24 research outputs found
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
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- Akbiyik M
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- Akimov AV
- Al Khoury K
- Alberghi GL
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- Alderweireldt S
- Aleksa M
- Aleksandrov IN
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- Argyropoulos S
- Arling J-H
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
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
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- Zhemchugov A
- Zheng Z
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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.]
The ATLAS inner detector trigger performance in pp collisions at 13 TeV during LHC Run 2
- Author
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- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Publication venue
- Publication date
- 01/01/2022
- Field of study
The design and performance of the inner detector trigger for the high level trigger of the ATLAS experiment at the Large Hadron Collider during the 2016-2018 data taking period is discussed. In 2016, 2017, and 2018 the ATLAS detector recorded 35.6 fb(-1), 46.9 fb(-1), and 60.6 fb(-1) respectively of proton-proton collision data at a centre-of-mass energy of 13TeV. In order to deal with the very high interaction multiplicities per bunch crossing expected with the 13TeV collisions the inner detector trigger was redesigned during the long shutdown of the Large Hadron Collider from 2013 until 2015. An overview of these developments is provided and the performance of the tracking in the trigger for the muon, electron, tau and b-jet signatures is discussed. The high performance of the inner detector trigger with these extreme interaction multiplicities demonstrates how the inner detector tracking continues to lie at the heart of the trigger performance and is essential in enabling the ATLAS physics programme
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at s√=13TeV
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- Zahreddine J
- Zaitsev AM
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- Zakharchuk N
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerradi S
- Zerwas D
- Zgubič M
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
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- Zhang L
- Zhang M
- Zhang R
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- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Aizenberg I
- Akatsuka S
- Akbiyik M
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
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- Astigarraga MEP
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- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
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- Austrup VA
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- Azuelos G
- Babal D
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- Celebi E
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- Centonze MS
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- Cervelli A
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- Chala M
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- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
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- Chen X
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- Cheremushkina E
- Cherepanova E
- Cheu E
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- Chevalier L
- Chiarella V
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- Chiodini G
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- Christopher LD
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- Chudoba J
- Chwastowski JJ
- Ciaccio AD
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- Ciesla KM
- Cindro V
- Cioară IA
- Ciocio A
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- Czurylo MM
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- da Costa JBG
- Da Cruz E Silva CB
- Da Cunha Sargedas De Sousa MJ
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- Da Via C
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- Dado T
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- Dawson I
- de Andrade Filho LM
- De Araujo MV
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- de Jong P
- de la Hoz SG
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- de Renstrom PAB
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- Deviveiros PO
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- Filthaut F
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- Zenger DT
- Zenin O
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- Zhao P
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- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhou N
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- Zhu C
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- EUROPEAN PHYSICAL JOURNAL C
- Publication date
- 01/01/2022
- Field of study
This paper presents the measurement of the electroweak production of two jets
in association with a Zγ pair with the Z boson decaying into two
neutrinos. It also presents the search for invisible or partially invisible
decays of a Higgs boson with a mass of 125 GeV produced through vector-boson
fusion with a photon in the final state. These results use data from LHC
proton-proton collisions at s = 13 TeV collected with the ATLAS
detector corresponding to an integrated luminosity of 139 fb−1. The event
signature, shared by all benchmark processes considered for measurements and
searches, is characterized by a significant amount of unbalanced transverse
momentum and a photon in the final state, in addition to a pair of forward
jets. For electroweak production of Zγ in association with two jets, the
background-only hypothesis is rejected with an observed (expected) significance
of 5.2 (5.1) standard deviations. The measured fiducial cross-section for this
process is 1.31±0.29 fb. Observed (expected) upper limit of 0.37 (0.34) at
95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to
invisible particles, assuming the Standard Model production cross-section. The
signature is also interpreted in the context of decays of a Higgs boson to a
photon and a dark photon. An observed (expected) 95% CL upper limit on the
branching ratio for this decay is set at 0.018 (0.017), assuming the 125 GeV
Standard Model Higgs boson production cross-section
Headmasters: Microglial regulation of learning and memory in health and disease
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- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2018
- Field of study
Search for the charged-lepton-flavor-violating decay Z→eμ in pp collisions at s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
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- Affolder AA
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- Alberghi GL
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- Aleksandrov IN
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- Antrim DJA
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- Arling J-H
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- Zakharchuk N
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- Zeitnitz C
- Zeißner SV
- Zeng JC
- Zenger DT
- Zenin O
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- Zerwas D
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- Zhao T
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu C
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- American Physical Society (APS)
- Publication date
- 01/01/2023
- Field of study
Evidence for Higgs boson decays to a low-mass dilepton system and a photon in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- 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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- Allaire C
- Allbrooke BMM
- Allport PP
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- Amelung C
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- Anthony MT
- Antipov E
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- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
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- Arnold H
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- Assahsah J
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- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Backman F
- Bagnaia P
- Bahilo JJL
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- Bahrasemani H
- Bailey AJ
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- Baines JT
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- Bassalat A
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- Basson CR
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- Benchekroun D
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- Cheplakov A
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- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
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- Christopher LD
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- Chudoba J
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- Cindro V
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- Zahreddine J
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- Zakharchuk N
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- Zanzi D
- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zgubič M
- Zhang B
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- Zhang G
- Zhang J
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- Zhang L
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- Zhang R
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- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2021
- Field of study
A search for the Higgs boson decaying into a photon and a pair of electrons or muons with an invariant mass
GeV is presented. The analysis is performed using 139 fb−1 of proton–proton collision data, produced by the LHC at a centre-of-mass energy of 13 TeV and collected by the ATLAS experiment. Evidence for the
process is found with a significance of 3.2 over the background-only hypothesis, compared to an expected significance of 2.1 for the Standard Model prediction. The best-fit value of the signal-strength parameter, defined as the ratio of the observed signal yield to the one expected in the Standard Model, is
. The Higgs boson production cross-section times the
branching ratio for
GeV is determined to be
fb
Measurement of the energy asymmetry in t(t)over-barj production at 13 TeV with the ATLAS experiment and interpretation in the SMEFT framework
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Aizenberg I
- Akatsuka S
- Akbiyik M
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
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- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
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- Beisiegel F
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- Burgard CD
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- Busch EL
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- Butler JM
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- Butterworth JM
- Buttinger W
- Buzykaev AR
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- Calafiura P
- Calderini G
- Calfayan P
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- Caloba LP
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- Camerlingo MT
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- Canale V
- Canesse A
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- Cao Y
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- Capriles FGD
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- Castillo FL
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- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
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- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
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- Christopher LD
- Chu MC
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- Chwastowski JJ
- Ciaccio AD
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- Cieri D
- Ciesla KM
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
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- Ciubotaru DA
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- Czurylo MM
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- da Costa JBG
- Da Cruz E Silva CB
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
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- De Araujo MV
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- de Jong P
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- de Renstrom PAB
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- Djuvsland JI
- Dodsworth D
- Doglioni C
- Dolejsi J
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- Dominguez LP
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- Donaldson CP
- Donato CD
- Donell DMM
- Dong B
- Donini J
- Donszelmann TC
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- Dova MT
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- Dreyer E
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- Dumitriu AE
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- Durglishvili A
- Dutta B
- Dyckes GI
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- Filthaut F
- Fiolhais MCN
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- Fleck I
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- Flierl BM
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- Ghazali YE
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- EUROPEAN PHYSICAL JOURNAL C
- Publication date
- 01/01/2022
- Field of study
A measurement of the energy asymmetry in jet-associated top-quark pair
production is presented using 139 fb−1 of data collected by the
ATLAS detector at the Large Hadron Collider during pp collisions at
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 decay channel, and the hadronically decaying top quark
must have transverse momentum above 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, in agreement with the SM prediction of −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
A search for an unexpected asymmetry in the production of e + μ − and e − μ + pairs in proton–proton collisions recorded by the ATLAS detector at s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Abramowicz H
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- Pizzimento L
- Pizzini A
- Pleier M-A
- Plesanovs V
- Pleskot V
- Plotnikova E
- Poblete PAU
- Podberezko P
- Poettgen R
- Poggi R
- Poggioli L
- Pogrebnyak I
- Pohl D
- Pokharel I
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Pollock ZB
- Polychronakos V
- Ponce JMI
- Ponomarenko D
- Pontecorvo L
- Popa S
- Popeneciu GA
- Portales L
- Pospisil S
- Postolache P
- Potamianos K
- Potrap IN
- Potter CJ
- Potti H
- Poulsen T
- Poveda J
- Powell TD
- Pownall G
- Pozo JAA
- Pralavorio P
- Prapa MM
- Prell S
- Price D
- Primavera M
- Proffitt ML
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
- Przybycien M
- Pudzha D
- Puzo P
- Pyatiizbyantseva D
- Qian J
- Qin Y
- Qiu T
- Quadt A
- Queitsch-Maitland M
- Quintero DMP
- Ragusa F
- Raine JA
- Rajagopalan S
- Ramos JM
- Ran K
- Rassloff DF
- Rauch DM
- Rave S
- Ravina B
- Ravinovich I
- Raymond M
- Read AL
- Readioff NP
- Rebuzzi DM
- Redlinger G
- Reeves K
- Regie JBDVD
- Reikher D
- Reiss A
- Rej A
- Rembser C
- Renardi A
- Renda M
- Rendel MB
- Rennie AG
- Renous DS
- Renteria CG
- Resconi S
- Ressegotti M
- Resseguie ED
- Rettie S
- Reynolds B
- Reynolds E
- Rezanova OL
- Reznicek P
- Ricci E
- Richter R
- Richter S
- Richter-Was E
- Ridel M
- Rieck P
- Riedler P
- Rifki O
- Rijssenbeek M
- Rimoldi A
- Rimoldi M
- Rinaldi L
- Rinn TT
- Rinnagel MP
- Ripellino G
- Riu I
- Rivadeneira P
- Rizatdinova F
- Rizvi E
- Rizzi C
- Roberts BA
- Roberts BR
- Robertson SH
- Robin M
- Robinson D
- Robson A
- Rocchi A
- Roda C
- Rodriguez AR
- Rodriguez GRG
- Roe S
- Roepe AR
- Roggel J
- Rojas JGRG
- Rojas RA
- Roland B
- Roland CPA
- Roloff J
- Romaniouk A
- Romano M
- Romero LM
- Rompotis N
- Ronzani M
- Roos L
- Rosati S
- Rosser BJ
- Rossi E
- Rossi E
- Rossi E
- Rossi LP
- Rossini L
- Rosten R
- Rotaru M
- Rottler B
- Rousseau D
- Rousso D
- Rovelli G
- Roy A
- Rozanov A
- Rozas AJ
- Rozen Y
- Ruan X
- Ruby AJ
- Ruggeri TA
- Ruiz-Martinez A
- Rummler A
- Rurikova Z
- Rusakovich NA
- Russell HL
- Rustige L
- Rutherfoord JP
- Rybar M
- Rye EB
- Ryzhov A
- Røhne O
- Rühr F
- Rüttinger EM
- Sabatini P
- Sabetta L
- Sadrozinski HF-W
- Sadykov R
- Saenz SRP
- Safdari M
- Saha S
- Sahinsoy M
- Sahu A
- Saimpert M
- Saito M
- Saito T
- Salamani D
- Salamanna G
- Salas AS
- Salnikov A
- Salt J
- Salvatore D
- Salvatore F
- Salzburger A
- Samani BS
- Sammel D
- Sampsonidis D
- Sampsonidou D
- Sanchez CAS
- Sanchez FJM
- Sanchez LP
- Sandaker H
- Sander CO
- Sanderswood IG
- Sandesara JA
- Sandhoff M
- Sandoval C
- Sankey DPC
- Sannino M
- Sansoni A
- Santoni C
- Santos H
- Santpur SN
- Santra A
- Santurio EV
- Saoucha KA
- Sapronov A
- Saraiva JG
- Sardain J
- Sasaki O
- Sato K
- Sauer C
- Sauerburger F
- Sauvan E
- Savard P
- Sawada R
- Sawyer C
- Sawyer L
- Sbarra C
- Sbrizzi A
- Scanlon T
- Schaarschmidt J
- Schacht P
- Schaefer D
- Schaffer AC
- Schaile D
- Schamberger RD
- Schanet E
- Scharf C
- Scharmberg N
- Schegelsky VA
- Scheirich D
- Schenck F
- Schernau M
- Schiavi C
- Schildgen LK
- Schillaci ZM
- Schioppa EJ
- Schioppa M
- Schlag B
- Schleicher KE
- Schlenker S
- Schmieden K
- Schmitt C
- Schmitt S
- Schoeffel L
- Schoening A
- Scholer PG
- Schopf E
- Schott M
- Schovancova J
- Schramm S
- Schroeder F
- Schroeder TV
- Schultz-Coulon H-C
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schwemling P
- Schwienhorst R
- Schäfer U
- Sciandra A
- Sciolla G
- Scuri F
- Scutti F
- Seabra LFO
- Sebastian VS
- Sebastiani CD
- Sedlaczek K
- Seema P
- Seidel SC
- Seiden A
- Seidlitz BD
- Seiss T
- Seitz C
- Seixas JM
- Sekhniaidze G
- Sekula SJ
- Selem L
- Semprini-Cesari N
- Sen S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sevova S
- Sforza F
- Sfyrla A
- Shabalina E
- Shaheen R
- Shahinian JD
- Shaikh NW
- Shan LY
- Shapiro M
- Sharma A
- Sharma AS
- Sharma S
- Shatalov PB
- Shaw K
- Shaw SM
- Sherwood P
- Shi L
- Shimmin CO
- Shimogama Y
- Shinner JD
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shochet MJ
- Shojaii J
- Shope DR
- Shrestha S
- Shrif EM
- Shroff MJ
- Shulga E
- Sicho P
- Sickles AM
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva JM
- Silverstein SB
- Simion S
- Simoniello R
- Simpson ND
- Simsek S
- Sinervo P
- Sinetckii V
- Singh S
- Singh S
- Sinha S
- Sinha S
- Sioli M
- Siral I
- Sivoklokov SY
- Sjölin J
- Skaf A
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith EA
- Smith HA
- Smizanska M
- Smolek K
- Smykiewicz A
- Snesarev AA
- Snoek HL
- Snyder S
- Sobie R
- Soffer A
- Sohns F
- Sola JDB
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Solomon S
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
- Son H
- Sonay A
- Song WY
- Sopczak A
- Sopio AL
- Sopkova F
- Sottocornola S
- Soualah R
- Soukharev AM
- Soumaimi Z
- South D
- Spagnolo S
- Spalla M
- Spangenberg M
- Spanò F
- Sperlich D
- Spieker TM
- Spigo G
- Spina M
- Spiteri DP
- Spousta M
- Stabile A
- Stamen R
- Stamenkovic M
- Stampekis A
- Standke M
- Stanecka E
- Stanislaus B
- Stanitzki MM
- Stankaityte M
- Stapf B
- Starchenko EA
- Stark GH
- Stark J
- Starko DM
- Staroba P
- Starovoitov P
- Staszewski R
- Stavropoulos G
- Steinberg P
- Steinhebel AL
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
- Stenzel H
- Stevenson TJ
- Stewart GA
- Stockton MC
- Stoicea G
- Stolarski M
- Stonjek S
- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strebler T
- Strizenec P
- Strom DM
- Strom LR
- Stroynowski R
- Strubig A
- Ströhmer R
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Stärz S
- Su D
- Su S
- Su W
- Su X
- Suarez RG
- Sugizaki K
- Sulin VV
- Sullivan MJ
- Sultan DMS
- Sultanaliyeva L
- Sultansoy S
- Sumida T
- Sun S
- Sun S
- Sun X
- Suster CJE
- Sutton MR
- Svatos M
- Swiatlowski M
- Swirski T
- Sykora I
- Sykora M
- Sykora T
- Sánchez J
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Taibah RHM
- Takashima R
- Takeda K
- Takeshita T
- Takeva EP
- Takubo Y
- Talby M
- Talyshev AA
- Tam KC
- Tame ZPA
- Tamir NM
- Tanaka A
- Tanaka J
- Tanaka R
- Tang J
- Tao Z
- Tapprogge S
- Tarem S
- Tariq K
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tassi E
- Tateno G
- Tayalati Y
- Taylor GN
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- Tee AS
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- Teoh JJ
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- Terron J
- Terzo S
- Testa M
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- Themistokleous N
- Theveneaux-Pelzer T
- Thielmann O
- Thomas DW
- Thomas JP
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- Thompson PD
- Thomson E
- Thorpe EJ
- Tian Y
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tipton P
- Tisserant S
- Tlou SH
- Tnourji A
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- Todt S
- Togawa M
- Tojo J
- Tokushuku K
- Tokár S
- Tolley E
- Tombs R
- Tomoto M
- Tompkins L
- Tornambe P
- Toro RC
- Torregrosa EF
- Torrence E
- Torres H
- Toscani M
- Tosciri C
- Toth J
- Tovey DR
- Traeet A
- Treado CJ
- Trefzger T
- Tricoli A
- Trigger IM
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- Trischuk DA
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- Trocmé B
- Trofymov A
- Troncon C
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- Tskhadadze EG
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- Tsujikawa Y
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsur O
- Tsybychev D
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- Tuna AN
- Turchikhin S
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- Unal G
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- Undrus A
- Unel G
- Ungaro FC
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- Urban J
- Urbán SC
- Urquijo P
- Usai G
- Ushioda R
- Usman M
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vafeiadis T
- Valderanis C
- Valente M
- Valentinetti S
- Valero A
- Vallance RA
- Vallier A
- Van Daalen TR
- Van Gemmeren P
- Van Stroud S
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vannicola D
- Vannoli L
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vaslin L
- Vasquez GA
- Vazeille F
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veliscek I
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Vera AMR
- Verbytskyi A
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vernieri C
- Verschuuren PJ
- Verzini MJA
- Vessella M
- Vesterbacka ML
- Vetterli MC
- Vgenopoulos A
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Villhauer EM
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vladimirov V
- Voevodina E
- Vogel M
- Vokac P
- Von Ahnen J
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vozak M
- Vozdecky L
- Vranjes N
- Vrba V
- Vreeswijk M
- Vu NK
- Vuillermet R
- Vujinovic OV
- Vukotic I
- Wada S
- Wagner C
- Wagner W
- Wahdan S
- Wahlberg H
- Wakasa R
- Wakida M
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Walls FMG
- Wang AM
- Wang AZ
- Wang C
- Wang C
- Wang H
- Wang J
- Wang P
- Wang R
- Wang R
- Wang R-J
- Wang S
- Wang SM
- Wang T
- Wang WT
- Wang WX
- Wang X
- Wang X
- Wang X
- Wang Y
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- Wanotayaroj C
- Warburton A
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- Warrack N
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- Webb AF
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- Weber MS
- Weber SA
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- Wei C
- Wei Y
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
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- Wendland B
- Wengler T
- Wenig S
- Wermes N
- Wessels M
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- Wharton AM
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- White MJ
- Whiteson D
- Wickremasinghe L
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilbern DJ
- Wilkens HG
- Wilkins LJ
- Williams DM
- Williams HH
- Williams S
- Willocq S
- Windischhofer PJ
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Wongel AF
- Worm SD
- Wosiek BK
- Woźniak KW
- Wraight K
- Wu J
- Wu SL
- Wu X
- Wu Y
- Wu Z
- Wuerzinger J
- Wyatt TR
- Wynne BM
- Wölker R
- Xella S
- Xia L
- Xia M
- Xiang J
- Xiao X
- Xie M
- Xie X
- Xiotidis I
- Xu D
- Xu H
- Xu L
- Xu R
- Xu T
- Xu W
- Xu Y
- Xu Z
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yamaguchi N
- Yamaguchi Y
- Yamatani M
- Yamauchi H
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan S
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang X
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yuan M
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zagazeta LFG
- Zaid E
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeißner SV
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- 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
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/07/2022
- Field of study