154 research outputs found
Search for High-Mass Resonances Decaying to ÏÎœ in pp Collisions at âs=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya S Tapia
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME Pozo
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Bakker PJ
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee Sw
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
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- Barillari T
- Barisits M-S
- Barkeloo JT
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- Barreiro Guimaraes da Costa J
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- Bartoldus R
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- Batista SJ
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- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beattie MD
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- Beauchemin PH
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- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
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- Bee CP
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- Behera A
- Behr JK
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- Bellerive A
- Bellomo M
- Belotskiy K
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen J Montejo
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- Bernius C
- Bernlochner FU
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- Bertella C
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- Besjes GJ
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- Besson N
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- Betti A
- Bevan AJ
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- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz NV
- Biglietti M
- Billoud TRV
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- Bingul A
- Bini C
- Biondi S
- Bisanz T
- Bittrich C
- Bjergaard DM
- Black JE
- Black KM
- Blair RE
- Blazek T
- Bloch I
- Blocker C
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- Blumenschein U
- Blunier Dr
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boeriu OE Vickey
- Boerner D
- Bogavac D
- Bogdanchikov AG
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- Bomben M
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- Bonilla JS
- Boonekamp M
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- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Boscherini D
- Bosman M
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
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- Boveia A
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- Boyko IR
- Bozson AJ
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- Brau JE
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- Brennan AJ
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- Bret M Cano
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- Bristow TM
- Britton D
- Britzger D
- Brock I
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- Brooijmans G
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- Broughton JH
- Bruncko D
- Bruni A
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- Brunt BH
- Bruschi M
- Bruscino N
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- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher D
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- Bugge MK
- Bulekov O
- Bullock D
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burka K
- Burke S
- Burmeister I
- Burr JTP
- Buschmann E
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund O Bessidskaia
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir I Turk
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
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- Calvet TP
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- Camarda S
- Camarri P
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- Camincher C
- Campana S
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- Camplani A
- Campoverde A
- Canale V
- Cantero J
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- Caprini I
- Caprini M
- Capua M
- Carbone RM
- Cardarelli R
- Cardillo F
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo LR Flores
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Chavez Barajas CA
- Che S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen C
- Chen H
- Chen J
- Chen J
- Chen S
- Chen S
- Chen X
- Chen Y
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Christodoulou V
- Chu MC
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Cinca D
- Cindro V
- Cioara IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
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- Clement C
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- Coccaro A
- Cochran J
- Colasurdo L
- Cole B
- Colijn AP
- Collaboration ATLAS
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- Conde Muino P
- Coniavitis E
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Corga K De Vasconcelos
- Cormier F
- Cormier KJR
- Cornell S Diez
- Corradi M
- Correia AM Henriques
- Corrigan EE
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- Costa MJ
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- Cottin G
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- Crane J
- Cranmer K
- Crawley SJ
- Creager RA
- Cree G
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- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cukierman AR
- Curatolo M
- Cuth J
- Czekierda S
- Czodrowski P
- D'amen G
- D'Auria S
- D'eramo L
- D'Onofrio M
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dale O
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio D Oliveira
- Dandoy JR
- Daneri MF
- Dang NP
- Dann NS
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dartsi O
- Dattagupta A
- Daubney T
- Davey W
- David C
- Davidek T
- Davis DR
- Dawe E
- Dawson I
- de Asmundis R
- De Benedetti A
- De Bruin PH Sales
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DE Ferreira
- De Lorenzi F
- De Maria A
- De Pedis D
- De Regie JB De Vivie
- de Renstrom PA Bruckman
- De Salvo A
- De Sanctis U
- De Santo A
- De K
- Debenedetti C
- Dedovich DV
- Dehghanian N
- Del Gaudio M
- Del Peso J
- Delgove D
- Deliot F
- Delitzsch CM
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- della Volpe D
- Delmastro M
- Delporte C
- Delsart PA
- DeMarco DA
- Demers S
- Demichev M
- Denisov SP
- Denysiuk D
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Devesa MR
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Micco B
- Di Nardo R
- Di Petrillo KF
- Di Simone A
- Di Sipio R
- Di Valentino D
- Diaconu C
- Diamond M
- Dias do Vale T
- Dias FA
- Diaz MA
- Dickinson J
- Diehl EB
- Dietrich J
- Dimitrievska A
- Dingfelder J
- Dittus F
- Djama F
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- Djuvsland JI
- do Vale MAB
- Dobre M
- Dodsworth D
- Doglioni C
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- Dolezal Z
- Donadelli M
- Donini J
- Donszelmann T Cuhadar
- Dopke J
- Doria A
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
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- Dris M
- Du Y
- Duarte-Campderros J
- Dubinin F
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducourthial A
- Ducu OA
- Duda D
- Dudarev A
- Dudder A Chr
- Duehrssen M
- Dueren M
- Duffield EM
- Duflot L
- Dulsen C
- Dumancic M
- Dumitriu AE
- Duncan AK
- Dunford M
- Duperrin A
- Durglishvili A
- Duschinger D
- Dutta B
- Duvnjak D
- Dyndal M
- Dziedzic BS
- Eckardt C
- Ecker KM
- Edgar RC
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Kosseifi R
- El Moursli R Cherkaoui
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
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- Elmsheuser J
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- Enari Y
- Ennis JS
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- Escalier M
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- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Favareto A
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedorko W
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- Feigl S
- Feligioni L
- Feng C
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- Fenyuk AB
- Feremenga L
- Ferrando J
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- Fiolhais MCN
- Fiorini L
- Fischer C
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- Fleck I
- Fleischmann P
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- Flierl BM
- Flores LM
- Foerster FA
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- Formica A
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- Zivkovic L
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- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to ÏÎœ using proton-proton collisions at âs=13 TeV produced by the Large Hadron Collider is presented. Only Ï-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fbâ1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible ÏÎœ production cross section. Heavy WâČ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2â3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Search for the direct production of charginos and neutralinos in final states with tau leptons in âs=13 TeV collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Alconada Verzini MJ
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- Aleksandrov IN
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- Yigitbasi E
- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
- Young C
- Young CJS
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- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
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- Zalieckas J
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- Zanzi D
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- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
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- Zhao Z
- Zhemchugov A
- Zhou B
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- Zhou N
- Zhu CG
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- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
A search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fbâ1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ËÏ+1 ËÏâ1 pair production and of Ëϱ1 ËÏ02 and ËÏ+1 ËÏâ1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the Ë ÏL state is set to be halfway between the masses of the Ëϱ1 and the ËÏ01. Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ËÏ+1 ËÏâ1 for a massless ËÏ01. Common Ëϱ1 and ËÏ02 masses up to 760 GeV are excluded in the case of production of Ëϱ1 ËÏ02 and ËÏ+1 ËÏâ1 assuming a massless ËÏ01. Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the Ëϱ1 and the ËÏ01 are also studied by varying the Ë ÏL mass between the masses of the Ëϱ1 and the ËÏ01
Combined measurement of differential and total cross sections in the HâŻââŻÎłÎł and the HâŻââŻZZ*âŻââŻ4â decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouzeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlas Collaboration
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Bakshi Gupta D
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro GuimarĂŁes Da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
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- Ălvarez Piqueras D
- Ă kesson TPA
- Ć filigoj T
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fbâ1 of 13 TeV protonâproton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured Hâγγ and HâZZ*(â4â event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0â5.9 +6.0 (stat.) â3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Measurement of differential cross sections and W + /W â cross-section ratios for W boson production in association with jets at âs =8 TeV with the ATLAS detector
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
This paper presents a measurement of the W boson production cross section and the W + /W â cross-section ratio, both in association with jets, in proton--proton collisions at s â =8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb â1 . Differential cross sections for events with one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles and the missing transverse momentum in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W + /W â the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proto
Measurement of the cross section for inclusive isolated-photon production in pp collisions at âs=13TeV using the ATLAS detector
- Author
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- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier E
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf' TMH
- Wolf A
- Wolff R
- Wolter MW
- Wolters H
- Wong KHY
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wotschack J
- Wozniak KW
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu L
- Xu T
- Xu W
- Yabsley B
- Yacooba S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Inclusive isolated-photon production in pp collisions at a centre-of-mass energy of 13TeVis studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 3.2fbâ1. The cross section is measured as a function of the photon transverse energy above 125GeVin different regions of photon pseudorapidity. Next-to-leading-order perturbative QCD and Monte Carlo event-generator predictions are compared to the cross-section measurements and provide an adequate description of the data
Operation and performance of the ATLAS Tile Calorimeter in Run 1
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouelfadl 
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez 
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor 
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Argos FC
- Arguin J-
- Argyropoulos S
- Armadans R
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME
- Atkin RJ
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- AÌlvarez Piqueras D
- AÌkesson TPA
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahilo JJL
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
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- Baldin EM
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- Balunas WK
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- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M
- Barkeloo J
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
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- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro GuimaraÌes da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batlamous S
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
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- Bessidskaia Bylund O
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- Biglietti M
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- Bindi M
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- Biswal JP
- Bittrich C
- Bjergaard DM
- Black JE
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- Bloch I
- Blocker C
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- Blunier D
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- Bocchetta SS
- Bocci A
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- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
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- Boldyrev AS
- Bolz AE
- Bomben M
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- Bostanabad M
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- Boumediene D
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- Boutle SK
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- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt A
- Brandt G
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- Braren F
- Bratzler U
- Brau B
- Brau JE
- Breaden Madden WD
- Brendlinger K
- Brennan AJ
- Brenner L
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- Brock I
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- Brown H
- Bruckman de Renstrom PA
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
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- Bulekov O
- Bullock D
- Burch TJ
- Burdin S
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- Burka K
- Burke S
- Burmeister I
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- Buschmann E
- Bussey P
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- Butterworth JM
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- Buttinger W
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- BuÌhrer F
- BuÌscher D
- BuÌscher V
- Cabras G
- Cabrera UrbaÌn S
- Caforio D
- Cai H
- Cairo VMM
- Cakir I
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarri P
- Cameron D
- Caminal 
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Cano Bret M
- Cantero J
- Cao T
- Cao Y
- Capeans Garrido MDM
- Caprini I
- Caprini M
- Capua M
- Carbone RM
- Cardarelli R
- Cardillo FC
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- CarraÌ S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
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- Chakraborty D
- Chan SK
- Chan WS
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- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Chavez Barajas CA
- Che S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y
- Chen Y
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Christodoulou V
- Chu MC
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Ciaccio A
- Ciaccio L
- Cinca D
- Cindro V
- CioaraÌ IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Clark A
- Clark MR
- Clark PJ
- Clement C
- Clemente WK
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Coimbra AEC
- Colasurdo L
- Cole B
- Colijn AP
- Collot J
- Conde MuinÌo P
- Coniavitis E
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Cormier F
- Cormier KJR
- Corradi M
- Correia AM
- Corrigan EE
- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
- Costanzo D
- Cottin G
- Cowan G
- Cox BE
- Crane J
- Cranmer K
- Crawley SJ
- Creager RA
- Cree G
- Crescioli F
- CreÌpeÌ-Renaudin S
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cuhadar Donszelmann T
- Cukierman AR
- Cunha 
- Curatolo M
- CuÌth J
- Czekierda S
- Czodrowski P
- Da Via C
- Da 
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallaire F
- Dallapiccola C
- Dam M
- Damp J
- Dandoy JR
- Daneri MF
- Dang NP
- Dann ND
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dartsi O
- Dattagupta A
- Daubney T
- Davey W
- David C
- Davidek T
- Davis DR
- Davydov Y
- Dawe E
- Dawson I
- De Asmundis R
- De Benedetti A
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- De Lorenzi F
- De Maria A
- De Moura 
- De Pedis D
- De Salvo A
- De Sanctis U
- De Santo A
- De Vasconcelos Corga K
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- De 
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- De K
- Debenedetti C
- Dedovich DV
- Dehghanian N
- Del Gaudio M
- Del Peso J
- Delgado A
- Delgove D
- Deliot F
- Delitzsch CM
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- Della Volpe D
- DellâAcqua A
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- Delmastro M
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- Demers S
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- Denisov SP
- Denysiuk D
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
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- Deviveiros PO
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- Dickinson J
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- Dietrich J
- Dimitrievska A
- Dingfelder J
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- Dodsworth D
- Doglioni C
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- Du Y
- Duarte-Campderros J
- Dubinin F
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducourthial A
- Ducu OA
- Duda D
- Dudarev A
- Dudder AC
- Duffield EM
- Duflot L
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- Dumitriu AE
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- Duran 
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- DuÌlsen C
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- Dysch S
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- Dâamen G
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- Ecker KM
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- Ekelof T
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- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
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- Elmsheuser J
- Elsing M
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- Enari Y
- Ennis JS
- Epland MB
- Erdmann J
- Ereditato A
- Errede S
- Escalier M
- Escobar C
- Esposito B
- Estrada 
- Etienvre AI
- Etzion E
- Evans H
- Ezhilov A
- Ezzi M
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- Fabiani V
- Facini G
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- Falke PJ
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- Fanti M
- Farbin A
- Farilla A
- Farina EM
- Farooque T
- Farrell S
- Farrington SM
- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Faucci Giannelli M
- Favareto A
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedorko W
- Feickert M
- Feigl S
- Feligioni L
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- Fenyuk AB
- Feremenga L
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- Ferreira de Lima DE
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- Zwalinski L
- ZÌenisÌ T
- ZÌivkovicÌ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The Tile Calorimeter is the hadron calorimeter covering the central region of the ATLAS experiment at the Large Hadron Collider. Approximately 10,000 photomultipliers collect light from scintillating tiles acting as the active material sandwiched between slabs of steel absorber. This paper gives an overview of the calorimeterâs performance during the years 2008â2012 using cosmic-ray muon events and protonâproton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fbâ1. The signal reconstruction methods, calibration systems as well as the detector operation status are presented. The energy and time calibration methods performed excellently, resulting in good stability of the calorimeter response under varying conditions during the LHC Run 1. Finally, the Tile Calorimeter response to isolated muons and hadrons as well as to jets from protonâproton collisions is presented. The results demonstrate excellent performance in accord with specifications mentioned in the Technical Design Report
Study of ordered hadron chains with the ATLAS detector
- Author
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- McDonald EF
- Mcfayden JA
- Mchedlidze G
- McMahon SJ
- McNamara PC
- McPherson RA
- Meehan S
- Megy TJ
- Mehlhase S
- Mehta A
- Meideck T
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- Mellenthin JD
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- Mengarelli A
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- Milic A
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- Minaenko AA
- Minami Y
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- Mizukami A
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- Onogi K
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- Oppen H
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- Oren Y
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- Osculati B
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- Otono H
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- Outschoorn VI Martinez
- Ouyang Q
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- Pacheco Pages A
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- Rusakovich NA
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- Sanchez FJ Munoz
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- Santurio E Valdes
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- Schaffer AC
- Schaile D
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- Schillo C
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- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
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- Schnoor U
- Schoeffel L
- Schoening A
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- Schopf E
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- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schroeder T Vazquez
- Schuh N
- Schulte A
- Schultens MJ
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune Ph
- Schwartzman A
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- Schweiger H
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- Schwienhorst R
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- Sciandra A
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- Seidel SC
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- Semprini-Cesari N
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- Sforza F
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- Shabalina E
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- Shehu CY
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- Shimizu S
- Shimmin CO
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- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet MJ
- Shojaii S
- Shope DR
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- Shulga E
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- Sidebo PE
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- Sidoti A
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- Simak V
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- Simion S
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- Simon M
- Sinervo P
- Sinev NB
- Sioli M
- Siragusa G
- Siral I
- Sivoklokov S Yu
- Sjolin J
- Skinner MB
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov S Yu
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith JW
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snyder IM
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- Sobie R
- Socher F
- Soffer A
- Sogaard A
- Soh DA
- Sokhrannyi G
- Solar M
- Soldatov E Yu
- Soldevila U
- Solis A Lopez
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Sopczak A
- Sosa D
- Sotiropoulou CL
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spettel F
- Spieker TM
- Spighi R
- Spigo G
- Spiller LA
- Spousta M
- Stabile A
- Stamen R
- Stamm S
- Stanecka E
- Stanek RW
- Stanescu C
- Stanitzki MM
- Stapf BS
- Stapnes S
- Starchenko EA
- Stark GH
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- Staroba P
- Starovoitov P
- Starz S
- Staszewski R
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- Stelzer-Chilton O
- Stenzel H
- Stewart GA
- Stockton MC
- Stoebe M
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- Stolte P
- Stonjek S
- Stradling AR
- Straessner A
- Stramaglia ME
- Strandberg J
- Strandberg S
- Strauss M
- Strizenec P
- Stroehmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Styles NA
- Su D
- Su J
- Suchek S
- Sugaya Y
- Suk M
- Sulin VV
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
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- Suruliz K
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
- Tafirout R
- Tahirovic E
- Taiblum N
- Takai H
- Takashima R
- Takasugi EH
- Takeshita T
- Takubo Y
- Talby M
- Talyshev AA
- Tanaka J
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- Tapia Araya S
- Tapprogge S
- Tarem S
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- Tas P
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- Tashiro T
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- Tavares Delgado A
- Tayalati Y
- Taylor AC
- Taylor AJ
- Taylor GN
- Taylor PTE
- Taylor W
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- Teixeira-Dias P
- Temple D
- Ten Kate H
- Teng PK
- Teoh JJ
- Tepel F
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- Thiele F
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- Tibbetts MJ
- Tikhomirov VO
- Tikhonov Yu A
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- Trocme B
- Trofymov A
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- Tsang KW
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- Tsiareshka PV
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsui KM
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Tupputi SA
- Turchikhin S
- Turgeman D
- Turra R
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- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
- Unverdorben C
- Urban J
- Urquijo P
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- Usai G
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- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Valkar S
- Vallier A
- Valls Ferrer JA
- Van Den Wollenberg W
- van der Graaf H
- van Gemmeren P
- Van Nieuwkoop J
- van Vulpen I
- van Woerden MC
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vardanyan G
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vasquez GA
- Vasquez JG
- Vazeille F
- Vazquez JG Panduro
- Veatch J
- Veeraraghavan V
- Veloce LM
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- Ventura A
- Venturi M
- Venturi N
- Venturini A
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Verzini MJ Alconada
- Vetterli MC
- Viaux Maira N
- Viazlo O
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Villa M
- Villar DI Narrias
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vogel M
- Vokac P
- Volpi G
- von der Schmitt H
- von Toerne E
- Vorobel V
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- Vos M
- Voss R
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
- Walder J
- Walker R
- Walkowiak W
- Wallangen V
- Walls FM Garay
- Wang C
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- Wang Q
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- Wang W
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- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Washbrook A
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- Watson AT
- Watson MF
- Watts G
- Watts S
- Waugh BM
- Webb AF
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- Weber MS
- Weber SA
- Weber SW
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weirich M
- Weiser C
- Weits H
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Werner P
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
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- White MJ
- White R
- Whiteson D
- Whitmore BW
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong KH Yau
- Wong VWS
- Worm SD
- Wosiek BK
- Wotschack J
- Wozniak KW
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu L
- Xu T
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
The analysis of the momentum difference between charged hadrons in high-energy proton-proton collisions is performed in order to study coherent particle production. The observed correlation pattern agrees with a model of a helical QCD string fragmenting into a chain of ground-state hadrons. A threshold momentum difference in the production of adjacent pairs of charged hadrons is observed, in agreement with model predictions. The presence of low-mass hadron chains also explains the emergence of charge-combination-dependent two-particle correlations commonly attributed to Bose-Einstein interference. The data sample consists of 190 ÎŒbâ1 of minimum-bias events collected with proton-proton collisions at a center-of-mass energy âs=7 TeV in the early low-luminosity data taking with the ATLAS detector at the LHC
Performance of missing transverse momentum reconstruction with the ATLAS detector using protonâproton collisions at âs = 13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Acharya BS
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in protonâproton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying Ï -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fbâ1
Search for supersymmetry in events with four or more leptons in âs =13 TeV pp collisions with ATLAS
- Author
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- Zemaityte G
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- Zhao Z
- Zhemchugov A
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- Zhu H
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Ălvarez Piqueras D
- Ă kesson TPA
- Ć filigoj T
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
Results from a search for supersymmetry in events with four or more charged leptons (electrons, muons and taus) are presented. The analysis uses a data sample corresponding to 36.1 fb â1 of proton-proton collisions delivered by the Large Hadron Collider at s â =13 TeV and recorded by the ATLAS detector. Four-lepton signal regions with up to two hadronically decaying taus are designed to target a range of supersymmetric scenarios that can be either enriched in or depleted of events involving the production and decay of a Z boson. Data yields are consistent with Standard Model expectations and results are used to set upper limits on the event yields from processes beyond the Standard Model. Exclusion limits are set at the 95% confidence level in simplified models of General Gauge Mediated supersymmetry, where higgsino masses are excluded up to 295 GeV. In R -parity-violating simplified models with decays of the lightest supersymmetric particle to charged leptons, lower limits of 1.46 TeV, 1.06 TeV, and 2.25 TeV are placed on wino, slepton and gluino masses, respectively
Measurements of integrated and differential cross sections for isolated photon pair production in pp collisions at âs=8 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TP
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty M
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkinson M
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- Korolkov I
- Korolkova EV
- Kortner O
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- Kosek T
- Kostyukhin VV
- Kotwal A
- Koulouris A
- Kourkoumeli-Charalampidi A
- Kourkoumelis C
- Kourlitis E
- Kouskoura V
- Kowalewska AB
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- Kozanecki W
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- Valentinetti S
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- Valls Ferrer JA
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- van der Graaf H
- van Gemmeren P
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- van Vulpen I
- van Woerden MC
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- Yildirim E
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- Zemla A
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimine NI
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of âs=8 TeV is presented. The results are based on an integrated luminosity of 20.2 fbâ1 recorded by the ATLAS detector at the Large Hadron Collider. The measurement considers photons with pseudorapidities satisfying |ηγ|40GeV and EÎłT,2>30 GeV for the two leading photons ordered in transverse energy produced in the interaction. The background due to hadronic jets and electrons is subtracted using data-driven techniques. The fiducial cross sections are corrected for detector effects and measured differentially as a function of six kinematic observables. The measured cross section integrated within the fiducial volume is 16.8 ± 0.8â pb . The data are compared to fixed-order QCD calculations at next-to-leading-order and next-to-next-to-leading-order accuracy as well as next-to-leading-order computations including resummation of initial-state gluon radiation at next-to-next-to-leading logarithm or matched to a parton shower, with relative uncertainties varying from 5% to 20%
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