6 research outputs found
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- 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
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
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- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
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- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
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- Anisenkov AV
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- Aparo MA
- Appelt C
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- Arcangeletti C
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- Arena E
- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Assahsah J
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- Atlay NB
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- Zhemchugov A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Direct constraint on the Higgs–charm coupling from a search for Higgs boson decays into charm quarks with the ATLAS detector
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- Ottino GJ
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- Ouellette J
- Ould-Saada F
- Outschoorn VIM
- Owen M
- Owen RE
- O’Keefe MW
- O’Neil DC
- O’neill AP
- O’Shea V
- Pardos CD
- Pascual JAG
- Paz IL
- Pena JJ
- Pietra MD
- Pino SAO
- Ponce JMI
- Pozo JAA
- Pree TAD
- Pretel JAF
- Ramos JM
- Renteria CG
- Rodriguez GRG
- Rojas JGRG
- Romero LM
- Rosende SJN
- Rozas AJ
- Sanchez FJM
- Santos SPAD
- Seabra LFO
- Sola JDB
- Solis AL
- Suarez PM
- Suarez RG
- Tame ZPA
- Toro RC
- Torregrosa EF
- Urbán SC
- Vazquez CJB
- Verzini MJA
- Volpe DD
- Walls FMG
- Yildiz HD
- Zagazeta LFG
- Åkesson TPA
- Öncel ÖO
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/08/2022
- Field of study
A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton–proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb−1. Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW, WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the (W/Z)Z(→cc¯) process and 3.8 (4.6) standard deviations for the (W/Z)W(→cq) process. The (W/Z)H(→cc¯) search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model cross-section times branching fraction for a Higgs boson with a mass of , corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier |κc|<8.5 (12.4), at the 95% confidence level. A combination with the ATLAS (W/Z)H,H→bb¯ analysis is performed, allowing the ratio κc/κb to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level
Search for neutral long-lived particles in pp collisions at root s = 13 TeV that decay into displaced hadronic jets in the ATLAS calorimeter
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli V S
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov V A
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- 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
- Alvarez Estevez M
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov V A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Achkar B
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- Zagazeta LFG
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- Zakharchuk N
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- Zeißner SV
- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
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- Zhang Z
- Zhao H
- Zhao P
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu C
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- Zhu H
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- 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
- 'American Physical Society (APS)'
- Publication date
- 01/05/2023
- Field of study
Determination of the parton distribution functions of the proton using diverse ATLAS data from pp collisions at root s=7, 8 and 13 TeV
- 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
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- Ahnen JV
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi A
- Alfonsi F
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- Ali B
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- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
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- Alves FLL
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- Ambler A
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- Amelung C
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- Amrouche CS
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- Andeen T
- Anders JK
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- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
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- Antrim DJA
- Anulli F
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- Aparo MA
- Aranda CP
- Aranzabal N
- Araujo MVD
- Araya ST
- Arcangeletti C
- Arce ATH
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- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
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- Asai K
- Asai S
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- Asimakopoulou EM
- Asmundis RD
- Asquith L
- Assahsah J
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- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
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- Azuelos G
- Babal D
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- Barkeloo J
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- Baron P
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- Barr AJ
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- Barrue RFC
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- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Baselga M
- Bashta I
- Bassalat A
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- Basson CR
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- Batlamous S
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- Bohm C
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- Booth CD
- Borbély AG
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Bosca SR
- Boscherini D
- Bosman M
- Bostanabad MG
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- Bryngemark L
- Brüers B
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- Carlson TI
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- Carvalho ALMD
- Casadei D
- Casado MP
- Casha AF
- Castiglia EG
- Castillo FL
- Castillo LRF
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- Catmore JR
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- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
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- Chekulaev SV
- Chelkov GA
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- Chen C
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- Chen H
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
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- Chen Y
- 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
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
- Chow YS
- Chowdhury T
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Ciaccio AD
- Ciaccio LD
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark PJ
- Clawson SE
- Clement C
- Clissa L
- Coadou Y
- Cobal M
- Coccaro A
- Codina EP
- Coelli S
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- Cole B
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- Connell SH
- Connelly IA
- Conroy EI
- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cormier F
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa AMMJD
- Costa MJ
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- Costanzo D
- Cote BM
- Coutinho YA
- Cowan G
- Cowley JW
- Cranmer K
- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
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- Crépé-Renaudin S
- Cueto A
- Cui H
- Cui Z
- Cukierman AR
- Cunningham WR
- Curcio F
- Czodrowski P
- Czurylo MM
- da Costa JBG
- Daalen TRV
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
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- Davis-Purcell B
- Dawson I
- de Jong P
- de la Hoz SG
- de Renstrom PAB
- De K
- Dedovich DV
- Degens J
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- Delitzsch CM
- Dell’Acqua A
- Dell’Asta L
- Delmastro M
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- Demichev M
- Denisov SP
- Derendarz D
- Derue F
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- Deutsch C
- Deviveiros PO
- Diaconu C
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- Dimitrievska A
- Ding W
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- Dinu I-M
- Dittmeier SJ
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- Djobava T
- Djuvsland JI
- Dodsworth D
- Doglioni C
- Dolejsi J
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- Domenico AD
- Dominguez LP
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- Donaldson CP
- Donato CD
- Donell DMM
- Dong B
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Drobac AS
- Du D
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- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Duflot L
- Dumitriu AE
- Dunford M
- Dungs S
- Dunne K
- Duperrin A
- Durglishvili A
- Dutta B
- Dwyer BL
- Dyckes GI
- Dyndal M
- Dysch S
- Dziedzic BS
- Dührssen M
- Dülsen C
- Düren M
- D’amen G
- D’Amico V
- D’Auria S
- D’Eramo L
- D’onofrio A
- D’Onofrio M
- D’uffizi M
- Eckerova B
- Eggleston MG
- Ehrke LF
- Eigen G
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- Ellajosyula V
- Ellert M
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- Enari Y
- Ene I
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- Errenst M
- Escalier M
- Escobar C
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- Estevez MA
- Etzion E
- Evans G
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- Evans MO
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- Ezzarqtouni S
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- Facini G
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- Fakhrutdinov RM
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- Falke PJ
- Falke S
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- Farilla A
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- Farrington SM
- Fassi F
- Fassouliotis D
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedotov G
- Feickert M
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- Fellers DE
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- Ferguson SW
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- Ferrere D
- Ferretti C
- Fiedler F
- Filho LMDA
- Filipčič A
- Filthaut F
- Fiolhais MCN
- Fiorini L
- Fischer F
- Fisher WC
- Fitschen T
- Fleck I
- Fleischmann P
- Flick T
- Flores L
- Flores M
- Follega FM
- Fomin N
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- Forland BC
- Formica A
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- Fortin E
- Fortman AW
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- Francescato S
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- Freund WS
- Freundlich EM
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- Frost JA
- Fu Y
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- Furelos DV
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- Gabrielli A
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- Gallas EJ
- Gallop BJ
- Galvan IS
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- García C
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- Garg RB
- Gargiulo S
- Garner CA
- Garonne V
- Garzon GOY
- Gasiorowski SJ
- Gaspar P
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- Gauzzi P
- Gavrilenko IL
- Gavrilyuk A
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- Gazis EN
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- Gentile S
- George S
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- Gerlach LO
- Gessinger-Befurt P
- Ghazali YE
- Ghosh A
- Ghosh A
- Giacobbe B
- Giagu S
- Giangiacomi N
- Giannelli MF
- Giannetti P
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- Gillwald NEK
- Gimenez VC
- Ginabat L
- Gingrich DM
- Ginn CM
- Giordani MP
- Giraud PF
- Girolamo AD
- Giugliarelli G
- Giugni D
- Giuli F
- Gkialas I
- Gkountoumis P
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- Gorišek A
- Goshaw AT
- Gostkin MI
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- Gouighri M
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- Heggelund AL
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- Iglesias JAS
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- Lösle A
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- McNamara PC
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- Minegishi Y
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
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- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
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- 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 an analysis at next-to-next-to-leading order in the
theory of quantum chromodynamics for the determination of a new set of proton
parton distribution functions using diverse measurements in pp collisions at
s=7, 8 and 13 TeV, performed by the ATLAS experiment at the Large
Hadron Collider, together with deep inelastic scattering data from ep
collisions at the HERA collider. The ATLAS data sets considered are
differential cross-section measurements of inclusive W± and Z/γ∗
boson production, W± and Z boson production in association with jets,
ttˉ production, inclusive jet production and direct photon production.
In the analysis, particular attention is paid to the correlation of systematic
uncertainties within and between the various ATLAS data sets and to the impact
of model, theoretical and parameterisation uncertainties. The resulting set of
parton distribution functions is called ATLASpdf2
Determination of the parton distribution functions of the proton using diverse ATLAS data from pp collisions at root s=7, 8 and 13 TeV
- 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
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
This paper presents an analysis at next-to-next-to-leading order in the theory of quantum chromodynamics for the determination of a new set of proton parton distribution functions using diverse measurements in pp collisions at root s = 7, 8 and 13 TeV, performed by the ATLAS experiment at the Large Hadron Collider, together with deep inelastic scattering data from ep collisions at the HERA collider. The ATLAS data sets considered are differential cross-section measurements of inclusive W-+/- and Z/gamma* boson production, W-+/- and Z boson production in association with jets, t (t) over bar production, inclusive jet production and direct photon production. In the analysis, particular attention is paid to the correlation of systematic uncertainties within and between the various ATLAS data sets and to the impact of model, theoretical and parameterisation uncertainties. The resulting set of parton distribution functions is called ATLASpdf21