169 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
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- Ahmadov F
- Ahmed WS
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- Aielli G
- Aizenberg I
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- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
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- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
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- Anders JK
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- Angelidakis S
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- Anisenkov AV
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- Antrim DJA
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- Aoki M
- 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
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- Artoni G
- Asada H
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- Asimakopoulou EM
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- Zhemchugov A
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- Zwalinski L
- 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.]
Measurement of the energy asymmetry in t(t)over-barj production at 13 TeV with the ATLAS experiment and interpretation in the SMEFT framework
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- Yexley MR
- Yildiz H Duran
- Yin P
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- Yoshihara K
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- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zagazeta LF Gutierrez
- Zaid E
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- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaplatilek O
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- Zeitnitz C
- Zeng JC
- Zenger DT
- Zenin O
- Zenis T
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- Zerradi S
- Zerwas D
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- Zhang DF
- Zhang G
- Zhang J
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- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
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- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
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- Zivkovic L
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 28/04/2022
- Field of study
A measurement of the energy asymmetry in jet-associated top-quark pair production is presented using 139fb−1
139
fb
-
1
of data collected by the ATLAS detector at the Large Hadron Collider during pp collisions at s=13TeV
s
=
13
TeV
. The observable measures the different probability of top and antitop quarks to have the higher energy as a function of the jet scattering angle with respect to the beam axis. The energy asymmetry is measured in the semileptonic ttˉ
t
t
¯
decay channel, and the hadronically decaying top quark must have transverse momentum above 350GeV
350
GeV
. The results are corrected for detector effects to particle level in three bins of the scattering angle of the associated jet. The measurement agrees with the SM prediction at next-to-leading-order accuracy in quantum chromodynamics in all three bins. In the bin with the largest expected asymmetry, where the jet is emitted perpendicular to the beam, the energy asymmetry is measured to be −0.043±0.020
-
0.043
±
0.020
, in agreement with the SM prediction of −0.037±0.003
-
0.037
±
0.003
. Interpreting this result in the framework of the Standard Model effective field theory (SMEFT), it is shown that the energy asymmetry is sensitive to the top-quark chirality in four-quark operators and is therefore a valuable new observable in global SMEFT fits
Determination of the parton distribution functions of the proton using diverse ATLAS data from pp collisions at √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 A Abed
- 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 P Martinez
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen J Von
- 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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- Aloisio A
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- Andana RY González
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- Zhemchugov A
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- Zhulanov V
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- Ziolkowski M
- Zoccoli A
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- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- 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 \sqrt{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\bar{t} 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
Modelling and computational improvements to the simulation of single vector-boson plus jet processes for the ATLAS experiment
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
- Zimine NI
- Zimmermann S
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
This paper presents updated Monte Carlo configurations used to model the production of single electroweak vector bosons (W, Z/gamma*) in association with jets in proton-proton collisions for the ATLAS experiment at the Large Hadron Collider. Improvements pertaining to the electroweak input scheme, parton-shower splitting kernels and scale-setting scheme are shown for multi-jet merged configurations accurate to next-to-leading order in the strong and electroweak couplings. The computational resources required for these set-ups are assessed, and approximations are introduced resulting in a factor three reduction of the per-event CPU time without affecting the physics modelling performance. Continuous statistical enhancement techniques are introduced by ATLAS in order to populate low cross-section regions of phase space and are shown to match or exceed the generated effective luminosity. This, together with the lower per-event CPU time, results in a 50% reduction in the required computing resources compared to a legacy set-up previously used by the ATLAS collaboration. The set-ups described in this paper will be used for future ATLAS analyses and lay the foundation for the next generation of Monte Carlo predictions for single vector-boson plus jets production
Configuration and performance of the ATLAS b-jet triggers in Run 2
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- Yin P
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- Yoshihara K
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- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
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- Zhang K
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- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
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- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
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- 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
- Zivkovic L
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/12/2021
- Field of study
Several improvements to the ATLAS triggers used to identify jets containing b-hadrons (b-jets) were implemented for data-taking during Run 2 of the Large Hadron Collider from 2016 to 2018. These changes include reconfiguring the b-jet trigger software to improve primary-vertex finding and allow more stable running in conditions with high pile-up, and the implementation of the functionality needed to run sophisticated taggers used by the offline reconstruction in an online environment. These improvements yielded an order of magnitude better light-flavour jet rejection for the same b-jet identification efficiency compared to the performance in Run 1 (2011–2012). The efficiency to identify b-jets in the trigger, and the conditional efficiency for b-jets that satisfy offline b-tagging requirements to pass the trigger are also measured. Correction factors are derived to calibrate the b-tagging efficiency in simulation to match that observed in data. The associated systematic uncertainties are substantially smaller than in previous measurements. In addition, b-jet triggers were operated for the first time during heavy-ion data-taking, using dedicated triggers that were developed to identify semileptonic b-hadron decays by selecting events with geometrically overlapping muons and jets
The ATLAS inner detector trigger performance in pp collisions at 13 TeV during LHC Run 2
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
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- Adiguzel A
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- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
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- Ai X
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- Alberghi GL
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- Alfonsi A
- Alfonsi F
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- Ali B
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- Allaire C
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- Aloisio A
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- Belotskiy K
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- Blumenthal J
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- Bobrovnikov VS
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- Borgna LS
- Borisov A
- Borissov G
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- Boscherini D
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- Briglin DL
- Britton D
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- Brooks WK
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- Bruni A
- Bruni G
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- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buddenbrock SEV
- Bugge MK
- Bulekov O
- Bullard BA
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buscher V
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
- Cabras G
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
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- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvet D
- Calvet S
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- Calvetti M
- Camarda S
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- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
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- Camplani A
- Canale V
- Canesse A
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- Cao Y
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- Capua M
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- Cardillo F
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- Carlino G
- Carlson BT
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- Carney RMD
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- Casado MP
- Casha AF
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- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
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- Celli F
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- Cerri A
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- Cheng HC
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- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
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- Chomont AR
- Chou Y
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- Christopher LD
- Chu MC
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- Ciesla KM
- Cindro V
- Cioara IA
- Ciocio A
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- Ciubotaru DA
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- Czekierda S
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- D'Amico V
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- Da Via C
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- Dachs F
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- de Renstrom PAB
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- Doglioni C
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- Dong B
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- Doria A
- Dova MT
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- Drechsler E
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- Ducu OA
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- Dumitriu AE
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- Dziedzic BS
- Eggleston MG
- Eifert T
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- 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
Corrigendum to "Search for flavour-changing neutral-current couplings between the top quark and the photon with the ATLAS detector at √s=13 TeV" (Physics Letters B, 842 (2023), 137379)
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- Publication venue
- ELSEVIER
- Publication date
- 01/01/2023
- Field of study
Constraints on Higgs boson production with large transverse momentum using H \rightarrow b\bar{b} decays in the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam Bourdarios C
- 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
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akatsuka S
- Akbiyik M
- Akimov AV
- 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
- Alunno Camelia E
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- 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 AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Aranzabal N
- Araujo Ferraz V
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Arrubarrena Tame ZP
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlay NB
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- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
- Avolio G
- Ayoub MK
- Azuelos G
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- Balasubramanian R
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- Barberio EL
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- Barends KN
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- Barklow T
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- Barreiro F
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- Barrue RF Coelho
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- Bartoldus R
- Bartolini G
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- Bednyakov VA
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- Belotskiy K
- Belyaev NL
- Benchekroun D
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- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
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- Bergeaas Kuutmann E
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- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Bernardi G
- Bernius C
- Bernlochner FU
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- Berta P
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- Bessidskaia Bylund O
- Bethke S
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- Bhattarai P
- Bhopatkar VS
- Bi R
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- Birch-sykes CJ
- Bird GA
- Birman M
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- Biswal JP
- Biswas D
- Bitadze A
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- Bjørke K
- Bloch I
- Blocker C
- Blue A
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- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
- Boehler M
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbély AG
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- Busch EL
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- Zhemchugov A
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- Zhulanov V
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- Zimmermann S
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- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/05/2022
- Field of study
This paper reports constraints on Higgs boson production with transverse momentum above 1 TeV. The analyzed data from proton–proton collisions at a center-of-mass energy of 13 TeV were recorded with the ATLAS detector at the Large Hadron Collider from 2015 to 2018 and correspond to an integrated luminosity of 136fb^{-1}. Higgs bosons decaying into b\bar{b} are reconstructed as single large-radius jets recoiling against a hadronic system and are identified by the experimental signature of two b-hadron decays. The experimental techniques are validated in the same kinematic regime using the Z \rightarrow b\bar{b} process. The 95% confidence-level upper limit on the cross section for Higgs boson production with transverse momentum above 450 GeV is 115 fb, and above 1 TeV it is 9.6 fb. The Standard Model cross section predictions for a Higgs boson with a mass of 125 GeV in the same kinematic regions are 18.4 fb and 0.13 fb, respectively
Observation of electroweak production of two jets and a Z-boson pair
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- Abbott B
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- Zhemchugov A
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- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
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- Zwalinski L
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 09/02/2023
- Field of study
Electroweak symmetry breaking explains the origin of the masses of elementary particles through their interactions with the Higgs field. Besides the measurements of the Higgs boson properties, the study of the scattering of massive vector bosons with spin 1 allows the nature of electroweak symmetry breaking to be probed. Among all processes related to vector-boson scattering, the electroweak production of two jets and a Z-boson pair is a rare and important one. Here we report the observation of this process from proton–proton collision data corresponding to an integrated luminosity of 139 fb−1 recorded at a centre-of-mass energy of 13 TeV with the ATLAS detector at the Large Hadron Collider. We consider two different final states originating from the decays of the Z-boson pair: one containing four charged leptons and another containing two charged leptons and two neutrinos. The hypothesis of no electroweak production is rejected with a statistical significance of 5.7σ, and the measured cross-section for electroweak production is consistent with the Standard Model prediction. In addition, we report cross-sections for inclusive production of a Z-boson pair and two jets for the two final states
Direct constraint on the Higgs–charm coupling from a search for Higgs boson decays into charm quarks with the ATLAS detector
- Author
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- Abbott B
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- Abhayasinghe DK
- Abidi SH
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- Mondal B
- Mondal S
- Monnier E
- Montella M
- Monticelli F
- Morange N
- Morettini P
- Morgenstern S
- Mori D
- Morii M
- Morinaga M
- Morisbak V
- Morley AK
- Morvaj L
- Moschovakos P
- Moser B
- Mosidze M
- Moskalets T
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- Moussaouy AE
- Moyse EJW
- Muanza S
- Mueller J
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- Muenstermann D
- Muiño PC
- Mullier GA
- Mullin JJ
- Mungo DP
- Munoz DC
- Murin M
- Murray WJ
- Murrone A
- Muse JM
- Muškinja M
- Mwewa C
- Myagkov AG
- Myers AA
- Myers AJ
- Myers G
- Myska M
- Mönig K
- Nachman BP
- Nackenhorst O
- Nag AN
- Nagai K
- Nagano K
- Nagle JL
- Nagy E
- Nairz AM
- Nakahama Y
- Nakamura K
- Nanjo H
- Narayan R
- Narayanan EA
- Naryshkin I
- Naseri M
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- Navarro G
- Navarro JEG
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- Navarro-Gonzalez J
- Nayak R
- Nechaeva PY
- Nechansky F
- Neep TJ
- Negri A
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- Nickerson RB
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- Nikiforou N
- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
- Nilsson P
- Nindhito HR
- Nisati A
- Nishu N
- Nisius R
- Nobe T
- Noel DL
- Noguchi Y
- Nomidis I
- Nomura MA
- Norfolk MB
- Norisam RRB
- Novak J
- Novak T
- Novgorodova O
- Novotny L
- Novotny R
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- Nurse E
- Oakham FG
- Ocariz J
- Ochi A
- Ochoa I
- Ochoa-Ricoux JP
- Oda S
- Oerdek S
- Ogrodnik A
- Oh A
- Ohm CC
- Oide H
- Oishi R
- Ojeda ML
- Okazaki Y
- Okumura Y
- Olariu A
- Oliver JL
- Olsson MJR
- Olszewski A
- Olszowska J
- Onofre A
- Onyisi PUE
- Oreglia MJ
- Orellana GE
- Orestano D
- Orlando N
- Orr RS
- Ospanov R
- Otono H
- Ott PS
- Ottino GJ
- Ouchrif M
- 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
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