27 research outputs found
Alignment of the ALICE Inner Tracking System with cosmic-ray tracks
- Author
- Aamodt K
- Abel N
- Abeysekara U
- Adamova D
- Aggarwal M
- Agocs AG
- Ahammed Z
- Ahmad A
- Ahmad N
- Ahn SU
- Akimoto R
- Akindinov A
- Aleksandrov D
- Alessandro B
- Alici A
- Alme J
- Alt T
- Altini V
- Altinpinar S
- Andrei C
- Andronic A
- Anelli G
- Angelov V
- Anson C
- Anticic T
- Antinori F
- Antinori S
- Antipin K
- Antonczyk D
- Antonioli P
- Anzo A
- Aphecetche L
- Appelshauser H
- Arcelli S
- Arceo R
- Arend A
- Armesto N
- Arnaldi R
- Aronsson T
- Arsene IC
- Asryan A
- Augustinus A
- Averbeck R
- Avina EA
- Awes TC
- Aysto J
- Azmi MD
- Bablok S
- Bach M
- Badala A
- Baek YW
- Bagnasco S
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Baldit A
- Ban J
- Barbera R
- Barile F
- Barnafoldi GG
- Barnby L
- Barret V
- Barroso VC
- Bartke J
- Basile M
- Basmanov V
- Bastid N
- Bathen B
- Batigne G
- Batyunya B
- Baumann C
- Bearden IG
- Becker B
- Belikov I
- Bellwied R
- Belmont-Moreno E
- Belogianni A
- Benhabib L
- Beole S
- Berceanu I
- Bercuci A
- Berdermann E
- Berdnikov Y
- Betev L
- Bhasin A
- Bhati AK
- Bianchi L
- Bianchi N
- Bianchin C
- Bielcik J
- Bielcikova J
- Bilandzic A
- Bimbot L
- Biolcati E
- Blanc A
- Blanco F
- Blanco F
- Blau D
- Blume C
- Boccioli M
- Bock N
- Bogdanov A
- Boggild H
- Bogolyubsky M
- Bohm J
- Boldizsar L
- Bombara M
- Bombonati C
- Bondila M
- Borel H
- Borisov A
- Borshchov V
- Bortolin C
- Bose S
- Bosisio L
- Bossu F
- Botje M
- Bottger S
- Bourdaud G
- Boyer B
- Braun M
- Braun-Munzinger P
- Bravina L
- Bregant M
- Breitner T
- Bruckner G
- Brun R
- Bruna E
- Bruno GE
- Budnikov D
- Buesching H
- Buncic P
- Busch O
- Buthelezi Z
- Caffarri D
- Cahuantzi MR
- Cai X
- Caines H
- Camacho E
- Camerini P
- Campbell M
- Capitani GP
- Carena F
- Carena W
- Carminati F
- Caselle M
- Castellanos JC
- Catanescu V
- Cattaruzza E
- Cavicchioli C
- Cerello P
- Cervantes IM
- Chambert V
- Chang B
- Chapeland S
- Charpy A
- Charvet JL
- Chattopadhyay S
- Chattopadhyay S
- Cherney M
- Cheshkov C
- Cheynis B
- Chiavassa E
- Chiesa AM
- Chinellato DD
- Chochula P
- Choi K
- Chojnacki M
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Chuman F
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Cobanoglu O
- Coffin JP
- Coli S
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- Contreras GJ
- Cormier TM
- Corral GH
- Cortese P
- Cosentino MR
- Costa F
- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
- Cunqueiro L
- Cussonneau J
- D'Erasmo G
- da Silva RSD
- Dainese A
- Dalsgaard HH
- Danu A
- Das I
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- Davalos AM
- de Barros GOV
- De Caro A
- de Cataldo G
- de Cuveland J
- De Falco A
- De Gaspari M
- de Groot J
- De Gruttola D
- de Guevara PL
- de Haas AP
- De Marco N
- de Matos CT
- De Pasquale S
- De Remigis R
- de Rooij R
- de Toledo AS
- de Vaux G
- del Valle ZC
- Delagrange H
- Dellacasa G
- Deloff A
- Demanov V
- Denes E
- Deppman A
- Derkach D
- Devaux A
- Di Bari D
- Di Giglio C
- Di Liberto S
- Di Mauro A
- Di Nezza P
- Dialinas M
- Diaz AC
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- Dietel T
- Ding H
- Divia R
- Djuvsland O
- Dobretsov V
- Dobrin A
- Dobrowolski T
- Dominguez I
- Don DMM
- Donigus B
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- Dubuisson J
- Ducroux L
- Dupieux P
- Elia D
- Emschermann D
- Enokizono A
- Espagnon B
- Estienne M
- Evans D
- Evrard S
- Eyyubova G
- Fabjan CW
- Fabris D
- Faivre J
- Falchieri D
- Fantoni A
- Fasel M
- Fateev O
- Fearick R
- Fedunov A
- Fehlker D
- Fekete V
- Felea D
- Fenton-Olsen B
- Feofilov G
- Ferreiro EG
- Ferretti A
- Ferretti R
- Figueredo MAS
- Filchagin S
- Fini R
- Fionda FM
- Fiore EM
- Floris M
- Fodor Z
- Foertsch S
- Foka Panagiota
- Fokin S
- Formenti F
- Fragiacomo E
- Fragkiadakis M
- Frankenfeld U
- Frolov A
- Fuchs U
- Furano F
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- Gaardhoje JJ
- Gadrat S
- Gagliardi M
- Gago A
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- Garabatos C
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- Gebelein J
- Gemme R
- Germain M
- Gheata A
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- Ghidini B
- Ghosh P
- Girard MF
- Giraudo G
- Giubellino P
- Gladysz-Dziadus E
- Glasow R
- Glassel P
- Glenn A
- Gomez R
- Gonzalez-Trueba LH
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- Gorbunov S
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- Gotovac S
- Gottschlag H
- Grabski V
- Grajcarek R
- Grelli A
- Grigoras A
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- Grigoriev V
- Grigoryan A
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- Grossiord JY
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- Guarnaccia C
- Guber F
- Guernane R
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- Gulbrandsen K
- Gulkanyan H
- Gunji T
- Gupta A
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- Gustafsson HA
- Gutbrod H
- Haaland O
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- Haiduc M
- Hamagaki H
- Hamar G
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- Hayrapetyan A
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- Helstrup H
- Herghelegiu A
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- Hrivnacova I
- Hu S
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- Huber S
- Humanic TJ
- Hutter D
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- Inaba M
- Innocenti PG
- Ippolitov M
- Irfan M
- Ivan C
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- Jacholkowski A
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- Jangal S
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- Jena C
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- Jirden L
- Jones GT
- Jones PG
- Jovanovic P
- Jung H
- Jung W
- Jusko A
- Kaidalov AB
- Kalcher S
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- Kalweit A
- Kamal A
- Kamermans R
- Kanaki K
- Kang E
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- Kapitan J
- Kaplin V
- Kapusta S
- Karavichev O
- Karavicheva T
- Karpechev E
- Kazantsev A
- Kebschull U
- Keidel R
- Khan MM
- Khan SA
- Khanzadeev A
- Kharlov Y
- Kikola D
- Kileng B
- Kim DJ
- Kim DS
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- Kim HN
- Kim J
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- Kim JS
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- Kim SH
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- Kirsch S
- Kisel I
- Kiselev S
- Kisiel A
- Klay JL
- Klein J
- Klein-Bosing C
- Kliemant M
- Klovning A
- Kluge A
- Kniege S
- Koch K
- Kolevatov R
- Kolojvari A
- Kondratiev V
- Kondratyeva N
- Konevskih A
- Kornas E
- Kour R
- Kowalski M
- Kox S
- Kozlov K
- Kral J
- Kralik I
- Kramer F
- Kraus I
- Kravcakova A
- Krawutschke T
- Krivda M
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- Krus M
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- Krzewicki M
- Kucheriaev Y
- Kuhn C
- Kuijer PG
- Kumar L
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- Laurenti G
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- Maevskaya A
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- Mastromarco M
- Mastroserio A
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- Mazza G
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- Meoni M
- Mereu P
- Miake Y
- Michalon A
- Miftakhov N
- Milosevic J
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- Viyogi YP
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- Vulpescu B
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- Willis N
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- Xu C
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- Yang H
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- Yermia F
- Yi J
- Yin Z
- Yokoyama H
- Yoo IK
- Yuan X
- Yurevich V
- Yushmanov I
- Zabrodin E
- Zagreev B
- Zalite A
- Zampolli C
- Zanevsky Y
- Zaporozhets S
- Zarochentsev A
- Zavada P
- Zbroszczyk H
- Zelnicek P
- Zenin A
- Zepeda A
- Zetina LM
- Zgura I
- Zhalov M
- Zhang X
- Zhou D
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- Zhu J
- Zichichi A
- Zinchenko A
- Zinovjev G
- Zoccarato Y
- Zychacek V
- Zynovyev M
- Publication venue
- Publication date
- 01/01/2010
- Field of study
37 pages, 15 figures, revised version, accepted by JINSTALICE (A Large Ion Collider Experiment) is the LHC (Large Hadron Collider) experiment devoted to investigating the strongly interacting matter created in nucleus-nucleus collisions at the LHC energies. The ALICE ITS, Inner Tracking System, consists of six cylindrical layers of silicon detectors with three different technologies; in the outward direction: two layers of pixel detectors, two layers each of drift, and strip detectors. The number of parameters to be determined in the spatial alignment of the 2198 sensor modules of the ITS is about 13,000. The target alignment precision is well below 10 micron in some cases (pixels). The sources of alignment information include survey measurements, and the reconstructed tracks from cosmic rays and from proton-proton collisions. The main track-based alignment method uses the Millepede global approach. An iterative local method was developed and used as well. We present the results obtained for the ITS alignment using about 10^5 charged tracks from cosmic rays that have been collected during summer 2008, with the ALICE solenoidal magnet switched off.Peer reviewe
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asawatavonvanich T
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
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- Chiu I
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
The ATLAS inner detector trigger performance in pp collisions at 13 TeV during LHC Run 2
- Author
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- Piegaia R
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- Pinfold JL
- Pino SAO
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- Pokharel I
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- Polifka R
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- Polychronakos V
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- Ponomarenko D
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- Popa S
- Popeneciu GA
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- Pownall G
- Pozo JAA
- Pralavorio P
- Prapa MM
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- Proklova N
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- Puri A
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- Ragusa F
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- Ravina B
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- Read AL
- Readioff NP
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- Rebuzzi DM
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- Reikher D
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- Renteria CG
- Resconi S
- Resseguie ED
- Rettie S
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- Rezanova OL
- Reznicek P
- Ricci E
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- Richter S
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- Rieck P
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- Rijssenbeek M
- Rimoldi A
- Rimoldi M
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- Ripellino G
- Riu I
- Rivadeneira P
- Rizatdinova F
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- Rossi LP
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- Rozen Y
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- Ruhr F
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- Rummler A
- Rurikova Z
- Rusakovich NA
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- Ruttinger EM
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- Sadrozinski HFW
- Sadykov R
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- Sanchez LP
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- Sanderswood IG
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- Sankey DPC
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- Schanet E
- Scharf C
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- Schegelsky VA
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- Schlenker S
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- Schmieden K
- Schmitt C
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- Schoening A
- Scholer PG
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schroeder F
- Schroeder TV
- Schulte A
- Schultz-Coulon HC
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schwemling P
- Schwienhorst R
- Sciandra A
- Sciolla G
- Scuri F
- Scutti F
- Scyboz LM
- Seabra LFO
- Sebastiani CD
- Sedlaczek K
- Seema P
- Seidel SC
- Seiden A
- Seidlitz BD
- Seiss T
- Seitz C
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- Sekhniaidze G
- Sekula SJ
- Semprini-Cesari N
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- Sforza F
- Sfyrla A
- Shabalina E
- Shahinian JD
- Shaikh NW
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- Sharma A
- Sharma AS
- Shatalov PB
- Shaw K
- Shaw SM
- Shehade M
- Shen Y
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- Shimogama Y
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- Shipsey IPJ
- Shirabe S
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- Shlomi J
- Shochet MJ
- Shojaii J
- Shope DR
- Shrestha S
- Shrif EM
- Shroff MJ
- Shulga E
- Sicho P
- Sickles AM
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silverstein SB
- Simion S
- Simoniello R
- Simpson-allsop CJ
- Simsek S
- Sinervo P
- Sinetckii V
- Singh S
- Sinha S
- Sioli M
- Sipio RD
- Siral I
- Sivoklokov SY
- Sjolin J
- Skaf A
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith EA
- Smith HA
- Smizanska M
- Smolek K
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- Snesarev AA
- Snoek HL
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- Sobie R
- Soffer A
- Sogaard A
- Sohns F
- Sola JDB
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Sonay A
- Song WY
- Sopczak A
- Sopio AL
- Sopkova F
- Sottocornola S
- Soualah R
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- South D
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- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spieker TM
- Spigo G
- Spina M
- Spiteri DP
- Spousta M
- Stabile A
- Stamas BL
- Stamen R
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- Stampekis A
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- Stanislaus B
- Stanitzki MM
- Stankaityte M
- Stapf B
- Starchenko EA
- Stark GH
- Stark J
- Staroba P
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- Starz S
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- Stavropoulos G
- Steinberg P
- Steinhebel AL
- Stelzer B
- Stelzer HJ
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- Stenzel H
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- Stewart GA
- Stockton MC
- Stoicea G
- Stolarski M
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strebler T
- Strizenec P
- Strohmer R
- Strom DM
- Stroud SV
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- Strubig A
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Su D
- Su W
- Su X
- Suarez NB
- Suarez RG
- Sulin VV
- Sullivan MJ
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suster CJE
- Sutton MR
- Svatos M
- Swiatlowski M
- Swift SP
- Swirski T
- Sydorenko A
- Sykora I
- Sykora M
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- Tagiev E
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- Talyshev AA
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- Tamir NM
- Tanaka J
- Tanaka R
- Tapprogge S
- Tarem S
- Tariq K
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tassi E
- Tateno G
- Tayalati Y
- Taylor GN
- Taylor W
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- Teixeira-Dias P
- Teoh JJ
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- Tikhonov YA
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- Tricoli A
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- Trincaz-Duvoid S
- Trischuk DA
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- Trocme B
- Trofymov A
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- Trovato F
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- Tsiareshka PV
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- Tsiskaridze V
- Tskhadadze EG
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- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tuna AN
- Turchikhin S
- Turgeman D
- Turner RJ
- Turra R
- Tuts PM
- Tzamarias S
- Tzovara E
- Uchida K
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- Unal G
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- Undrus A
- Unel G
- Ungaro FC
- Uno K
- Urban J
- Urban SC
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- Usai G
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vafeiadis T
- Vaidya A
- Valderanis C
- Vale MABD
- Vale TDD
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vannicola D
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vasquez GA
- Vazeille F
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Vera AMR
- Verbytskyi A
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vernieri C
- Verschuuren PJ
- Verzini MJA
- Vesterbacka ML
- Vetterli MC
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Villhauer EM
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
- Volpe DD
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vozak M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vu NK
- Vuillermet R
- Vukotic I
- Vulpen IV
- Wada S
- Wagner C
- Wagner P
- Wagner W
- Wahdan S
- Wahlberg H
- Wakasa R
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Walls FMG
- Wang AM
- Wang AZ
- Wang C
- Wang C
- Wang H
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- Wang RJ
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- Wang WT
- Wang WX
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- Wanotayaroj C
- Warburton A
- Ward CP
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- Webb AF
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- Weber SA
- Weber SM
- Wei Y
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wendland B
- Wengler T
- Wenig S
- Wermes N
- Wessels M
- Weston TD
- Whalen K
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams DM
- Williams HH
- Williams S
- Willocq S
- Windischhofer PJ
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolker R
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Wongel AF
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wuerzinger J
- Wyatt TR
- Wynne BM
- Xella S
- Xiang J
- Xiao X
- Xie X
- Xiotidis I
- Xu D
- Xu H
- Xu H
- Xu L
- Xu R
- Xu T
- Xu W
- Xu Y
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamatani M
- Yamauchi H
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang X
- Yang Y
- Yang Z
- Yao WM
- Yap YC
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zagazeta LFG
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Publication venue
- Publication date
- 01/01/2022
- Field of study
The design and performance of the inner detector trigger for the high level trigger of the ATLAS experiment at the Large Hadron Collider during the 2016-2018 data taking period is discussed. In 2016, 2017, and 2018 the ATLAS detector recorded 35.6 fb(-1), 46.9 fb(-1), and 60.6 fb(-1) respectively of proton-proton collision data at a centre-of-mass energy of 13TeV. In order to deal with the very high interaction multiplicities per bunch crossing expected with the 13TeV collisions the inner detector trigger was redesigned during the long shutdown of the Large Hadron Collider from 2013 until 2015. An overview of these developments is provided and the performance of the tracking in the trigger for the muon, electron, tau and b-jet signatures is discussed. The high performance of the inner detector trigger with these extreme interaction multiplicities demonstrates how the inner detector tracking continues to lie at the heart of the trigger performance and is essential in enabling the ATLAS physics programme
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at s√=13TeV
- Author
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- Zaffaroni E
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- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zgubič M
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
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- Zhang L
- Zhang M
- Zhang R
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- Zhang X
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Aizenberg I
- Akatsuka S
- Akbiyik M
- Akimov AV
- 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
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
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- Backman F
- Badea A
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- Bahilo JJL
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- Bailey AJ
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- Bartels F
- Bartoldus R
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- Casadei D
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- Casha AF
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- Castillo FL
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- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
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- Celebi E
- Celli F
- Centonze MS
- Cerny K
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- Cerri A
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- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chala M
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
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- Chen CH
- Chen H
- Chen H
- Chen J
- Chen J
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- Chen SJ
- Chen X
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- Chen Y
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- Cheng CL
- Cheng HC
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
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- Chowdhury T
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Ciaccio AD
- Ciaccio LD
- Cieri D
- Ciesla KM
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
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- Conroy EI
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- Cooke HG
- Cooper-Sarkar AM
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- Corpe LD
- Corradi M
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- Costanza F
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- Cote BM
- Coutinho YA
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- Cranmer K
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- Cristoforetti M
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- Cueto A
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- Curcio F
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- Czurylo MM
- Da Costa AMMJ
- da Costa JBG
- Da Cruz E Silva CB
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Daalen TRV
- Dabrowski W
- Dado T
- Dahbi S
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- Dam M
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- Dao V
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- Dawson I
- de Andrade Filho LM
- De Araujo MV
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- De Beurs M
- De Carvalho ALM
- De Castro S
- De Groot N
- de Jong P
- de la Hoz SG
- De la Torre H
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- De Maria A
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- de Renstrom PAB
- De Sa RCL
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- De Souza EEP
- De Vivie De Regie JB
- De K
- Dedovich DV
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- Delsart PA
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- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
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- Deviveiros PO
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- Diaz LP
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- Dodsworth D
- Doglioni C
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- Donaldson CP
- Donato CD
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- EUROPEAN PHYSICAL JOURNAL C
- Publication date
- 01/01/2022
- Field of study
This paper presents the measurement of the electroweak production of two jets
in association with a Zγ pair with the Z boson decaying into two
neutrinos. It also presents the search for invisible or partially invisible
decays of a Higgs boson with a mass of 125 GeV produced through vector-boson
fusion with a photon in the final state. These results use data from LHC
proton-proton collisions at s = 13 TeV collected with the ATLAS
detector corresponding to an integrated luminosity of 139 fb−1. The event
signature, shared by all benchmark processes considered for measurements and
searches, is characterized by a significant amount of unbalanced transverse
momentum and a photon in the final state, in addition to a pair of forward
jets. For electroweak production of Zγ in association with two jets, the
background-only hypothesis is rejected with an observed (expected) significance
of 5.2 (5.1) standard deviations. The measured fiducial cross-section for this
process is 1.31±0.29 fb. Observed (expected) upper limit of 0.37 (0.34) at
95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to
invisible particles, assuming the Standard Model production cross-section. The
signature is also interpreted in the context of decays of a Higgs boson to a
photon and a dark photon. An observed (expected) 95% CL upper limit on the
branching ratio for this decay is set at 0.018 (0.017), assuming the 125 GeV
Standard Model Higgs boson production cross-section
Midrapidity antiproton-to-proton ratio in pp collisons root s=0.9 and 7 TeV measured by the ALICE experiment
- Author
- Aamodt Kenneth
- Abel N
- Abeysekara U
- Abramyan A
- Adamová D
- Aggarwal MM
- Agocs AG
- Ahammed Z
- Ahmad A
- Ahmad N
- Ahn SU
- Akimoto R
- Akindinov A
- Aleksandrov D
- Alessandro B
- Alici A
- Alme Johan
- Alt T.
- Altini V
- Altinpinar S
- Andrei C
- Andronic A
- Anelli G
- Angelov V
- Anson C
- Anticic T
- Antinori F
- Antinori S
- Antipin K
- Antonczyk D
- Antonioli P
- Anzo A
- Aphecetche L
- Appelshauser SA
- Arcelli S
- Arceo R
- Arend A
- Armesto N
- Arnaldi R
- Aronsson T
- Arsene Ionut Christian
- Asryan A
- Augustinus A
- Averbeck R
- Avina EA
- Awes TC
- Aysto J
- Azmi MD
- Bablok Sebastian Robert
- Bach M
- Badala A
- Baek YW
- Bagnasco S
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisser A
- Baldit A
- Ban J
- Barbera R
- Barile F
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso VC
- Bartke J
- Basile M
- Basmanov V
- Bastid N
- Bathen B
- Batigne G
- Batyunya B
- Baumann C
- Bearden IG
- Becker B
- Belikov I
- Bellwied R
- Belmont-Moreno E
- Belogianni A
- Benhabib L
- Beole S
- Berceanu I
- Bercuci A
- Berdermann E
- Berdnikov Y
- Betev L
- Bhasin A
- Bhati AK
- Bianchi L
- Bianchi N
- Bianchin C
- Bielcik J
- Bielcikova J
- Bilandzic A
- Bimbot L
- Biolcati E
- Blanc A
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- Blau D
- Blume C
- Boccioli M
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- Bogdanov A
- Boggild H
- Bogolyubsky M
- Bohm J
- Boldizsar L
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- Borisov A
- Bortolin C
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- Bossu F
- Botje M
- Bottger S
- Bourdaud G
- Boyer B
- Braun M
- Braun-Munzinger P
- Bravina Larissa
- Bregant M
- Breitner T
- Bruckner G
- Brun R
- Bruna E
- Bruno GE
- Budnikov D
- Buesching H
- Buncic P
- Busch O
- Buthelezi Z
- Caffarri D
- Cahuantzi MR
- Cai X
- Caines H
- Calvo E
- Camacho E
- Camerini P
- Campbell M
- Capitani GP
- Carena F
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- Carminati F
- Caselle M
- Castellanos JC
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- Cavicchioli C
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- Chambert V
- Chang B
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- Chattopadhyay S
- Cherney M
- Cheshkov C
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- Chiavassa E
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- Chinellato DD
- Chochula P
- Choi K
- Chojnacki M
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Chuman F
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Cobanoglu O
- Coffin JP
- Coli S
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- Conner ES
- Constantin P
- Contin G
- Contreras JG
- Cormier TM
- Corral GH
- Cortese P
- Cosentino MR
- Costa F
- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
- Cunqueiro L
- Cussonneau J
- D'Erasmo G
- da Silva RSD
- Dainese A
- Dalsgaard HH
- Danu A
- Das I
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- Davalos AM
- de Barros GOV
- de Caro A
- de Cataldo G
- de Cuveland J
- De Falco A
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- de Groot J
- De Gruttola D
- de Guevara PL
- De Marco N
- de Matos CT
- De Pasquale S
- De Remigis R
- de Rooij R
- de Toledo AS
- de Vaux G
- del Valle ZC
- Delagrange H
- Delgado Y
- Dellacasa G
- Deloff A
- Demanov V
- Denes E
- Deppman A
- Derkach D
- Devaux A
- Di Bari D
- Di Giglio C
- Di Liberto S
- Di Mauro A
- Di Nezza P
- Dialinas M
- Diaz AC
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- Dietel T
- Divia R
- Djuvsland Øystein
- Dobretsov V
- Dobrin A
- Dobrowolski T
- Dominguez I
- Don DMM
- Donigus B
- Dordic Olja
- Dubey AK
- Dubuisson J
- Ducroux L
- Dupieux P
- Elia D
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- Enokizono A
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- Eyyubova Gyulnara
- Fabjan CW
- Fabris D
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- Fehlker Dominik
- Fekete V
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- Feofilov G
- Ferreiro EG
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- Filchagin S
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- Tsiledakis G
- Tsilis E
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- Turvey A
- Tveter Trine Spedstad
- Tydesjo H
- Tywoniuk Konrad
- Ulery J
- Ullaland Kjetil
- Uras A
- Urban J
- Urciuoli GM
- Usai GL
- Vacchi A
- Vala M
- Vallero S
- van der Kolk N
- van Leeuwen M
- Vannucci L
- Vargas A
- Vargas HL
- Varma R
- Vasileiou M
- Vasiliev A
- Vasquez MAS
- Vassiliev I
- Vechernin V
- Velasquez AO
- Venaruzzo M
- Vercellin E
- Vergara S
- Vernet R
- Verweij M
- Vetlitskiy I
- Vickovic L
- Viesti G
- Vikhlyantsev O
- Vilakazi Z
- Vinogradov A
- Vyvre PV
- Wagner Boris
- Wikne Jon Christopher
- Zabrodin Evgeny
- Zetina LM
- Øvrebekk Gaute
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 09/10/2017
- Field of study
The ratio of the yields of antiprotons to protons in pp collisions has been measured by the ALICE experiment at root s = 0.9 and 7 TeV during the initial running periods of the Large Hadron Collider. The measurement covers the transverse momentum interval 0.45 < p(t) < 1.05 GeV/c and rapidity vertical bar y vertical bar < 0.5. The ratio is measured to be R-vertical bar y vertical bar<0.5 = 0.957 +/- 0.006(stat) +/- 0.0014(syst) at 0.9 Tev and R-vertical bar y vertical bar<0.5 = 0.991 +/- 0.005 +/- 0.014(syst) at 7 TeV and it is independent of both rapidity and transverse momentum. The results are consistent with the conventional model of baryon-number transport and set stringent limits on any additional contributions to baryon-number transfer over very large rapidity intervals in pp collisions
Two-pion Bose-Einstein correlations in pp collisions at root s=900 GeV
- Author
- Aamodt K
- Abel N
- Abeysekara U
- Abramyan A
- Adamova D
- Aggarwal MM
- Agocs AG
- Ahammed Z
- Ahmad A
- Ahmad N
- Ahn SU
- Akimoto R
- Akindinov A
- Aleksandrov D
- Alessandro B
- ALICE Collaboration
- Alici A
- Alme J
- Alt T
- Altini V
- Altinpinar S
- Andrei C
- Andronic A
- Anelli G
- Angelov V
- Anson C
- Anticic T
- Antinori S
- Antipin K
- Antonczyk D
- Antonioli P
- Anzo A
- Aphecetche L
- Appelshauser H
- Arcelli S
- Arceo R
- Arend A
- Armesto N
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- Arsene IC
- Asryan A
- Augustinus A
- Averbeck R
- Avina EA
- Awes TC
- Aysto J
- Azmi MD
- Bablok S
- Bach M
- Badala A
- Baek YW
- Bagnasco S
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
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- Baldit A
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- Barbera R
- Barile F
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso VC
- Bartke J
- Basile M
- Basmanov V
- Bastid N
- Bathen B
- Batigne G
- Batyunya B
- Baumann C
- Bearden IG
- Becker B
- Belikov I
- Bellwied R
- Belmont Moreno E
- Belogianni A
- Benhabib L
- Beole S
- Berceanu I
- Bercuci A
- Berdermann E
- Berdnikov Y
- Betev L
- Bhasin A
- Bhati AK
- Bianchi L
- Bianchi N
- Bianchin C
- Bielcik J
- Bielcikova J
- Bilandzic A
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- Biolcati E
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- Boccioli M
- Bock N
- Bogdanov A
- Boggild H
- Bogolyubsky M
- Bohm J
- Boldizsar L
- Bombara M
- Bombonati C
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- Borel H
- Borisov A
- Bortolin C
- Bose S
- Bosisio L
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- Boyer B
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- Braun Munzinger P
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- Bruckner G
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- Budnikov D
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- Buncic P
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- Buthelezi Z
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- Cahuantzi MR
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- Caines H
- Calvo E
- Camacho E
- Camerini P
- Campbell M
- Capitani GP
- Carena F
- Carena W
- Carminati F
- Caselle M
- Castellanos JC
- Catanescu V
- Cattaruzza E
- Cavicchioli C
- Cerello P
- Cervantes IM
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- Cherney M
- Cheshkov C
- Cheynis B
- Chiavassa E
- Chiesa AM
- Chinellato DD
- Chochula P
- Choi K
- Chojnacki M
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Chuman F
- Cicalo C
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- Coffin JP
- Coli S
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- Conner ES
- Constantin P
- Contin G
- Contreras JG
- Cormier TM
- Corral GH
- Cortese P
- Cosentino MR
- Costa F
- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
- Cunqueiro L
- Cussonneau J
- D'Erasmo G
- da Silva RSD
- Dainese A
- Dalsgaard HH
- Danu A
- Das I
- Dash A
- Dash S
- Davalos AM
- de Barros GOV
- De Caro A
- de Cataldo G
- de Cuveland J
- De Falco A
- De Gaspari M
- de Groot J
- De Gruttola D
- de Guevara PL
- De Marco N
- de Matos CT
- De Pasquale S
- De Remigis R
- De Rooij R
- de Toledo AS
- de Vaux G
- del Valle ZC
- Delagrange H
- Delgado Y
- Dellacasa G
- Deloff A
- Demanov V
- Denes E
- Deppman A
- Derkach D
- Devaux A
- Di Bari D
- DI BARI Domenico
- Di Giglio C
- Di Liberto S
- Di Mauro A
- Di Nezza P
- Dialinas M
- Diaz AC
- Diaz L
- Diaz R
- Dietel T
- Divia R
- Djuvsland O
- Dobretsov V
- Dobrin A
- Dobrowolski T
- Dominguez I
- Don DMM
- Donigus B
- Dordic O
- Dubey AK
- Dubuisson J
- Ducroux L
- Dupieux P
- Elia D
- Emschermann D
- Enokizono A
- Espagnon B
- Estienne M
- Esumi S
- Evans D
- Evrard S
- Eyyubova G
- Fabjan CW
- Fabris D
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- Falchieri D
- Fantoni A
- Fasel M
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- Fearick R
- Fedunov A
- Fehlker D
- Fekete V
- Felea D
- Fenton Olsen B
- Feofilov G
- Ferreiro EG
- Ferretti A
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- Figueredo MAS
- Filchagin S
- Fini R
- Fionda FM
- Fiore EM
- Floris M
- Fodor Z
- Foertsch S
- Foka P
- Fokin S
- Formenti F
- Fragiacomo E
- Fragkiadakis M
- Frankenfeld U
- Frolov A
- Fuchs U
- Furano F
- Furget C
- Gaardhoje JJ
- Gadrat S
- Gagliardi M
- Gago A
- Gallio M
- Ganoti P
- Ganti MS
- Garabatos C
- Garcia GM
- Gebelein J
- Gemme R
- Germain M
- Gheata A
- Gheata M
- Ghidini B
- Ghosh P
- Girard MF
- Giraudo G
- Giubellino P
- Gladysz Dziadus E
- Glasow R
- Glassel P
- Glenn A
- Gonzalez Trueba LH
- Gonzalez Zamora P
- Gorbunov S
- Gorbunov Y
- Gotovac S
- Gottschlag H
- Grabski V
- Grajcarek R
- Grelli A
- Grigoras A
- Grigoras C
- Grigoriev V
- Grigoryan A
- Grigoryan S
- Grinyov B
- Grion N
- Gros P
- Grosse Oetringhaus JF
- Grossiord JY
- Grosso R
- Guber F
- Guernane R
- Guerra C
- Guerzoni B
- Gulbrandsen K
- Gulkanyan H
- Gunji T
- Gupta A
- Gupta R
- Gustafsson HA
- Gutbrod H
- Haaland O
- Hadjidakis C
- Haiduc M
- Hamagaki H
- Hamar G
- Hamblen J
- Han BH
- Harris JW
- Hartig M
- Harutyunyan A
- Hasch D
- Hasegan D
- Hatzifotiadou D
- Hayrapetyan A
- Heide M
- Heinz M
- Helstrup H
- Herghelegiu A
- Hernandez C
- Hernandez JFC
- Hernandez MIM
- Herrmann N
- Hetland KF
- Hicks B
- Hiei A
- Hille PT
- Hippolyte B
- Horaguchi T
- Hori Y
- Hristov P
- Hrivnacova I
- Hu S
- Huang M
- Huber S
- Humanic TJ
- Hutter D
- Hwang DS
- Ichou R
- Ilkaev R
- Ilkiv I
- Inaba M
- Innocenti PG
- Ippolitov M
- Irfan M
- Ivan C
- Ivanov A
- Ivanov M
- Ivanov V
- Iwasaki T
- Jacholkowski A
- Jacobs P
- Jancurova L
- Jangal S
- Janik R
- Jena C
- Jena S
- Jimenez RG
- Jirden L
- Jones GT
- Jones PG
- Jovanovic P
- Jung H
- Jung W
- Jusko A
- Kaidalov AB
- Kalcher S
- Kalinak P
- Kalisky M
- Kalliokoski T
- Kalweit A
- Kamal A
- Kamermans R
- Kanaki K
- Kang E
- Kang JH
- Kapitan J
- Kaplin V
- Kapusta S
- Karavichev O
- Karavicheva T
- Karpechev E
- Kazantsev A
- Kebschull U
- Keidel R
- Khan MM
- Khan SA
- Khanzadeev A
- Kharlov Y
- Kikola D
- Kileng B
- Kim DJ
- Kim DS
- Kim DW
- Kim HN
- Kim J
- Kim JH
- Kim JS
- Kim M
- Kim M
- Kim S
- Kim SH
- Kim Y
- Kirsch S
- Kisel I
- Kiselev S
- Kisiel A
- Klay JL
- Klein Bosing C
- Klein J
- Kliemant M
- Klovning A
- Kluge A
- Knichel ML
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- Yokoyama H
- Yoo IK
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- Yushmanov I
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- Zarochentsev A
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- Zbroszczyk H
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- Zepeda A
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- Zgura I
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- Zhou S
- Zhu J
- Zichichi A
- Zinchenko A
- Zinovjev G
- Zoccarato Y
- Zychacek V
- Zynovyev M.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2010
- Field of study
We report on the measurement of two-pion correlation functions from pp collisions at root s = 900 GeV performed by the ALICE experiment at the Large Hadron Collider. Our analysis shows an increase of the Hanbury Brown-Twiss radius with increasing event multiplicity, in line with other measurements done in particle- and nuclear collisions. Conversely, the strong decrease of the radius with increasing transverse momentum, as observed at the Relativistic Heavy Ion Collider and at Tevatron, is not manifest in our data
Midrapidity Antiproton-to-Proton Ratio in pp Collisons root s=0.9 and 7 TeV Measured by the ALICE Experiment
- Author
- Aamodt K
- Abel N
- Abeysekara U
- Abramyan A
- Adamova D
- Aggarwal MM
- Agocs AG
- Ahammed Z
- Ahmad A
- Ahmad N
- Ahn SU
- Akimoto R
- Akindinov A
- Aleksandrov D
- Alessandro B
- Alici A
- Alme J
- Alt T
- Altini V
- Altinpinar S
- Andrei C
- Andronic A
- Andronic A
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- Angelov V
- Anson C
- Anticic T
- Antinori F
- Antinori S
- Antipin K
- Antonczyk D
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- Appelshauser SA
- Arcelli S
- Arceo R
- Arend A
- Armesto N
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- Aronsson T
- Arsene IC
- Asryan A
- Augustinus A
- Averbeck R
- Avina EA
- Awes TC
- Aysto J
- Azmi MD
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- Badala A
- Baek YW
- Bagnasco S
- Bailhache R
- Baillie OV
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- Belogianni A
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- Berceanu I
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- Berdermann E
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- Cheshkov C
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- Chinellato DD
- Chochula P
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- Christakoglou P
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- Cicalo C
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- Hippolyte B
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- Hrivnacova I
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- Humanic TJ
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- Ichou R
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- Ilkiv I
- Inaba M
- Innocenti PG
- Ippolitov M
- Irfan M
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- Ivanov A
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- Iwasaki T
- Jacholkowski A
- Jacobs P
- Jancurova L
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- Jimenez RG
- Jirden L
- Jones GT
- Jones PG
- Jovanovic P
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- Jung W
- Jusko A
- Kaidalov AB
- Kalcher S
- Kalinak P
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- Kalliokoski T
- Kalweit A
- Kamal A
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- Kanaki K
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- Kang JH
- Kapitan J
- Kaplin V
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- Karavichev O
- Karavicheva T
- Karpechev E
- Kazantsev A
- Kebschull U
- Keidel R
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- Khanzadeev A
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- Kisel I
- Kiselev S
- Kisiel A
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- Kliemant M
- Klovning A
- Kluge A
- Knichel ML
- Kniege S
- Koch K
- Kolevatov R
- Kolojvari A
- Kondratiev V
- Kondratyeva N
- Konevskih A
- Kornas E
- Kour R
- Kowalski M
- Kox S
- Kozlov K
- Kral J
- Kralik I
- Kramer F
- Kraus I
- Kravcakova A
- Krawutschke T
- Krivda M
- Krumbhorn D
- Krus M
- Kryshen E
- Krzewicki M
- Kucheriaev Y
- Kuhn C
- Kuijer PG
- Kumar L
- Kumar N
- Kupczak R
- Kurashvili P
- Kurepin A
- Kurepin AN
- Kuryakin A
- Kushpil S
- Kushpil V
- Kutouski M
- Kvaerno H
- Kweon MJ
- Kwon Y
- La Rocca P
- Lackner F
- Lafage V
- Lal C
- Lara C
- Larsen DT
- Laurenti G
- Lazzeroni C
- Le Bornec Y
- Le Bris N
- Lee H
- Lee KS
- Lee SC
- Lefevre F
- Lehnert J
- Leistam L
- Lenhardt M
- Lenti V
- Leon H
- Lerma PLMP
- Levai P
- Li X
- Li Y
- Lietava R
- Lindal S
- Lindenstruth V
- Lippmann C
- Lisa MA
- Liu L
- Loginov V
- Lohn S
- Lopez SR
- Lopez X
- Lopez-Ramirez R
- Lorenzo PM
- Lovhoiden G
- Lu S
- Lunardon M
- Luparello G
- Luquin L
- Lutz JR
- Ma K
- Ma R
- Madagodahettige-Don DM
- Maevskaya A
- Mager M
- Mahapatra DP
- Maire A
- Majumdar AKD
- Majumdar MRD
- Makhlyueva I
- Mal'Kevich D
- Malaev M
- Malagalage KJ
- Maldonado IC
- Malek M
- Malkiewicz T
- Malzacher P
- Mamonov A
- Manceau L
- Mangotra L
- Manko V
- Manso F
- Manzari V
- Mao Y
- Mares J
- Margagliotti GV
- Margotti A
- Marin A
- Martashvili I
- Martinengo P
- Maruyama Y
- Masciocchi S
- Masera M
- Masetti M
- Masoni A
- Massacrier L
- Mastromarco M
- Mastroserio A
- Matthews ZL
- Matyja A
- Mayani D
- Mazza G
- Mazzoni MA
- Meddi F
- Menchaca-Rocha A
- Meoni M
- Mereu P
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- Zinovjev G
- Zoccarato Y
- Zychacek V
- Zynovyev M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 26/11/2015
- Field of study
Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)The ratio of the yields of antiprotons to protons in pp collisions has been measured by the ALICE experiment at root s = 0.9 and 7 TeV during the initial running periods of the Large Hadron Collider. The measurement covers the transverse momentum interval 0.45 < p(t) < 1.05 GeV/c and rapidity vertical bar y vertical bar < 0.5. The ratio is measured to be R-vertical bar y vertical bar<0.5 = 0.957 +/- 0.006(stat) +/- 0.0014(syst) at 0.9 Tev and R-vertical bar y vertical bar<0.5 = 0.991 +/- 0.005 +/- 0.014(syst) at 7 TeV and it is independent of both rapidity and transverse momentum. The results are consistent with the conventional model of baryon-number transport and set stringent limits on any additional contributions to baryon-number transfer over very large rapidity intervals in pp collisions.1057Calouste Gulbenkian Foundation from LisbonConselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)Financiadora de Estudos e Projetos (FINEP)Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)National Natural Science Foundation of China (NSFC)Chinese Ministry of Education (CMOE)Ministry of Science and Technology of China (MSTC)Ministry of Education and Youth of the Czech RepublicDanish Natural Science Research CouncilCarlsberg FoundationDanish National Research FoundationThe European Research CouncilHelsinki Institute of PhysicsAcademy of FinlandFrench CNRS-IN2P3Region Pays de LoireRegion AlsaceRegion AuvergneCEA, FranceGerman BMBFHelmholtz AssociationHungarian OTKANational Office for Research and Technology (NKTH)Department of Atomic EnergyDepartment of Science and Technology of the Government of IndiaIstituto Nazionale di Fisica Nucleare (INFN) of ItalyMEXT, JapanJoint Institute for Nuclear Research, DubnaKorea Foundation for International Cooperation of Science and Technology (KICOS)CONACYTDGAPA, MexicoALFA-ECHELEN Program (High-Energy physics Latin-American-European Network)Stichting voor Fundamenteel Onderzoek der Materie (FOM)Nederlandse Organisatie voor Wetenschappelijk Onderzoek (NWO), The NetherlandsResearch Council of Norway (NFR)Polish Ministry of Science and Higher EducationNational Authority for Scientific Research-NASR (Autontatea Nationala pentru Cercetare Stiintifica-ANCS)Federal Agency of Science of the Ministry of Education and Science of Russian FederationInternational Science and Technology CenterRussian Academy of SciencesRussian Federal Agency of Atomic EnergyRussian Federal Agency for Science and InnovationsCERN-INTASMinistry of Education of SlovakiaCIEMATEELAMinisterio de Educacion y Ciencia of SpainXunta de Galicia (Conselleria de Educacion)CEADENCubaenergia, CubaIAEA (International Atomic Energy Agency)Swedish Reseach CouncilKnut & Alice Wallenberg FoundationUkraine Ministry of Education and ScienceUnited Kingdom Science and Technology Facilities Council (STFC)The United States Department of EnergyUnited States National Science Foundation, State of TexasSwiss Fonds Kidagan, ArmeniaUnited States National Science Foundation, the State of OhioConselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP
Gamma-aminobutyric acid uptake and the termination of inhibitory synaptic potentials in the rat hippocampal slice.
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- Publication venue
- Publication date
- 01/09/1985
- Field of study
Intracellular recordings were made from CA1 pyramidal cells in the rat hippocampal slice to study the processes that influence the time course of inhibitory post-synaptic potentials (i.p.s.p.s) mediated by gamma-aminobutyric acid (GABA), and conductance changes evoked by ionophoretically applied GABA. The GABA-uptake inhibitors, nipecotic acid and cis-4-OH-nipecotic acid (1 mM), greatly prolonged conductance increases associated with both hyperpolarizing and depolarizing responses to ionophoretically applied GABA. In contrast to their effects on GABA-evoked conductances, uptake inhibitors only slightly prolonged antidromically evoked i.p.s.p.s. Their primary effect occurred after the i.p.s.p. had decayed to 5-30% of its peak. 4-OH-isonipecotic acid, a nipecotic acid analogue that does not inhibit GABA uptake, did not prolong i.p.s.p.s or ionophoretically evoked conductance changes. Sodium pentobarbitone (100 microM), a drug that prolongs the open time of GABA-activated chloride channels, potentiated both i.p.s.p.s and responses to ionophoretically applied GABA. Whereas pentobarbitone also prolonged i.p.s.p.s, it did not prolong responses to ionophoretically applied GABA. The prolongation of i.p.s.p.s by pentobarbitone occurred equally in both the early and late phases of the i.p.s.p., in contrast to the effects of GABA-uptake inhibitors. I.p.s.p.s did not usually decay exponentially. The observation that uptake inhibitors prolonged the late but not the early decay phase of the i.p.s.p., together with the previous finding that the conductance change persists for the duration of the i.p.s.p., indicate that GABA is present in the synapse throughout much of the i.p.s.p. These data suggest that diffusion of GABA out of the synapse, a non-exponential process, is an important determinant of the i.p.s.p. decay time course. Increasing the extracellular potassium concentration from 3.5 to 8.5 mM resulted in spontaneously occurring, synchronous burst firing of pyramidal cells. Cis-4-OH-nipecotic acid significantly reduced the number and amplitude of extracellularly recorded population spikes within each burst. We conclude that diffusion, channel open time and GABA uptake all influence the time course of GABA-mediated i.p.s.p.s. The time course of a single, brief i.p.s.p. is determined predominantly by post-synaptic channel kinetics and diffusion of GABA out of the synapse, whereas the inhibition produced by prolonged synaptic bursts or relatively long application of exogenous GABA can be markedly influenced by GABA uptake.(ABSTRACT TRUNCATED AT 400 WORDS