6 research outputs found
Radiation Treatment of Cutaneous T-Cell Lymphomas: Indian Experience
- Author
- A Funk
- A Kuten
- A Neri
- A Ranki
- AG Liceta
- AS Whittemore
- B Micaily
- BA Pancake
- BJ Nickoloff
- BJ Nickoloff
- CE Introcaso
- CJ Karzmark
- D Faj
- DG Merwe Van Der
- DK Parida
- DK Parida
- DK Parida
- E Diamandidou
- E Tuyp
- EA Abel
- EH Epstein
- G Jones
- GS Wood
- GS Wood
- GW Cotter
- GW Jones
- GW Jones
- GW Jones
- GW Jones
- GW Jones
- GW Jones
- HK Koh
- JC Brouet
- JG Trump
- JH Kim
- JL Haybittle
- L Ysebaert
- LG Blasic
- LM Weiss
- LZ Nisce
- M Becker
- MA Lutzner
- MA Weinstock
- MA Weinstock
- MH Green
- MM Reavely
- NL Harris
- P Heald
- P Heald
- P Heald
- P Heald
- PA Quiros
- PA Quiros
- PR Bergtresser
- R Edelson
- R Edelson
- RM Marti
- RT Hoppe
- RT Hoppe
- RT Hoppe
- RT Hoppe
- RT Hoppe
- RT Hoppe
- S Reddy
- SA Buchner
- SB Green
- TCM Lo
- TS Kupper
- V Manzari
- WA Vloten Van
- WC Dewey
- WE Lever
- WL Macaulay
- YH Kim
- Z Fuks
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
PHENIX central arm tracking detectors
- Author
- Adcox K
- Ajitanand NN
- Alexander J
- Autrey D
- Averbeck R
- Azmoun B
- Barish KN
- Baublis VV
- Belkin R
- Bhaganatula S
- Biggs JC
- Borland D
- Botelho S
- Bryan WL
- Burward-Hoy J
- Butsyk SA
- Chang WC
- Christ T
- Dietzsch O
- Drees A
- du Rietz Rickard
- El Chenawi K
- Evseev VA
- Fellenstein J
- Ferdousi T
- Fraenkel Z
- Franz A
- Fung SY
- Gannon J
- Garpman Sten
- Godoi AL
- Green SV
- Gustafsson Hans-Åke
- Harder J
- Hemmick TK
- Heuser JM
- Holzmann W
- Hutter R
- Issah M
- Ivanov VI
- Jacak BV
- Jagadish U
- Jia J
- Johnson SC
- Kandasamy A
- Kann MR
- Kelley MA
- Khanzadeev AV
- Khomutnikov A
- Komkov BG
- Kopytine ML
- Kotchenda L
- Kotchetkov D
- Kozlov VS
- Kravtsov PA
- Kudin LG
- Kuriatkov VV
- Lacey R
- Lauret J
- Lebedev A
- Lebedev VD
- Li XH
- Libby B
- Liccardi W
- Machnowski R
- Mahon J
- Markushin DG
- Matathias F
- Messer F
- Miftakhov NM
- Milan J
- Miller TE
- Milov A
- Minuzzo K
- Mioduszewski S
- Mitchell JT
- Muniruzzamann M
- Nandi BK
- Negrin J
- Nilsson Pål
- Nystrand J
- O'Brien E
- O'Connor P
- Oskarsson Anders
- Otterlund Ingvar
- Pancake CE
- Pantuev VS
- Petersen R
- Pinkenburg CH
- Pisani RP
- Purwar AK
- Rankowitz S
- Ravinovich I
- Riabov VG
- Riabov YG
- Rosati M
- Roschin EV
- Rose AA
- Samsonov VM
- Sangster TC
- Seto R
- Silvermyr David
- Sivertz M
- Smith M
- Solodov GP
- Stenlund Evert
- Takagui EM
- Tarakanov VI
- Tarasenkova OP
- Thomas JL
- Trofimov VA
- Tserruya I
- Tydesjö Henrik
- Velkovska J
- Velkovsky M
- Vishnevskii VI
- Vorobyov AA
- Vznuzdaev EA
- Vznuzdaev M
- Wang HQ
- Weimer T
- Wolniewicz K
- Wu J
- Xie W
- Young GR
- Österman Lennart
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2003
- Field of study
The PHENIX tracking system consists of Drift Chambers (DC), Pad Chambers (PC) and the Time Expansion Chamber (TEC). PC1/DC and PC2/TEC/PC3 form the inner and outer tracking units, respectively. These units link the track segments that transverse the RICH and extend to the EMCal. The DC measures charged particle trajectories in the r-phi direction to determine P-T of the particles and the invariant mass of particle pairs. The PCs perform 3D spatial point measurements for pattern recognition and longitudinal momentum reconstruction and provide spatial resolution of a few mm in both r-phi and z. The TEC tracks particles passing through the region between the RICH and the EMCal. The design and operational parameters of the detectors are presented and running experience during the first year of data taking with PHENIX is discussed. The observed spatial and momentum resolution is given which imposes a limitation on the identification and characterization of charged particles in various momentum ranges. (C) 2002 Published by Elsevier Science B.V
PHENIX on-line systems
- Author
- Adler SS
- Allen M
- Alley G
- Amirikas R
- Arai Y
- Awes TC
- Barish KN
- Barta F
- Batsouli S
- Belikov S
- Bennett MJ
- Bobrek M
- Boissevain JG
- Boose S
- Britton C
- Britton L
- Bryan WL
- Cafferty MM
- Carey TA
- Chang WC
- Chi CY
- Chi M
- Cianciolo V
- Cole BA
- Constantin P
- Cook KC
- Cunitz H
- Desmond EJ
- Ebisu K
- Efremenko YV
- El Chenawi K
- Emery MS
- Engo D
- Ericson N
- Fields DE
- Frank S
- Frantz JE
- Franz A
- Frawley AD
- Fried J
- Gannon J
- Gee TF
- Gentry R
- Giannotti P
- Gustafsson Hans-Åke
- Haggerty JS
- Hahn S
- Halliwell J
- Hamagaki H
- Hansen AG
- Hara H
- Harder J
- He X
- Heistermann F
- Hemmick TK
- Hibino M
- Hill JC
- Homma K
- Jacak BV
- Jagadish U
- Jia J
- Kajihara F
- Kametani S
- Kamyshkov Y
- Kandasamy A
- Kang JH
- Kapustinsky J
- Katou K
- Kelley MA
- Kelly S
- Kikuchi J
- Kim SY
- Kim YG
- Kistenev E
- Kotchetkov D
- Kurita K
- Lajoie JG
- Lenz M
- Lenz W
- Li XH
- Lin S
- Liu MX
- Markacs S
- Matathias F
- Matsumoto T
- Mead J
- Mischke RE
- Mishra GC
- Moore A
- Muniruzzamann M
- Musrock M
- Nagle JL
- Nandi BK
- Newby J
- Nystrand Joakim
- O'Brien E
- O'Connor P
- Ohnishi H
- Oskarsson Anders
- Oyama K
- Paffrath L
- Pancake CE
- Pantuev VS
- Petridis AN
- Pisani RP
- Plagge T
- Plasil F
- Purschke ML
- Rankowitz S
- Rao R
- Rau M
- Read KF
- Ryu SS
- Sakaguchi T
- Sato HD
- Seto R
- Shiina T
- Silvermyr David
- Simon-Gillo J
- Simpson M
- Sippach W
- Skank HD
- Skutnik S
- Sleege GA
- Smith GD
- Smith M
- Stankus PW
- Steinberg P
- Sugitate T
- Sullivan JP
- Taketani A
- Tamai M
- Tanaka Y
- Thomas WD
- Todd R
- Toldo F
- Turner G
- Ushiroda T
- van Hecke HW
- Van Lith M
- Velkovska J
- Villatte L
- Von Achen W
- Walker JW
- Wang HQ
- White SN
- Wintenberg AL
- Witzig C
- Wood L
- Xie W
- Young GR
- Zajc WA
- Zhang C
- Zhang L
- Österman Lennart
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2003
- Field of study
The PHENIX On-Line system takes signals from the Front End Modules (FEM) on each detector subsystem for the purpose of generating events for physics analysis. Processing of event data begins when the Data Collection Modules (DCM) receive data via fiber-optic links from the FEMs. The DCMs format and zero suppress the data and generate data packets. These packets go to the Event Builders (EvB) that assemble the events in final form. The Level-1 trigger (LVL1) generates a decision for each beam crossing and eliminates uninteresting events. The FEMs carry out all detector processing of the data so that it is delivered to the DCMs using a standard format. The FEMs also provide buffering for LVL1 trigger processing and DCM data collection. This is carried out using an architecture that is pipelined and deadtimeless. All of this is controlled by the Master Timing System (MTS) that distributes the RHIC clocks. A Level-2 trigger (LVL2) gives additional discrimination. A description of the components and operation of the PHENIX On-Line system is given and the solution to a number of electronic infrastructure problems are discussed. (C) 2002 Elsevier Science B.V. All rights reserved
PHENIX detector overview
- Author
- Adcox K
- Adler SS
- Aizama M
- Ajitanand NN
- Akiba Y
- Akikawa H
- Al-Jamel A
- Alexander J
- Allen M
- Alley G
- Amirikas R
- Aphecetche L
- Arai Y
- Archuleta JB
- Archuleta JR
- Armendariz R
- Armijo V
- Aronson SH
- Autrey D
- Averbeck R
- Awes TC
- Azmoun B
- Baldisseri A
- Banning J
- Barish KN
- Barker AB
- Barnes PD
- Barrette J
- Barta F
- Bassalleck B
- Bathe S
- Batsouli S
- Baublis VV
- Bazilevsky A
- Begay R
- Behrendt J
- Belikov S
- Belkin R
- Bellaiche FG
- Belyaev ST
- Bennett MJ
- Berdnikov Y
- Bhaganatula S
- Biggs JC
- Bland AW
- Blume C
- Bobrek M
- Boissevain JG
- Boose S
- Borel H
- Borland D
- Bosze E
- Botelho S
- Bowers J
- Britton C
- Britton L
- Brooks ML
- Brown AW
- Brown DS
- Bruner N
- Bryan WL
- Bucher D
- Buesching H
- Bumazhnov V
- Bunce G
- Burward-Hoy J
- Butsyk SA
- Cafferty MM
- Carey TA
- Chai JS
- Chand P
- Chang J
- Chang WC
- Chappell RB
- Chavez LL
- Chernichenko S
- Chiba J
- Chiu CY
- Chiu M
- Chollet S
- Choudhury RK
- Christ T
- Chujo T
- Chung MS
- Chung P
- Cianciolo V
- Clark DJ
- Cobigo Y
- Cole BA
- Constantin P
- Conway R
- Cook KC
- Crook DW
- Cunitz H
- Cunningham R
- Cutshaw M
- D'Enterria DG
- Dabrowski CM
- Danby G
- Daniels S
- Danmura A
- David G
- de Cassagnac RG
- Debraine A
- Delagrange H
- DeMoss J
- Denisov A
- Deshpande A
- Desmond EJ
- Dietzsch O
- Dinesh BV
- Drachenberg JL
- Drapier O
- Drees A
- du Rietz Rickard
- Durum A
- Dutta D
- Ebisu K
- Echave MA
- Efremenko YV
- El Chenawi K
- Emery MS
- En'yo H
- Engo D
- Enokizono A
- Enosawa K
- Ericson N
- Esumi S
- Evseev VA
- Ewell L
- Fackler O
- Fellenstein J
- Ferdousi T
- Ferrierra J
- Fields DE
- Fleuret F
- Fokin SL
- Fox B
- Fraenkel Z
- Frank S
- Frantz JE
- Franz A
- Frawley AD
- Freidberg JP
- Fried J
- Fujisawa E
- Funahashi H
- Fung SY
- Gadrat S
- Gannon J
- Garpman Sten
- Gastaldi F
- Gee TF
- Gentry R
- Ghosh TK
- Giannotti P
- Glenn A
- Godoi AL
- Gogiberidze G
- Gonin M
- Gosset J
- Goto Y
- Greene SV
- Griffin V
- Gupta SK
- Guryn W
- Gustafsson Hans-Åke
- Hachiya T
- Haggerty JS
- Hahn S
- Halliwell J
- Hamagaki H
- Hance RH
- Hansen AG
- Hara H
- Harder J
- Hart GW
- Hartouni EP
- Harvey A
- Hawkins L
- Hayano RS
- Hayashi H
- Hayashi N
- He X
- Heine N
- Heistermann F
- Held S
- Hemmick TK
- Heuser JM
- Hibino M
- Hicks JS
- Higuchi R
- Hill JC
- Hirano T
- Ho DS
- Hoade R
- Holzmann W
- Homma K
- Honaguchi T
- Hong B
- Hoover A
- Hunter CT
- Hurst DE
- Hutter R
- Ichihara T
- Ikonnikov VV
- Imai K
- Inaba M
- Ippolitov MS
- Isenhower LD
- Isenhower LD
- Ishihara M
- Issah M
- Ivanov VI
- Jacak BV
- Jackson G
- Jackson J
- Jaffe D
- Jagadish U
- Jang WY
- Jayakumar R
- Jia J
- Johnson BM
- Johnson J
- Johnson SC
- Jones JP
- Jones K
- Joo KS
- Jouan D
- Kahn S
- Kajihara F
- Kametani S
- Kamihara N
- Kamyshkov Y
- Kandasamy A
- Kang JH
- Kann MR
- Kapoor SS
- Kapustinsky J
- Karadjev KV
- Kashikhin V
- Kato S
- Katou K
- Kehayias HJ
- Kelley MA
- Kelly S
- Kennedy M
- Khachaturov B
- Khanzadeev AV
- Khomutnikov A
- Kikuchi J
- Kim DJ
- Kim DW
- Kim GB
- Kim HJ
- Kim SY
- Kim YG
- Kinnison WW
- Kistenev E
- Kiyomichi A
- Klein-Boesing C
- Klinksiek S
- Kluberg L
- Kobayashi H
- Kochetkov V
- Koehler D
- Kohama T
- Komkov BG
- Kopytine ML
- Koseki K
- Kotchenda L
- Kotchetkov D
- Koutcheryaev IA
- Kozlov A
- Kozlov VS
- Kravtsov PA
- Kroon PJ
- Kuberg CH
- Kudin LG
- Kurata-Nishimura M
- Kuriatkov VV
- Kurita K
- Kuroki Y
- Kweon MJ
- Kwon Y
- Kyle GS
- LaBounty JJ
- Lacey R
- Lajoie JG
- Lauret J
- Lebedev A
- Lebedev VA
- Lebedev VD
- Lee DM
- Lee S
- Leitch M
- Lenz M
- Lenz W
- Li XH
- Li Z
- Libby B
- Libkind M
- Liccardi W
- Lim DJ
- Lin S
- Liu MX
- Liu X
- Liu Y
- Liu Z
- Lockner E
- Longbotham N
- Lopez JD
- Machnowski R
- Maguire CF
- Mahon J
- Makdisi YI
- Manko VI
- Mao Y
- Marino S
- Mark SK
- Markacs S
- Markushin DG
- Martinez G
- Martinez XB
- Marx MD
- Masaike A
- Matathias F
- Matsumoto T
- McCain MC
- McGaughey PL
- Mead J
- Melnikov E
- Melnikov Y
- Meng WZ
- Merschmeyer M
- Messer F
- Messer M
- Miake Y
- Miftakhov NM
- Migluolio S
- Milan J
- Miller TE
- Milov A
- Minuzzo K
- Mioduszewski S
- Mischke RE
- Mishra GC
- Mitchell JT
- Miyamoto Y
- Mohanty AK
- Montoya BC
- Moore A
- Moore T
- Morrison DP
- Moscone GG
- Moss JM
- Muhlbacher F
- Muniruzzaman M
- Murata J
- Murray MM
- Musrock M
- Nagamiya S
- Nagasaka Y
- Nagle JL
- Nakada Y
- Nakamura T
- Nandi BK
- Negrin J
- Newby J
- Nikkinen L
- Nikolaev SA
- Nilsson Pål
- Nishimura S
- Nyanin AS
- Nystrand Joakim
- O'Brien E
- O'Conner P
- Obenshain F
- Ogilvie CA
- Ohnishi H
- Ojha ID
- Ono M
- Onuchin V
- Oskarsson Anders
- Otterlund Ingvar
- Oyama K
- Paffrath L
- Palounek APT
- Pancake CE
- Pantuev VS
- Papavassiliou V
- Pate SF
- Peitzmann T
- Perdekamp MG
- Petersen R
- Petridis AN
- Pinkenburg CH
- Pisani RP
- Pitukhin P
- Plagge T
- Plasil F
- Pollack M
- Pope K
- Prigl R
- Purschke ML
- Purwar AK
- Qualls JM
- Rankowitz S
- Rao G
- Rao R
- Rau M
- Ravinovich I
- Raynis R
- Read KF
- Reygers K
- Riabov G
- Riabov VG
- Riabov YG
- Robinson SH
- Roche G
- Romana A
- Rosati M
- Roschin EV
- Rose AA
- Rosnet P
- Roth R
- Ruggiero R
- Ryu SS
- Saito N
- Sakaguchi A
- Sakaguchi T
- Sakai S
- Sako H
- Sakuma T
- Salomone S
- Samsonov VM
- Sandhoff WF
- Sanfratello L
- Sangster TC
- Santo R
- Sato HD
- Sato S
- Savino R
- Sawada S
- Schlei BR
- Schleuter R
- Schutz Y
- Sekimoto M
- Semenov V
- Seto R
- Severgin Y
- Shajii A
- Shangin V
- Shaw MR
- Shea TK
- Shein I
- Shelikhov V
- Shibata TA
- Shigaki K
- Shiina T
- Shimada T
- Shin YH
- Sibiriak IG
- Silvermyr David
- Sim KS
- Simon-Gillo J
- Simpson M
- Singh CP
- Singh V
- Sippach W
- Sivertz M
- Skank HD
- Skutnik S
- Sleege GA
- Smith DC
- Smith GD
- Smith M
- Soldatov A
- Solodov GP
- Soltz RA
- Sondheim WE
- Sourikova I
- Staley F
- Stankus PW
- Starinsky N
- Steffens S
- Stein EM
- Steinberg P
- Stenlund Evert
- Stepanov M
- Ster A
- Stewering J
- Stokes W
- Stoll SP
- Sugioka M
- Sugitate T
- Sullivan JP
- Sumi Y
- Sun Z
- Suzuki-Nara M
- Sörensen Stacey
- Takagui EM
- Taketani A
- Tamai M
- Tanaka KH
- Tanaka Y
- Taniguchi E
- Tannenbaum MJ
- Tarakanov VI
- Tarasenkova OP
- Tepe JD
- Thern R
- Thomas JH
- Thomas JL
- Thomas TL
- Thomas WD
- Thornton GW
- Tian W
- Todd R
- Tojo J
- Toldo F
- Torii H
- Towell RS
- Tradeski J
- Trofimov VA
- Tserruya I
- Tsuruoka H
- Tsvetkov AA
- Tulli SK
- Turner G
- Tydesjö Henrik
- Tyurin N
- Urasawa S
- Usachev A
- Ushiroda T
- van Hecke HW
- Van Lith M
- Vasiliev AA
- Vasiliev V
- Vassent M
- Velissaris C
- Velkovska J
- Velkovsky M
- Verhoeven W
- Villatte L
- Vinogradov AA
- Vishnevskii VI
- Volkov MA
- Von Achen W
- Vorobyov AA
- Vznuzdaev EA
- Vznuzdaev M
- Walker JW
- Wan Y
- Wang HQ
- Wang S
- Watanabe Y
- Watkins LC
- Weimer T
- White SN
- Whitus BR
- Williams C
- Willis PS
- Wintenberg AL
- Witzig C
- Wohn FK
- Wolniewicz K
- Wong-Swanson BG
- Wood L
- Woody CL
- Wright LW
- Wu J
- Xie W
- Xu N
- Yagi K
- Yamamoto R
- Yang Y
- Yokkaichi S
- Yokota Y
- Yoneyama S
- Young GR
- Yushmanov IE
- Zajc WA
- Zhang C
- Zhang L
- Zhang Z
- Zhou S
- Österman Lennart
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2003
- Field of study
The PHENIX detector is designed to perform a broad study of A-A, p-A, and p-p collisions to investigate nuclear matter under extreme conditions. A wide variety of probes, sensitive to all timescales, are used to study systematic variations with species and energy as well as to measure the spin structure of the nucleon. Designing for the needs of the heavy-ion and polarized-proton programs has produced a detector with unparalleled capabilities. PHENIX measures electron and muon pairs, photons, and hadrons with excellent energy and momentum resolution. The detector consists of a large number of subsystems that are discussed in other papers in this volume. The overall design parameters of the detector are presented. (C) 2002 Elsevier Science B.V. All rights reserved
The ATLAS experiment at the CERN Large Hadron Collider: a description of the detector configuration for Run 3
- Author
- Aad G
- Abbott B
- Abbott DC
- Abdallah J
- Abeling K
- Abidi SH
- Aboulhorma A
- Abovyan S
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akhperjanyan G
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Alkakhi W
- Allaire C
- Allard J
- Allbrooke BMM
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Gonzalez B
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amor Dos Santos SP
- Amos KR
- Ananiev V
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antonescu M
- Antrim DJA
- Anulli F
- Aoki M
- Aoki T
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Appelt C
- Aranzabal N
- Araujo Ferraz V
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyris A
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armijo CE
- Arnaez O
- Arnold H
- Arrubarrena Tame ZP
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Assahsah J
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Aubernon E
- Augsten K
- Aune S
- Auricchio S
- Auriol AD
- Aust F
- Austrup VA
- Avner G
- Avolio G
- Avoni G
- Axen D
- Axiotis K
- Aydiner P
- Ayoub MK
- Azaryan T
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahmani M
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Bakos E
- Bakshi Gupta D
- Balaji S
- Balasubramanian R
- Balbi G
- Baldin EM
- Balek P
- Ball R
- Ballabene E
- Ballansat J
- Balli F
- Baltes LM
- Balunas WK
- Balz J
- Ban J
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- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cavaliere V
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- Cavasinni V
- Celebi E
- Celli F
- Centonze MS
- Ceradini F
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- Cherepanova E
- Cherkaoui El Moursli R
- Cheu E
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- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
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- Zorbas TG
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- Zullo A
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- IOP Publishing
- Publication date
- 01/05/2024
- Field of study
Abstract
The ATLAS detector is installed in its experimental cavern
at Point 1 of the CERN Large Hadron Collider. During Run 2 of the
LHC, a luminosity of
ℒ = 2 × 1034 cm-2 s-1 was
routinely achieved at the start of fills, twice the design
luminosity. For Run 3, accelerator improvements, notably luminosity
levelling, allow sustained running at an instantaneous luminosity of
ℒ = 2 × 1034 cm-2 s-1,
with an average of up to 60 interactions per bunch crossing. The
ATLAS detector has been upgraded to recover Run 1 single-lepton
trigger thresholds while operating comfortably under Run 3 sustained
pileup conditions. A fourth pixel layer 3.3 cm from the beam axis
was added before Run 2 to improve vertex reconstruction and
b-tagging performance. New Liquid Argon Calorimeter digital
trigger electronics, with corresponding upgrades to the Trigger and
Data Acquisition system, take advantage of a factor of 10 finer
granularity to improve triggering on electrons, photons, taus, and
hadronic signatures through increased pileup rejection. The inner
muon endcap wheels were replaced by New Small Wheels with Micromegas
and small-strip Thin Gap Chamber detectors, providing both precision
tracking and Level-1 Muon trigger functionality. Trigger coverage of
the inner barrel muon layer near one endcap region was augmented
with modules integrating new thin-gap resistive plate chambers and
smaller-diameter drift-tube chambers. Tile Calorimeter scintillation
counters were added to improve electron energy resolution and
background rejection. Upgrades to Minimum Bias Trigger Scintillators
and Forward Detectors improve luminosity monitoring and enable total
proton-proton cross section, diffractive physics, and heavy ion
measurements. These upgrades are all compatible with operation in
the much harsher environment anticipated after the High-Luminosity
upgrade of the LHC and are the first steps towards preparing ATLAS
for the High-Luminosity upgrade of the LHC. This paper describes
the Run 3 configuration of the ATLAS detector.</jats:p
Recommended from our members
The ATLAS experiment at the CERN Large Hadron Collider: a description of the detector configuration for Run 3
- Author
- Aad G
- Abbott B
- Abbott DC
- Abdallah J
- Abeling K
- Abidi SH
- Aboulhorma A
- Abovyan S
- Abramowicz H
- Abreu H
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- Abusleme Hoffman AC
- Acharya BS
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- Addepalli SV
- Adelman J
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- Castillo Gimenez V
- Castillo FL
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Journal of Instrumentation
- Publication date
- 23/05/2024
- Field of study
Abstract
The ATLAS detector is installed in its experimental cavern
at Point 1 of the CERN Large Hadron Collider. During Run 2 of the
LHC, a luminosity of
ℒ = 2 × 1034 cm-2 s-1 was
routinely achieved at the start of fills, twice the design
luminosity. For Run 3, accelerator improvements, notably luminosity
levelling, allow sustained running at an instantaneous luminosity of
ℒ = 2 × 1034 cm-2 s-1,
with an average of up to 60 interactions per bunch crossing. The
ATLAS detector has been upgraded to recover Run 1 single-lepton
trigger thresholds while operating comfortably under Run 3 sustained
pileup conditions. A fourth pixel layer 3.3 cm from the beam axis
was added before Run 2 to improve vertex reconstruction and
b-tagging performance. New Liquid Argon Calorimeter digital
trigger electronics, with corresponding upgrades to the Trigger and
Data Acquisition system, take advantage of a factor of 10 finer
granularity to improve triggering on electrons, photons, taus, and
hadronic signatures through increased pileup rejection. The inner
muon endcap wheels were replaced by New Small Wheels with Micromegas
and small-strip Thin Gap Chamber detectors, providing both precision
tracking and Level-1 Muon trigger functionality. Trigger coverage of
the inner barrel muon layer near one endcap region was augmented
with modules integrating new thin-gap resistive plate chambers and
smaller-diameter drift-tube chambers. Tile Calorimeter scintillation
counters were added to improve electron energy resolution and
background rejection. Upgrades to Minimum Bias Trigger Scintillators
and Forward Detectors improve luminosity monitoring and enable total
proton-proton cross section, diffractive physics, and heavy ion
measurements. These upgrades are all compatible with operation in
the much harsher environment anticipated after the High-Luminosity
upgrade of the LHC and are the first steps towards preparing ATLAS
for the High-Luminosity upgrade of the LHC. This paper describes
the Run 3 configuration of the ATLAS detector.</jats:p