chris
- Pordes Stephen
- Potekhin Maxim
- Potenza Renato
- Prakash Arati
- Prokofiev Oleg
- Qian Xin
- Raaf Jennifer L.
- Radeka Veljko
- Rakhno Igor
- Ramachers Yorck
- Rameika Regina
- Ramsey John
- Rappoldi A.
- Raselli G. L.
- Ratoff Peter
- Ravindra Shreyas
- Rebel Brian
- Reichenbacher Juergen
- Reitzner Dianne
- Rescia Sergio
- Richardson Martin
- Rielage Kieth
- Riesselmann Kurt
- Robinson Matt
- Rochester Leon
- Ronquest Michael
- Rosen Marc
- Rossella M.
- Rubbia Carlo
- Rucinski Russ
- Sahijpal Sandeep
- Sahoo Himansu
- Sala Paola
- Salmiera Delia
- Samios Nicholas
- Sanchez Mayly
- Scaramelli Alberto
- Schellman Heidi
- Schmitt Richard
- Schmitz David
- Schneps Jack
- Scholberg Kate
- Segreto Ettore
- Seibert Stanley
- Sexton-Kennedy Liz
- Shaevitz Mike
- Shanahan Peter
- Sharma Rahul
- Shaw Terri
- Simos Nikolaos
- Singh Venktesh
- Sinnis Gus
- Sippach William
- Skwarnicki Tomasz
- Smy Michael
- Sobel Henry
- Soderberg Mitch
- Sondericker John
- Sondheim Walter
- Sousa Alexandre
- Spooner Neil J. C.
- Stancari Michelle
- Stancu Ion
- Stefan Dorota
- Stefanik Andy
- Stewart James
- Stone Sheldon
- Strait James
- Strait Matthew
- Striganov Sergei
- Sullivan Gregory
- Sun Yujing
- Suter Louise
- Svenson Andrew
- Svoboda Robert
- Szczerbinska Barbara
- Szelc Andrzej
- Szydagis Matthew
- Söldner-Rembold Stefan
- Talaga Richard
- Tamsett Matthew
- Tariq Salman
- Tayloe Rex
- Taylor Charles
- Taylor David
- Teymourian Artin
- Themann Harry
- Thiesse Matthew
- Thomas Jenny
- Thompson Lee F.
- Thomson Mark
- Thorn Craig
- Thorpe Matt
- Tian Xinchun
- Tiedt Doug
- Toki Walter
- Tolich Nikolai
- Torti M.
- Toups Matt
- Touramanis Christos
- Tripathi Mani
- Tropin Igor
- Tsai Yun-Tse
- Tull Craig
- Tzanov Martin
- Urheim Jon
- Usman Shawn
- Vagins Mark
- Valdiviesso Gustavo
- Van Berg Rick
- Van de Water Richard
- Van Gemmeren Peter
- Varanini Filippo
- Varner Gary
- Vaziri Kamran
- Velev Gueorgui
- Ventura Sandro
- Vignoli Chiara
- Viren Brett
- Wahl Dan
- Waldron Abby
- Walter Christopher W.
- Wang Hanguo
- Wang Wei
- Warburton Karl
- Warner David
- Wasserman Ryan
- Watson Blake
- Weber Alfons
- Wei Wenzhao
- Wells Douglas
- Wetstein Matthew
- White Andy
- White Hywel
- Whitehead Lisa
- Whittington Denver
- Willhite Joshua
- Wilson Robert J.
- Winslow Lindley
- Wood Kevin
- Worcester Elizabeth
- Worcester Matthew
- Xin Tian
- Yarritu Kevin
- Ye Jingbo
- Yeh Minfang
- Yu Bo
- Yu Jae
- Yuan Tianlu
- Zani A.
- Zeller Geralyn P.
- Zhang Chao
- Zhang Chao
- Zimmerman Eric D.
- Zwaska Robert
- Publication venue
- Publication date
- 28/07/2013
- Field of study
The preponderance of matter over antimatter in the early Universe, the
dynamics of the supernova bursts that produced the heavy elements necessary for
life and whether protons eventually decay --- these mysteries at the forefront
of particle physics and astrophysics are key to understanding the early
evolution of our Universe, its current state and its eventual fate. The
Long-Baseline Neutrino Experiment (LBNE) represents an extensively developed
plan for a world-class experiment dedicated to addressing these questions. LBNE
is conceived around three central components: (1) a new, high-intensity
neutrino source generated from a megawatt-class proton accelerator at Fermi
National Accelerator Laboratory, (2) a near neutrino detector just downstream
of the source, and (3) a massive liquid argon time-projection chamber deployed
as a far detector deep underground at the Sanford Underground Research
Facility. This facility, located at the site of the former Homestake Mine in
Lead, South Dakota, is approximately 1,300 km from the neutrino source at
Fermilab -- a distance (baseline) that delivers optimal sensitivity to neutrino
charge-parity symmetry violation and mass ordering effects. This ambitious yet
cost-effective design incorporates scalability and flexibility and can
accommodate a variety of upgrades and contributions. With its exceptional
combination of experimental configuration, technical capabilities, and
potential for transformative discoveries, LBNE promises to be a vital facility
for the field of particle physics worldwide, providing physicists from around
the globe with opportunities to collaborate in a twenty to thirty year program
of exciting science. In this document we provide a comprehensive overview of
LBNE's scientific objectives, its place in the landscape of neutrino physics
worldwide, the technologies it will incorporate and the capabilities it will
possess.Comment: Major update of previous version. This is the reference document for
LBNE science program and current status. Chapters 1, 3, and 9 provide a
comprehensive overview of LBNE's scientific objectives, its place in the
landscape of neutrino physics worldwide, the technologies it will incorporate
and the capabilities it will possess. 288 pages, 116 figure
Doping liquid argon with xenon in ProtoDUNE Single-Phase: effects on scintillation light
- 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.
- Aimard B.
- Akbar F.
- Allison K.
- Alonso Monsalve S.
- Alrashed M.
- Alton A.
- Alvarez R.
- Amar Es-sghir H.
- Amedo P.
- Anderson J.
- Andrade D. A.
- Andreopoulos C.
- Andreotti M.
- Andrews M. P.
- Andrianala F.
- Andringa S.
- Anfimov N.
- Ankowski A.
- Antoniassi M.
- Antonova M.
- Antoshkin A.
- Aranda-Fernandez A.
- Arellano L.
- Arrieta Diaz E.
- Arroyave M. A.
- Asaadi J.
- Ashkenazi A.
- Asquith L.
- Atkin E.
- Auguste D.
- Aurisano A.
- Aushev V.
- Autiero D.
- Azfar F.
- Back A.
- Back H.
- Back J. J.
- Bagaturia I.
- Bagby L.
- Balashov N.
- Balasubramanian S.
- Baldi P.
- Baldini W.
- Baller B.
- Bambah B.
- Banerjee R.
- Barao F.
- Barenboim G.
- Barham AlzaÌs P.
- Barker G. J.
- Barkhouse W.
- Barr G.
- Barranco Monarca J.
- Barros A.
- Barros N.
- Barrow D.
- Barrow J. L.
- Basharina-Freshville A.
- Bashyal A.
- Basque V.
- Batchelor C.
- Bathe-Peters L.
- Battat J. B. R.
- Battisti F.
- Bay F.
- Bazetto M. C. Q.
- Bazo Alba J. L. L.
- Beacom J. F.
- Bechetoille E.
- Behera B.
- Belchior E.
- Bell G.
- Bellantoni L.
- Bellettini G.
- Bellini V.
- Beltramello O.
- Benekos N.
- Benitez Montiel C.
- Benjamin D.
- Bento Neves F.
- Berger J.
- Berkman S.
- Bernardini P.
- Bersani A.
- Bertolucci S.
- Betancourt M.
- Betancur RodriÌguez A.
- Bevan A.
- Bezawada Y.
- Bezerra A. T.
- Bezerra T. J.
- Bhat A.
- Bhatnagar V.
- Bhatt J.
- Bhattacharjee M.
- Bhattacharya M.
- Bhuller S.
- Bhuyan B.
- Biagi S.
- Bian J.
- Biery K.
- Bilki B.
- Bishai M.
- Bitadze A.
- Blake A.
- Blaszczyk F. D.
- Blazey G. C.
- Blucher E.
- Boissevain J.
- Bolognesi S.
- Bolton T.
- Bomben L.
- Bonesini M.
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- Bonini F.
- Booth A.
- Boran F.
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- Borkum A.
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- Bracinik J.
- Braga D.
- Brahma B.
- Brailsford D.
- Bramati F.
- Branca A.
- Brandt A.
- Bremer J.
- Brew C.
- Brice S. J.
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- Brizzolari C.
- Bromberg C.
- Brooke J.
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- Brunetti G.
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- Butchart S.
- Caceres Vera G.
- Cagnoli I.
- Cai T.
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- Calcutt J.
- Calin M.
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- Caminata A.
- Campanelli W.
- Campos Benitez A.
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- CapoÌ J.
- Caracas I.
- Caratelli D.
- Carber D.
- Carceller J. M.
- Carini G.
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- Carneiro M. F.
- Carniti P.
- Caro Terrazas I.
- Carranza H.
- Carrara N.
- Carroll L.
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- Carter A.
- Casazza D.
- CastanÌo Forero J. F.
- CastanÌo F. A.
- Castillo A.
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- Cattadori C.
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- Centro S.
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- Chatterjee A.
- Chen H.
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- Chen W. C.
- Chen Y.
- Chen-Wishart Z.
- Cherdack D.
- Chi C.
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- Cho K.
- Choate S.
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- Chowdhury B.
- Christian D.
- Chukanov A.
- Chung M.
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- Cicero V.
- Ciolini R.
- Clair J.
- Clarke P.
- Cline G.
- Coan T. E.
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- Conley E.
- Conrad J. M.
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- Cooke P.
- Copello S.
- Cova P.
- Cox C.
- Cremaldi L.
- Cremonesi L.
- Crespo-AnadoÌn J. I.
- Crisler M.
- Cristaldo E.
- Crnkovic J.
- Crone G.
- Cross R.
- Cudd A.
- Cuesta C.
- Cui Y.
- Cussans D.
- da Motta H.
- Da Silva Peres L.
- Dai J.
- Dalager O.
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- Dar Z. A.
- Darby R.
- Das Chagas Marques F.
- David Q.
- Davies G. S.
- Davini S.
- Dawson J.
- De Aguiar R.
- De Almeida P.
- De Bonis I.
- de GouveÌa A.
- De Holanda P. C.
- De Icaza Astiz I. L.
- De Jong P.
- De la Torre A.
- De Lurgio P.
- de Mello Neto J. R. T.
- De Roeck A.
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- Debbins P.
- Decowski M. P.
- Delbart A.
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- Dell'Acqua A.
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- Dennis S.
- Densham C.
- Denton P.
- Deptuch G. W.
- Detje J. P.
- Devine J.
- Dharmapalan R.
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- Di Domenico A.
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- Di Giulio L.
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- Distefano C.
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- Doering D.
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- Domenici D.
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- Doyle T. A.
- Dragone A.
- Drielsma F.
- Duarte L.
- Duchesneau D.
- Duffy K.
- Dugas K.
- Dunne P.
- Dutta B.
- Duyang H.
- Dvornikov O.
- Dwyer D. A.
- Dyshkant A. S.
- Dytman S.
- Eads M.
- Earle A.
- Edayath S.
- Edmunds D.
- Eisch J.
- Englezos P.
- Ereditato A.
- Erjavec T.
- Escobar C. O.
- Evans J. J.
- Ewart E.
- Ezeribe A. C.
- Fahey K.
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- Fani' M.
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- Farzan Y.
- Fedoseev D.
- Felix J.
- Feng Y.
- Fernandez-Martinez E.
- Ferraro F.
- Ferry G.
- Fields L.
- Filip P.
- Filkins A.
- Filthaut F.
- Fine R.
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- Fogarty S.
- Foreman W.
- Forero D. V.
- Fowler J.
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- Franklin J.
- Freeman J.
- Fried J.
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- Fuess S.
- Furic I. K.
- Furman K.
- Furmanski A. P.
- Gaba R.
- Gabrielli A.
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- Galizzi F.
- Gallagher H.
- Gallas A.
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- Gamberini E.
- Gamble T.
- Ganacim F.
- Gandhi R.
- Ganguly S.
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- GarciÌa-Peris M. AÌ.
- Gardiner S.
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- Gomez Fajardo L. S.
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- Gonzalez-Diaz D.
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- Goodman M. C.
- Goswami S.
- Gotti C.
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- Grace C.
- Gramellini E.
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- Grant C.
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- Green P.
- Greenberg S.
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- Griffith W. C.
- Groetschla F. T.
- Grzelak K.
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- Guarino V.
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- Guenette R.
- Guerard E.
- Guerzoni M.
- Guffanti D.
- Guglielmi A.
- Guo B.
- Guo Y.
- Gupta A.
- Gupta V.
- Gurung G.
- Gutierrez D.
- Guzowski P.
- Guzzo M. M.
- Gwon S.
- Haaf K.
- Habig A.
- Hadavand H.
- Haenni R.
- Hagaman L.
- Hahn A.
- Haiston J.
- Hakenmueller J.
- Hamernik T.
- Hamilton P.
- Hancock J.
- Happacher F.
- Harris D. A.
- Hartnell J.
- Hartnett T.
- Harton J.
- Hasegawa T.
- Hasnip C.
- Hatcher R.
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- Hazen E.
- He M.
- Heavey A.
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- Heise J.
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- Hernandez Morquecho M. A.
- Herner K.
- Hewes V.
- Higuera A.
- Hilgenberg C.
- Hillier S. J.
- Himmel A.
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- Hirsch L. R.
- Ho J.
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- Hoppe E.
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- Houdy T.
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- Howell R.
- Hristova I.
- Hronek M. S.
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- Publication venue
- Publication date
- 01/01/2024
- Field of study
Doping 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 720 t of total liquid argon mass with 410 t of fiducial mass. A 5.4 ppm nitrogen contamination was present during the xenon doping campaign. 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
Gamma-ray and radio properties of six pulsars detected by the fermi large area telescope
- Author
- Abdo Aous A.
- Ackermann Markus
- Ajello Marco
- Angelis Alessandro de
- Axelsson Magnus
- Baldini Luca
- Ballet Jean
- Barbiellini Guido
- Bastieri Denis
- Baughman Brian M.
- Bechtol Keith
- Bellazzini Ronaldo
- Berenji Bijan
- Bloom Elliott D.
- Bonamente Emanuele
- Borgland Anders W.
- Bregeon Jean
- Brez Alessandro
- Brigida Monica
- Bruel Philippe
- Burnett Thompson H.
- Buson Sara
- Caliandro Giuseppe Andrea
- Cameron Robert A.
- Camilo Fernando
- Caraveo Patrizia A.
- Casandjian Jean-Marc
- Cecchi Claudia
- Charles Eric
- Chekhtman Alexandre
- Cheung C. C. Teddy
- Chiang James
- Ciprini Stefano
- Claus Rachel
- Cognard Ismaël
- Cohen-Tanugi Johan
- Cominsky Lynn R.
- Conrad Jan
- Couto e Silva Eduardo do
- Cutini Sara
- Dermer Charles Dennison
- Desvignes Gregory
- Digel Seth W.
- Dormody Michael
- Drell Persis S.
- Dubois Richard
- Dumora Denis
- Farnier Christian
- Favuzzi Cecilia
- Fegan Stephen, J.
- Focke Warren B.
- Fortin Pascal
- Frailis Marco
- Francesco Giordano
- Freire Paulo C. C.
- Fusco Piergiorgio
- Gargano Fabio
- Gasparrini Dario
- Gehrels Neil
- Germani Stefano
- Giavitto Gianluca
- Giebels Berrie
- Giglietto Nicola
- Glanzman Tom
- Godfrey Gary
- Grenier Isabelle A.
- Grondin Marie-HĂ©lĂšne
- Grove J. Eric
- Guillemot Lucas
- Guiriec Sylvain
- Hanabata Yoshitaka
- Harding Alice K.
- Hays Elizabeth
- Hobbs George
- Hughes Richard E.
- Jackson Miranda S.
- Johannesson Gueolaugur
- Johnson A. S.
- Johnson Tyrel J.
- Johnson W. Neil
- Johnston Simon
- Kamae Tuneyoshi
- Katagiri Hideaki
- Kataoka Jun
- Kawai Nobuyuki
- Keith Mike
- Kerr Matthew
- Knödlseder JĂŒrgen
- Kocian Martin L.
- Kramer Michael
- Kuss M.
- Lande Joshua
- Latronico Luca
- Lemoine-Goumard Marianne
- Longo Francesco
- Loparco Francesco
- Lott Benoit
- Lovellette Michael N.
- Lubrano Pasquale
- Luca Andrea de
- Lyne Andrew G.
- Makeev Andrey
- Manchester Richard N.
- Mazziotta Mario Nicola
- McEnery Julie E.
- McGlynn Sinead
- Meurer Christine
- Michelson Peter F.
- Mitthumsiri Warit
- Mizuno Takafumi
- Moiseev Alex A.
- Monte Claudia
- Monzani Maria Elena
- Morselli Aldo
- Moskalenko Igor V.
- Murgia Simona
- Nolan Pat L.
- Norris Joel N.
- Nuss Eric
- Ohsugi Takashi
- Omodei Nicola
- Orlando Elena
- Ormes Jonathan F.
- Palma Francesco de
- Paneque David
- Panetta Jim H.
- Paolo Spinelli
- Parent D.
- Pelassa VĂ©ronique
- Pepe Monica
- Pesce-Rollins Melissa
- Piron Frédéric
- Porter Troy A.
- RainĂČ Silvia
- Ransom Scott M.
- Razzano Massimiliano
- Rea Nanda
- Reimer Anita
- Reimer Olaf
- Reposeur Thierry
- Riccardo Rando
- Rochester Leon S.
- RodrĂguez Ana Yaiza
- Romani Roger W.
- Roth Marshall
- Ryde Felix
- Sadrozinski Hartmut F. W.
- Sander Aaron
- Saz Parkinson Pablo M.
- SgrĂČ Carmelo
- Siskind Eric J.
- Smith David A.
- Smith Patrick D.
- Spandre Gloria
- Stappers Ben W.
- Strickman Mark Samuel
- Suson Daniel Jeffrey
- SĂĄnchez David
- Tajima Hiro
- Takahashi Hiromitsu
- Tanaka Takaaki
- Thayer Jana B.
- Thayer John Gregg
- Theureau Gilles
- Thompson David J.
- Thorsett Stephen E.
- Tibaldo Luigi
- Torres Diego F.
- Tosti Gino
- Tramacere Andrea
- Uchiyama Yasunobu
- Usher Tracy L.
- Van Etten Adam
- Vasileiou Vlasios
- Venter Christo
- Vilchez NicolĂĄs
- Vitale Vincenzo
- Waite Anthony P.
- Wang Na
- Wang Ping
- Watters Kyle
- Weltevrede Patrick
- Winer Brian L.
- Wood Kent S.
- Ylinen Tomi
- Ziegler Marcus
- Ăelik Ăzlem
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We report the detection of pulsed Îł-rays for PSRs J0631+1036, J0659+1414, J0742-2822, J1420-6048, J1509-5850, and J1718-3825 using the Large Area Telescope on board the Fermi Gamma-ray Space Telescope (formerly known as GLAST). Although these six pulsars are diverse in terms of their spin parameters, they share an important feature: their Îł-ray light curves are (at least given the current count statistics) single peaked. For two pulsars, there are hints for a double-peaked structure in the light curves. The shapes of the observed light curves of this group of pulsars are discussed in the light of models for which the emission originates from high up in the magnetosphere. The observed phases of the Îł-ray light curves are, in general, consistent with those predicted by high-altitude models, although we speculate that the Îł-ray emission of PSR J0659+1414, possibly featuring the softest spectrum of all Fermi pulsars coupled with a very low efficiency, arises from relatively low down in the magnetosphere. High-quality radio polarization data are available showing that all but one have a high degree of linear polarization. This allows us to place some constraints on the viewing geometry and aids the comparison of the Îł-ray light curves with high-energy beam models
Multi-messenger observations of a binary neutron star merger
- Author
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- Aartsen MG
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- Zhang WZ
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Y-H
- Zhang YF
- Zhang YJ
- Zhang Z
- Zhang ZL
- Zhao C
- Zhao HS
- Zhao JL
- Zhao W
- Zhao XF
- Zheng SJ
- Zhou H
- Zhou J
- Zhou M
- Zhou Z
- Zhu SJ
- Zhu XJ
- Zhu Y
- Zhu YX
- Zhu Z
- Ziegler A
- Zimmerman AB
- Zimmermann B
- Zimnukhov DS
- Ziolkowski M
- Zoll M
- Zong Z
- Zorn J
- Zornoza JD
- Zou CL
- Zuccarello F
- Zucker ME
- Zuniga J
- Zweizig J
- Zywucka N
- Publication venue
- 'American Astronomical Society'
- Publication date
- 01/01/2017
- Field of study
On 2017 August 17 a binary neutron star coalescence candidate (later designated GW170817) with merger time 12:41:04 UTC was observed through gravitational waves by the Advanced LIGO and Advanced Virgo detectors. The Fermi Gamma-ray Burst Monitor independently detected a gamma-ray burst (GRB 170817A) with a time delay of ~1.7 s with respect to the merger time. From the gravitational-wave signal, the source was initially localized to a sky region of 31 deg2 at a luminosity distance of 40+8-8 Mpc and with component masses consistent with neutron stars. The component masses were later measured to be in the range 0.86 to 2.26 Mo. An extensive observing campaign was launched across the electromagnetic spectrum leading to the discovery of a bright optical transient (SSS17a, now with the IAU identification of AT 2017gfo) in NGC 4993 (at ~40 Mpc) less than 11 hours after the merger by the One- Meter, Two Hemisphere (1M2H) team using the 1 m Swope Telescope. The optical transient was independently detected by multiple teams within an hour. Subsequent observations targeted the object and its environment. Early ultraviolet observations revealed a blue transient that faded within 48 hours. Optical and infrared observations showed a redward evolution over ~10 days. Following early non-detections, X-ray and radio emission were discovered at the transientâs position ~9 and ~16 days, respectively, after the merger. Both the X-ray and radio emission likely arise from a physical process that is distinct from the one that generates the UV/optical/near-infrared emission. No ultra-high-energy gamma-rays and no neutrino candidates consistent with the source were found in follow-up searches. These observations support the hypothesis that GW170817 was produced by the merger of two neutron stars in NGC4993 followed by a short gamma-ray burst (GRB 170817A) and a kilonova/macronova powered by the radioactive decay of r-process nuclei synthesized in the ejecta
The DUNE far detector vertical drift technology. Technical design report
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- Publication venue
- IOP Publishing
- Publication date
- 01/01/2024
- Field of study
DUNE is an international experiment dedicated to addressing some of the questions at the forefront of particle physics and astrophysics, including the mystifying preponderance of matter over antimatter in the early universe. The dual-site experiment will employ an intense neutrino beam focused on a near and a far detector as it aims to determine the neutrino mass hierarchy and to make high-precision measurements of the PMNS matrix parameters, including the CP-violating phase. It will also stand ready to observe supernova neutrino bursts, and seeks to observe nucleon decay as a signature of a grand unified theory underlying the standard model. The DUNE far detector implements liquid argon time-projection chamber (LArTPC) technology, and combines the many tens-of-kiloton fiducial mass necessary for rare event searches with the sub-centimeter spatial resolution required to image those events with high precision. The addition of a photon detection system enhances physics capabilities for all DUNE physics drivers and opens prospects for further physics explorations. Given its size, the far detector will be implemented as a set of modules, with LArTPC designs that differ from one another as newer technologies arise. In the vertical drift LArTPC design, a horizontal cathode bisects the detector, creating two stacked drift volumes in which ionization charges drift towards anodes at either the top or bottom. The anodes are composed of perforated PCB layers with conductive strips, enabling reconstruction in 3D. Light-trap-style photon detection modules are placed both on the cryostat's side walls and on the central cathode where they are optically powered. This Technical Design Report describes in detail the technical implementations of each subsystem of this LArTPC that, together with the other far detector modules and the near detector, will enable DUNE to achieve its physics goals
Performance of a modular ton-scale pixel-readout liquid argon time projection chamber
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- Publication venue
- MDPI
- Publication date
- 11/09/2024
- Field of study
The Module-0 Demonstrator is a single-phase 600 kg liquid argon time projection chamber operated as a prototype for the DUNE liquid argon near detector. Based on the ArgonCube design concept, Module-0 features a novel 80k-channel pixelated charge readout and advanced high-coverage photon detection system. In this paper, we present an analysis of an eight-day data set consisting of 25 million cosmic ray events collected in the spring of 2021. We use this sample to demonstrate the imaging performance of the charge and light readout systems as well as the signal correlations between the two. We also report argon purity and detector uniformity measurements and provide comparisons to detector simulations
Photoproduction of ETA mesons from hydrogen at photon energies between 0.8 and 1.45 GeV
- Author
- Publication venue
- Publication date
- 01/01/1968
- Field of study
We measured the differential cross section of the process Îłp â pÆ at the 1.5 GeV Caltech electron synchrotron, at photon energies from 0.8 to 1.45 GeV, at various angles between 45° and 100° in the center of mass. A counter-spark chamber array was used to determine the kinematics of all particles in the final state of the partial mode Îłp â pÆ (Æ â 2Îł). Analysis of 40,000 pictures yielded 6,000 events above a background which varied with energy from 5% to 30% of foreground. The cross section shows an energy dependence confirming earlier results up to 1000 MeV, but with improved statistics; it then remains roughly constant (at 50° C.M.), to 1.45 GeV. The data show a small angular variation, within the limited range covered, at energies between 1000 and 1100 MeV.</p
Notes/Notice
- Author
- Adlershof
- At a session of the Summer Meeting of the American Association for the Advancement of Science of which the Institute is an affiliated society the subject of
- Australia
- City Asas
- England
- Flugwesen Czechoslovakia
- France Canadian Aviation
- France L'Aerophile
- Germany Envoi
- Hours
- House
- Italy
- Mr Leon T
- Official Aviation Guide S. Dearborn St.
- Paris France
- Piccadilly London
- Politecnico Via
- Rd London
- Rochester Committee in charge of the arrangements for' the meeing are Dr. Walter Clark
- Rockets Through Space
- St
- Texas Sportsman Pilot
- Washington D. C.
- Western Flying S.
- Publication venue
- 'American Institute of Aeronautics and Astronautics (AIAA)'
- Publication date
- Field of study
- âŠ