306 research outputs found
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
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- Yin P
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- Zaid E
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- Zakharchuk N
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- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
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- Zerwas D
- Zhai M
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- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao T
- Zhao Y
- Zhao Z
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- 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
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
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
- 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
- Amos KR
- Amrouche CS
- Ananiev V
- 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
- Appelt C
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- 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
- Assamagan K
- Astalos R
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- Zhemchugov A
- Zheng Z
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- Zorbas TG
- Zormpa O
- Zou W
- 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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- Yildiz H Duran
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- Yue X
- Zaazoua M
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- Zagazeta LF Gutierrez
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- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
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- Zhang DF
- Zhang G
- Zhang J
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- Zhang R
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- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhou H
- Zhou N
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- Zhu CG
- Zhu H
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
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- 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
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- 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
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- Addepalli SV
- Adelman J
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- Agaras MN
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- Alberghi GL
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- Aleksandrov IN
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- Zhemchugov A
- Zheng Z
- Zhong D
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- 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
- '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
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
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- Abusleme Hoffman AC
- Acharya BS
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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
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
Constraints on Higgs boson production with large transverse momentum using H \rightarrow b\bar{b} decays in the ATLAS detector
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- Zeißner SV
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- Zenger DT
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- Zhemchugov A
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
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- 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
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)
- Author
- Aad G
- Abbott B
- Abbott Dc
- Abed Abud A
- Abeling K
- 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
- 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
- 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
- Amelung C
- Ames Cg
- 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
- Appelt C
- Aranzabal N
- Araujo Ferraz V
- Arcangeletti C
- Arce Ath
- Arena E
- Arguin J
- Argyropoulos S
- Arling J-
- Armbruster Aj
- Arnaez O
- Arnold H
- Arrubarrena Tame Zp
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah Na
- Asimakopoulou Em
- Assahsah J
- Assamagan K
- Astalos R
- Atkin Rj
- Atkinson M
- Atlay Nb
- Atmani H
- Atmasiddha Pa
- Augsten K
- Auricchio S
- Auriol Ad
- Austrup Va
- Avner G
- Avolio G
- Axiotis K
- Ayoub Mk
- Azuelos G
- Åkesson Tpa
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahmani M
- Bailey Aj
- Bailey Vr
- Baines Jt
- Bakalis C
- Baker Ok
- Bakker Pj
- Bakos E
- Bakshi Gupta D
- Balaji S
- Balasubramanian R
- Baldin Em
- Balek P
- Ballabene E
- Balli F
- Baltes Lm
- Balunas Wk
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barberio El
- Barberis D
- Barbero M
- Barbour G
- Barends Kn
- Barillari T
- Barisits M
- Barkeloo J
- Barklow T
- Barnett Rm
- Baron Moreno Da
- Baron P
- Baroncelli A
- Barone G
- Barr Aj
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- Barreiro F
- Barron U
- Barsov S
- Bartels F
- Bartoldus R
- Barton Ae
- Bartos P
- Basalaev A
- Basan A
- Baselga M
- Bashta I
- Bassalat A
- Basso Mj
- Basson Cr
- Bates Rl
- Batlamous S
- Batley Jr
- Batool B
- Battaglia M
- Bauce M
- Bauer P
- Bayirli A
- Beacham Jb
- Beau T
- Beauchemin Ph
- Becherer F
- Bechtle P
- Beck Hp
- Becker K
- Becot C
- Beddall Aj
- Bednyakov Va
- Bee Cp
- Beemster Lj
- Beermann Ta
- Begalli M
- Begel M
- Behera A
- Behr Jk
- Beirao Da Cruz E Silva C
- Beirer Jf
- Beisiegel F
- Belfkir M
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev Nl
- Benchekroun D
- Benhammou Y
- Benjamin Dp
- Benoit M
- Bensinger Jr
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Bergmann B
- Beringer J
- Berlendis S
- Bernardi G
- Bernius C
- Bernlochner Fu
- Berry T
- Berta P
- Berthold A
- Bertram Ia
- Bessidskaia Bylund O
- Bethke S
- Betti A
- Bevan Aj
- Bhatta S
- Bhattacharya Ds
- Bhattarai P
- Bhopatkar Vs
- Bi R
- Bi R
- Bianchi Rm
- Biebel O
- Bielski R
- Biesuz Nv
- Biglietti M
- Billoud Trv
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Biondini A
- Birch-sykes Cj
- Bird Ga
- Birman M
- Bisanz T
- Biswas D
- Bitadze A
- Bjørke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- 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
- Borecka-Bielska Hm
- Borgna Ls
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola Jd
- Bouaouda K
- Boudreau J
- Bouhova-Thacker Ev
- Boumediene D
- Bouquet R
- Boveia A
- Boyd J
- Boye D
- Boyko Ir
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau Je
- Breaden Madden Wd
- Brendlinger K
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Brickwedde B
- Britton D
- Britzger D
- Brock I
- Brooijmans G
- Brooks Wk
- Brost E
- Bruckman de Renstrom Pa
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Brüers B
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley Ag
- Budagov Ia
- Bugge Mk
- Bulekov O
- Bullard Ba
- Burdin S
- Burgard Cd
- Burger Am
- Burghgrave B
- Burr Jtp
- Burton Cd
- Burzynski Jc
- Busch El
- Bussey Pj
- Butler Jm
- Buttar Cm
- Butterworth Jm
- Buttinger W
- Buxo Vazquez Cj
- Buzykaev Ar
- Büscher V
- Cabras G
- Cabrera Urbán S
- Caforio D
- Cai H
- Cai Y
- Cairo Vmm
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba Lp
- Calvet D
- Calvet S
- Calvet Tp
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Camerlingo Mt
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cano Bret M
- Cantero J
- Cao Y
- Capocasa F
- Capua M
- Carbone A
- Cardarelli R
- Cardenas Jcj
- Cardillo F
- Carli T
- Carlino G
- Carlson Bt
- Carlson Em
- Carminati L
- Carnesale M
- Caron S
- Carquin E
- Carratta G
- Carrá S
- Carter Jws
- Carter Tm
- Casado Mp
- Casha Af
- Castiglia Eg
- Castillo Garcia L
- Castillo Gimenez V
- Castillo Fl
- Castro Nf
- Catinaccio A
- Catmore Jr
- Cavaliere V
- Cavalli N
- Cavasinni V
- Celebi E
- Celli F
- Centonze Ms
- Cerny K
- Cerqueira As
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin Sa
- Chadi Z
- Chakraborty D
- Chala M
- Chan J
- Chan Ws
- Chan Wy
- Chapman Jd
- Chargeishvili B
- Charlton Dg
- Charman Tp
- Chatterjee M
- Chekanov S
- Chekulaev Sv
- Chelkov Ga
- Chen A
- Chen B
- Chen B
- Chen C
- Chen H
- Chen H
- Chen J
- Chen J
- Chen S
- Chen Sj
- Chen X
- Chen X
- Chen Y
- Cheng Cl
- Cheng Hc
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cherkaoui El Moursli R
- 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 Eys
- Chowdhury T
- Christopher Ld
- Chu Kl
- Chu Mc
- Chu X
- Chudoba J
- Chwastowski Jj
- Cieri D
- Ciesla Km
- Cindro V
- Ciocio A
- Cirotto F
- Citron Zh
- Citterio M
- Ciubotaru Da
- Ciungu Bm
- Clark A
- Clark Pj
- Clavijo Columbie Jm
- Clawson Se
- Clement C
- Clercx J
- Clissa L
- Coadou Y
- Cobal M
- Coccaro A
- Coelho Barrue Rf
- Coelho Lopes De Sa R
- Coelli S
- Cohen H
- Coimbra Aec
- Cole B
- Collot J
- Conde Muiño P
- Connell Sh
- Connelly Ia
- Conroy Ei
- Conventi F
- Cooke Hg
- Cooper-Sarkar Am
- Cormier F
- Corpe Ld
- Corradi M
- Corrigan Ee
- Corriveau F
- Cortes-Gonzalez A
- Costa Mj
- Costanza F
- Costanzo D
- Cote Bm
- Cowan G
- Cowley Jw
- Cranmer K
- Crescioli F
- Crépé-Renaudin S
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosetti G
- Cueto A
- Cuhadar Donszelmann T
- Cui H
- Cui Z
- Cukierman Ar
- Cunningham Wr
- Curcio F
- Czodrowski P
- Czurylo Mm
- D'Amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- D'Onofrio A
- D'Onofrio M
- D'Uffizi M
- Da Cunha Sargedas De Sousa Mj
- Da Fonseca Pinto Jv
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damp J
- Dandoy Jr
- Daneri Mf
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Das Sj
- Dattagupta A
- David C
- Davidek T
- Davis Dr
- Davis-Purcell B
- Dawson I
- De Asmundis R
- De Beurs M
- De Castro S
- De Groot N
- de Jong P
- De la Torre H
- De Maria A
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Vivie De Regie Jb
- De K
- Dedovich Dv
- Degens J
- Deiana Am
- Del Corso F
- Del Peso J
- Del Rio F
- Deliot F
- Delitzsch Cm
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delsart Pa
- Demers S
- Demichev M
- Denisov Sp
- Derendarz D
- Derue F
- Dervan P
- Desch K
- Dette K
- Deutsch C
- Deviveiros Po
- Di Bello Fa
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
- Di Nardo R
- Diaconu C
- Dias Do Vale T
- Dias Fa
- Diaz Capriles Fg
- Diaz Ma
- Didenko M
- Diehl Eb
- Diehl L
- Diez Pardos C
- Dimitriadi C
- Dimitrievska A
- Ding W
- Dingfelder J
- Dinu I
- Dittmeier Sj
- Dittus F
- Díez Cornell S
- Djama F
- Djobava T
- Djuvsland Ji
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Donadelli M
- Dong B
- Donini J
- Dopke J
- Doria A
- Dova Mt
- Doyle At
- Draguet Ma
- Drechsler E
- Dreyer E
- Drivas-koulouris I
- Drobac As
- du Pree Ta
- Du D
- Dubinin F
- Dubovsky M
- Duchovni E
- Duckeck G
- Ducu Oa
- Duda D
- Dudarev A
- Duflot L
- Dumitriu Ae
- Dunford M
- Dungs S
- Dunne K
- Duperrin A
- Duran Yildiz H
- Durglishvili A
- Dührssen M
- Dülsen C
- Düren M
- Dwyer Bl
- Dyckes Gi
- Dyndal M
- Dysch S
- Dziedzic Bs
- Eckerova B
- Eggleston Mg
- Egidio Purcino De Souza E
- Ehrke Lf
- Eigen G
- Einsweiler K
- Ekelof T
- Ekman Pa
- El Ghazali Y
- El Jarrari H
- El Moussaouy A
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot Aa
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Emerman A
- Enari Y
- Ene I
- Epari S
- Erdmann J
- Ereditato A
- Erland Pa
- Errenst M
- Escalier M
- Escobar C
- Etzion E
- Evans G
- Evans H
- Evans Mo
- Ezhilov A
- Ezzarqtouni S
- Fabbri F
- Fabbri L
- Facini G
- Fadeyev V
- Fakhrutdinov Rm
- Falciano S
- Falke Pj
- Falke S
- Faltova J
- Fan Y
- Fang Y
- Fanourakis G
- Fanti M
- Faraj M
- Farbin A
- Farilla A
- Farooque T
- Farrington Sm
- Fassi F
- Fassouliotis D
- Faucci Giannelli M
- Fawcett Wj
- Fayard L
- Fedin Ol
- Fedotov G
- Feickert M
- Feligioni L
- Fell A
- Fellers De
- Feng C
- Feng M
- Fenton Mj
- Fenyuk Ab
- Ferencz L
- Ferguson Sw
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrere D
- Ferretti C
- Fiedler F
- Filipčič A
- Filmer Ek
- Filthaut F
- Fiolhais Mcn
- Fiorini L
- Fischer F
- Fisher Wc
- Fitschen T
- Fleck I
- Fleischmann P
- Flick T
- Flores Castillo Lr
- Flores L
- Flores M
- Follega Fm
- Fomin N
- Foo Jh
- Forland Bc
- Formica A
- Forti Ac
- Fortin E
- Fortman Aw
- Foti Mg
- Fountas L
- Fournier D
- Fox H
- Francavilla P
- Francescato S
- Franchini M
- Franchino S
- Francis D
- Franco L
- Franconi L
- Franklin M
- Frattari G
- Freegard Ac
- Freeman Pm
- Freund Ws
- Fritzsche N
- Froch A
- Froidevaux D
- Frost Ja
- Fu Y
- Fujimoto M
- Fullana Torregrosa E
- Fuster J
- Gabrielli A
- Gabrielli A
- Gadow P
- Gagliardi G
- Gagnon Lg
- Gallardo Ge
- Gallas Ej
- Gallop Bj
- Gamboa Goni R
- Gan Kk
- Ganguly S
- Gao J
- Gao Y
- Garay Walls Fm
- Garcia B
- Garcia-Sciveres M
- García Navarro Je
- García Pascual Ja
- García C
- Gardner Rw
- Garg D
- Garg Rb
- Gargiulo S
- Garner Ca
- Garonne V
- Gasiorowski Sj
- Gaspar P
- Gaudio G
- Gauzzi P
- Gavrilenko Il
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis En
- Geanta Aa
- Gee Cm
- Geisen J
- Geisen M
- Gemme C
- Genest Mh
- Gentile S
- George S
- George Wf
- Geralis T
- Gerlach Lo
- Gessinger-Befurt P
- Ghasemi Bostanabad M
- Ghneimat M
- Ghosal A
- Ghosh A
- Ghosh A
- Giacobbe B
- Giagu S
- Giangiacomi N
- Giannetti P
- Giannini A
- Gibson Sm
- Gignac M
- Gil Dt
- Gilbert Ak
- Gilbert Bj
- Gillberg D
- Gilles G
- Gillwald Nek
- Ginabat L
- Gingrich Dm
- Giordani Mp
- Giraud Pf
- Giugliarelli G
- Giugni D
- Giuli F
- Gkialas I
- Gladilin Lk
- Glasman C
- Gledhill Gr
- Glisic M
- Gnesi I
- Go Y
- Goblirsch-Kolb M
- Gocke B
- Godin D
- Goldfarb S
- Golling T
- Gololo Mgd
- Golubkov D
- Gombas Jp
- Gomes A
- Gomez Delegido Aj
- Goncalves Gama R
- Gonçalo R
- Gonella G
- Gonella L
- Gongadze A
- Gonnella F
- Gonski Jl
- Gonzalez Fernandez S
- Gonzalez Lopez R
- Gonzalez Renteria C
- Gonzalez Suarez R
- Gonzalez-Sevilla S
- Gonzalvo Rodriguez Gr
- González Andana Ry
- González de la Hoz S
- Goossens L
- Gorasia Na
- Gorbounov Pa
- Gorini B
- Gorini E
- Gorišek A
- Goshaw At
- Gostkin Mi
- Gottardo Ca
- Gouighri M
- Goumarre V
- Goussiou Ag
- Govender N
- Goy C
- Grabowska-Bold I
- Graham K
- Gramstad E
- Grancagnolo S
- Grandi M
- Gratchev V
- Gravila Pm
- Gravili Fg
- Gray Hm
- Greco M
- Grefe C
- Gregor Im
- Grenier P
- Grieco C
- Grillo Aa
- Grimm K
- Grinstein S
- Grivaz J-
- Gross E
- Grosse-Knetter J
- Grud C
- Grummer A
- Grundy Jc
- Guan L
- Guan W
- Gubbels C
- Guerrero Rojas Jgr
- Guerrieri G
- Guescini F
- Gugel R
- Guhit Jam
- Guida A
- Guillemin T
- Guilloton E
- Guindon S
- Guo F
- Guo J
- Guo L
- Guo Y
- Gupta R
- Gurbuz S
- Gustavino G
- Guth M
- Gutierrez Zagazeta Lf
- Gutierrez P
- Gutschow C
- Guyot C
- Gwenlan C
- Gwilliam Cb
- Haaland Es
- Haas A
- Habedank M
- Haber C
- Hadavand Hk
- Hadef A
- Hadzic S
- Haleem M
- Haley J
- Hall Jj
- Hallewell Gd
- Halser L
- Hamano K
- Hamdaoui H
- Hamer M
- Hamity Gn
- Han J
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- Han Yf
- Hanagaki K
- Hance M
- Hangal Da
- Hank Md
- Hankache R
- Hansen Jb
- Hansen Jd
- Hansen Ph
- Hara K
- Harada D
- Harenberg T
- Harkusha S
- Harris Yt
- Harrison Pf
- Hartman Nm
- Hartmann Nm
- Hasegawa Y
- Hasib A
- Haug S
- Hauser R
- Havranek M
- Hawkes Cm
- Hawkings Rj
- Hayashida S
- Hayden D
- Hayes C
- Hayes Rl
- Hays Cp
- Hays Jm
- Hayward Hs
- He F
- He Y
- He Y
- Heath Mp
- Hedberg V
- Heggelund Al
- Hehir Nd
- Heidegger C
- Heidegger Kk
- Heidorn Wd
- Heilman J
- Heim S
- Heim T
- Heinemann B
- Heinlein Jg
- Heinrich Jj
- Heinrich L
- Hejbal J
- Helary L
- Held A
- Hellesund S
- Helling Cm
- Hellman S
- Helsens C
- Henderson Rcw
- Henkelmann L
- Henriques Correia Am
- Herde H
- Hernández Jiménez Y
- Herr H
- Herrmann Mg
- Herrmann T
- Herten G
- Hertenberger R
- Hervas L
- Hessey Np
- Hibi H
- Higón-Rodriguez E
- Hillier Sj
- Hinchliffe I
- Hinterkeuser F
- Hirose M
- Hirose S
- Hirschbuehl D
- Hiti B
- Hobbs J
- Hobincu R
- Hod N
- Hodgkinson Mc
- Hodkinson Bh
- Hoecker A
- Hofer J
- Hohn D
- Holm T
- Holzbock M
- Hommels Lbah
- Honan Bp
- Hong J
- Hong Tm
- Hong Y
- Honig Jc
- Hooberman Bh
- Hopkins Wh
- Horii Y
- Hou S
- Howarth J
- Hoya J
- Hönle A
- Hrabovsky M
- Hryn'Ova T
- Hrynevich A
- Hsu Pj
- Hsu S-
- Hu Q
- Hu Yf
- Huang Dp
- Huang S
- Huang X
- Huang Y
- Huang Y
- Huang Z
- Hubacek Z
- Huebner M
- Huegging F
- Huffman Tb
- Huhtinen M
- Huiberts Sk
- Hulsken R
- Huseynov N
- Huston J
- Huth J
- Hyneman R
- Hyrych S
- Iacobucci G
- Iakovidis G
- Ibragimov I
- Iconomidou-Fayard L
- Iengo P
- Iguchi R
- Iizawa T
- Ikegami Y
- Ilg A
- Ilic N
- Imam H
- Ingebretsen Carlson T
- Introzzi G
- Iodice M
- Ippolito V
- Ishino M
- Islam W
- Issever C
- Istin S
- Ito H
- Iturbe Ponce Jm
- Iuppa R
- Ivina A
- Izen Jm
- Izzo V
- Jacka P
- Jackson P
- Jacobs Rm
- Jaeger Bp
- Jagfeld Cs
- Jakobs K
- Jakoubek T
- Jamieson J
- Janas Kw
- Jarlskog G
- Jaspan Ae
- Javurkova M
- Javůrek T
- Jäkel G
- Jeanneau F
- Jeanty L
- Jejelava J
- Jenni P
- Jessiman Ce
- Jézéquel S
- Jia J
- Jia X
- Jia X
- Jia Z
- Jiang Y
- Jiggins S
- Jimenez Pena J
- Jin S
- Jinaru A
- Jinnouchi O
- Jivan H
- Johansson P
- Johns Ka
- Johnson Ca
- Jones Dm
- Jones E
- Jones Rwl
- Jones Tj
- Jovicevic J
- Ju X
- Junggeburth Jj
- Juste Rozas A
- Kabana S
- Kaczmarska A
- Kado M
- Kagan H
- Kagan M
- Kahn A
- Kahn A
- Kahra C
- Kaji T
- Kajomovitz E
- Kakati N
- Kalderon Cw
- Kamenshchikov A
- Kang Nj
- Kano Y
- Kar D
- Karava K
- Kareem Mj
- Karentzos E
- Karkanias I
- Karpov Sn
- Karpova Zm
- Kartvelishvili V
- Karyukhin An
- Kasimi E
- Kato C
- Katzy J
- Kaur S
- Kawade K
- Kawagoe K
- Kawaguchi T
- Kawamoto T
- Kawamura G
- Kay Ef
- Kaya Fi
- Kazakos S
- Kazanin Vf
- Ke Y
- Keaveney Jm
- Keeler R
- Kehris Gv
- Keller Js
- Kelly As
- Kelsey D
- Kempster Jj
- Kendrick J
- Kennedy Ke
- Kepka O
- Kerridge Bp
- Kersten S
- Kerševan Bp
- Keszeghova L
- Ketabchi Haghighat S
- Khandoga M
- Khanov A
- Kharlamov Ag
- Kharlamova T
- Khoda Ee
- Khoo Tj
- Khoriauli G
- Khubua J
- Khwaira Yar
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- Kilgallon A
- Kim E
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- Kirfel C
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- Kishimoto T
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- Klassen M
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- Klimek P
- Klimentov A
- Klimpel F
- Klingl T
- Klioutchnikova T
- Klitzner Ff
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- Knight Tm
- Knue A
- Kobayashi D
- Kobayashi R
- Kocian M
- Kodama T
- Kodyš P
- Koeck Dm
- Koenig Pt
- Koffas T
- Kolb M
- Koletsou I
- Komarek T
- Kong Axy
- Kono T
- Konstantinidis N
- Konya B
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- Koperny S
- Korcyl K
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- Korolkov I
- Korotkova N
- Kortman B
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- Kostecka Wh
- Kostyukhin Vv
- Kotsokechagia A
- Kotwal A
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- Kourkoumeli-Charalampidi A
- Kourkoumelis C
- Kourlitis E
- Kovanda O
- Kowalewski R
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- Kramarenko Va
- Kramberger G
- Kramer P
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- Kumari N
- Kuna M
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- Kupfer T
- Kupich A
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- Kurchaninov Ll
- Kurochkin Ya
- Kurova A
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- Lakomiec Ik
- Lalloue N
- Lambert Je
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- Lançon E
- Landgraf U
- Landon Mpj
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- Langenberg Rj
- Lankford Aj
- Lanni F
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- Lanza A
- Lapertosa A
- Laporte Jf
- Lari T
- Lasagni Manghi F
- Lassnig M
- Latonova V
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- Laudrain A
- Laurier A
- Lawlor Sd
- Lawrence Z
- Lazzaroni M
- Le B
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- Lebedev A
- Leblanc M
- Lecompte T
- Ledroit-Guillon F
- Lee Aca
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- Lipniacka A
- Liss Tm
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- Liu D
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- Walkowiak W
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- Wilbern Dj
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- Wittgen M
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- Wosiek Bk
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- Yexley Mr
- Yin P
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- Yuan M
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- Zakharchuk N
- Zambito S
- Zang J
- Zanzi D
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- Zeitnitz C
- Zeißner Sv
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
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- Živković L
- Publication venue
- ELSEVIER
- Publication date
- 01/01/2023
- Field of study
International Consensus Statement on Rhinology and Allergy: Rhinosinusitis
- Author
- Aanaes K
- Abadie WM
- Abi Najm S
- Abigail P
- Abrahams JJ
- Abrass LJ
- Abreu CB
- Abreu NA
- Abshirini H
- Abuzeid WM
- Abuzeid WM
- Achar P
- Ackerhans M
- Adam P
- Adappa ND
- Adappa ND
- Adappa ND
- Adappa ND
- Adriaensen G
- Agache I
- Aghamohammadi A
- Agius AM
- Agyeman AA
- Ahn CN
- Ahn HJ
- Ahn JC
- Ahn SH
- Ahovuo‐Saloranta A
- Aitken M
- Ajaiyeoba A
- Akbari E
- Akdis CA
- Akira S
- Akiyama K
- Akiyama K
- Akiyama K
- Al Komser MK
- Alam ES
- Alandejani T
- Alanin MC
- Albritton FDT
- Albu S
- Albu S
- Albu S
- Aldini G
- Alexander NS
- Aljebab F
- Alkire BC
- Allen EK
- Alobid I
- Alobid I
- Alobid I
- Aloulah M
- Alqudah M
- Alromaih S
- Alsaleh S
- Alsharif S
- Alt JA
- Alt JA
- Alt JA
- Alt JA
- Alt JA
- Alves MP
- Al‐Qudah M
- Al‐Qudah M.
- Al‐Qudah M.
- Al‐Rawi MM
- Al‐Shaikh S
- Al‐Shemari H
- Al‐Swiahb JN
- Amali A
- Amar YG
- Amble FR
- American Academy of Pediatrics Steering Committee on Quality Improvement and Management (AAP SCQIM)
- Amin MR
- Amine M
- Amodu EJ
- Anamika A
- Anand V
- Anderson DE
- Anderson WC
- Andhale S
- Ankichetty SP
- Annamalai S
- Anon JB
- Anselmo‐Lima WT
- Antisdel JL
- Antisdel JL
- Antunes MB
- Antunes MB
- Anushiravani M
- Anzai Y
- Anzić SA
- Aramani A
- Arden KE
- Arild Danielsen K
- Aring AM
- Arjomandi H
- Armenaka M
- Arnstead N
- Arslan H
- Arslan HH
- Asaka D
- Asero R
- Asero R
- Atighechi S
- Atlas SJ
- Au J
- Aukema AA
- Aurora R
- Autio TJ
- Autio TJ
- Autio TJ
- Autio TJ
- Avdeeva K
- Awad OG
- Awad OGA
- Ayers CM
- Ayoub N
- Ayoub N
- Ayoub N
- Azbell C
- Azila A
- Baba S
- Baba S
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- Babinski D
- Bachert C
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- Bachert C
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- Bae JS
- Bagheri SHR
- Baguley C
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- Balk EM
- Bang YJ
- Banhiran W
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- Baraniuk JN
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- Barham HP
- Barham HP
- Barham HP
- Baroody FM
- Basharat U
- Bassiouni A
- Bassiouni A
- Bassiouni A
- Batikhan H
- Batra PS
- Batra PS
- Batra PS
- Baudoin T
- Baumann A
- Bayonne E
- Becker SS
- Bednarski KA
- Behan L
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- Beule AG
- Beyea JA
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- Bhattacharyya N
- Bhattacharyya N
- Bhattacharyya N
- Bhattacharyya N
- Bhattacharyya N
- Bhattacharyya N
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- Bhattacharyya N
- Bhattacharyya N
- Bhattacharyya N.
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- Bhawana G
- Bidder T
- Biedlingmaier JF
- Biedlingmaier JF
- Biedlingmaier JF.
- Biel MA
- Biel MA
- Bikhazi N
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- Biswas K
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- Bizaki AJ
- Blackwell DL
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- Blount A
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- Boezaart AP
- Bohman A
- Bohman A
- Bohnhorst I
- Boita MM
- Bolger WE
- Bolger WE
- Bolger WE
- Bomeli SR
- Bondioni MP
- Bonfils P
- Bonfils P
- Bonfils P
- Bonnomet A
- Boonmak P
- Borish L
- Borsetto D
- Bosse Y
- Bosso JV
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- Bousquet J
- Bousquet J
- Brandsted R
- Braun JJ
- Braun JJ
- Braunstahl GJ
- Braverman I
- Brescia G
- Brescia G
- Brietzke SE
- Brietzke SE
- Brodner D
- Brook I
- Brook I
- Brook I
- Brook I
- Brook I.
- Brook I.
- Bross‐Soriano D
- Brot C
- Brown CL
- Brown S
- Brozek JL
- Brozek JL
- Brumund KT
- Brunner JP
- Buckley CE
- Buehring I
- Bugten V
- Bukowy‐Bieryllo Z
- Burgstaller JM
- Burton BN
- Bush A
- Businco LD
- Buysschaert ID
- Byun JY
- Cahill KN
- Cai Y
- Calhoun KH
- Calixto NE
- Callejas CA
- Campbell AP
- Campbell AP
- Campbell RG
- Campbell RG.
- Candoni A
- Cannady SB
- Cannoni M
- Canonica GW
- Cantrell H.
- Cao PP
- Cao P‐P
- Cao Y
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- Chakrabarti A
- Chalermwatanachai T
- Chalton R
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- Chandra RK
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- Chandra RK
- Chandra RK
- Chandy Z
- Chang CC
- Chang CC
- Chang EH
- Chang EH
- Chang EH
- Chang HS
- Chang MT
- Chang MT
- Chang MT
- Chang Y‐S
- Chaudhary N
- Che C
- Chee L
- Chen B
- Chen B
- Chen CF
- Chen F
- Chen FH
- Chen H
- Chen J‐B
- Chen PH
- Chen X
- Chen YT
- Cheng YK
- Cheon YI
- Chester AC
- Chester AC
- Chester AC
- Chiarella SE
- Chiesa‐Estomba CM
- Chin D
- Chinratanapisit S
- Chiu A
- Chiu AG
- Chiu AG
- Chiu AG
- Cho DY
- Cho DY
- Cho DY
- Cho DY
- Cho DY
- Cho DY
- Cho DY
- Cho DY
- Cho DY
- Cho GS
- Cho HJ
- Cho JH
- Cho K
- Cho KS
- Cho KS
- Cho SH
- Cho SH
- Cho SH
- Chobillon MA
- Choby G
- Choby GW
- Choi EB
- Choi JH
- Chong LY
- Chong LY
- Chong LY
- Chow AW
- Chowdhury NI
- Chowdhury NI
- Christensen DN
- Christensen JM
- Chu DK
- Chung BJ
- Chung SD
- Church CA
- Cirkovic I
- Citardi MJ
- Citardi MJ
- Claeys S
- Claeys S
- Clarhed UKE
- Clark DW
- Clark NM
- Clayman GL
- Cleland EJ
- Cleland EJ
- Cleland EJ
- Clement PA
- Clinger JD
- Clunes LA
- Coates ML
- Codispoti CD
- Coey JG
- Cohen NA
- Cohen NA
- Collins FS
- Collins FS
- Collins MM
- Comert S
- Conboy P
- Conger BT
- Conger BT
- Conley DB
- Cope EK
- Copeland E
- Cormier C
- Cormier C
- Cornelius RS
- Cornet ME
- Corradini C
- Corriveau M‐N
- Costa Carvalho BT
- Costa ML
- Costa ML
- Costerton JW
- Cottrell J
- Craig JR
- Craig JR.
- Crawley BK
- Criddle MW
- Cronin MJ
- Crosby DL
- Cross JL
- Crotty Alexander LE
- Cryan JF
- Cui XY
- Cui YH
- Cutler J
- Cutler J
- Cutting GR
- Czerny MS
- Côté DWJ
- D'Anza B
- Dabirmoghaddam P
- Dahlen B
- Dai Q
- Dalgic A
- Dalgorf DM
- Dalm VA
- Daramola OO
- Darveaux J
- Das A
- Daudia AT
- Dautremont JF
- Davis GE
- Dawson B
- Dawson B
- De Boeck I
- De Greve G
- De Schryver E
- De Schryver E
- DeConde AS
- DeConde AS
- DeConde AS
- DeConde AS
- DeConde AS
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- DeConde AS
- DeConde AS
- Dejima K
- Dejima K
- Delehaye E
- Delemarre T
- DelGaudio JM
- DelGaudio JM
- DelGaudio JM
- DelGaudio JM
- DelGaudio JM
- Dellamonica P
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- Demirhan A
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- DeMuri GP
- DeMuri GP
- DeMuri GP
- Den Beste KA
- den Broek MF
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- Denlinger LC
- Derendorf H
- Derry S
- deShazo RD
- Deshazo RD.
- Desrosiers M
- Desrosiers M
- Desrosiers M
- Desrosiers M
- Desrosiers MY
- Detwiller KY
- Deutsch PG
- DeYoung K
- Dhawale VS
- Di Capite J
- Di Cicco M
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- Dietz CJ
- Dietz de Loos D
- Dietz de Loos DA
- Dijkstra MD
- Dilger AE
- Dilidaer D
- Dilokthornsakul P
- Dingsor G
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- Divekar RD
- Dixon AE
- Dixon BJ
- Djupesland PG
- Djupesland PG
- Djupesland PG
- Do TQ
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- Doellman MS
- Dogan M
- Dolor RJ
- Don DM
- Dong D
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- Druce HM
- Du K
- Dubin MG
- Dubin MG
- Dubin MG
- Dubin MR
- Duclos P
- Dunbar J
- Dunlop G
- Durr ML
- Dutta M
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- Dykewicz MS
- Dykewicz MS
- Ebbens FA
- Ebbens FA
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- Ebell MH
- Eberhart LH
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- Ecevit MC
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- Eggesbo HB.
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- Ehnhage A
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- Passali D
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- Patel NA
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- Peng Y
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- Perloff JR
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- Ramakrishnan V
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- Rotenberg BW
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- Schwarzbach HL
- Schwitzguébel AJ‐P
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- Sedaghat AR
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- Snidvongs K
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- Snow DG
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- Zuckerman JD
- Zurlo JJ
- Zuskin E
- Čulig J
- Publication venue
- 'Wiley'
- Publication date
- 01/01/2021
- Field of study
Background: The 5 years since the publication of the first International Consensus Statement on Allergy and Rhinology: Rhinosinusitis (ICAR‐RS) has witnessed foundational progress in our understanding and treatment of rhinologic disease. These advances are reflected within the more than 40 new topics covered within the ICAR‐RS‐2021 as well as updates to the original 140 topics. This executive summary consolidates the evidence‐based findings of the document. Methods: ICAR‐RS presents over 180 topics in the forms of evidence‐based reviews with recommendations (EBRRs), evidence‐based reviews, and literature reviews. The highest grade structured recommendations of the EBRR sections are summarized in this executive summary. Results: ICAR‐RS‐2021 covers 22 topics regarding the medical management of RS, which are grade A/B and are presented in the executive summary. Additionally, 4 topics regarding the surgical management of RS are grade A/B and are presented in the executive summary. Finally, a comprehensive evidence‐based management algorithm is provided. Conclusion: This ICAR‐RS‐2021 executive summary provides a compilation of the evidence‐based recommendations for medical and surgical treatment of the most common forms of RS
Accuracy versus precision in boosted top tagging with the ATLAS detector
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- Filipčič A
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- Filthaut F
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- Fisher WC
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- Fitzhugh PM
- Fleck I
- Fleischmann P
- Flick T
- Flores CAA
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- Follega FM
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- Formica A
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- Zhemchugov A
- Zheng J
- Zheng K
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- Zhong D
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- 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
- IOP Publishing
- Publication date
- 01/08/2024
- Field of study
Abstract
The identification of top quark decays where the top quark has a large momentum transverse to the beam axis, known as top tagging, is a crucial component in many measurements of Standard Model processes and searches for beyond the Standard Model physics at the Large Hadron Collider.
Machine learning techniques have improved the performance of top tagging algorithms, but the size of the systematic uncertainties for all proposed algorithms has not been systematically studied.
This paper presents the performance of several machine learning based top tagging algorithms on a dataset constructed from simulated proton-proton collision events measured with the ATLAS detector at √
s
= 13 TeV.
The systematic uncertainties associated with these algorithms are estimated through an approximate procedure that is not meant to be used in a physics analysis, but is appropriate for the level of precision required for this study.
The most performant algorithms are found to have the largest uncertainties, motivating the development of methods to reduce these uncertainties without compromising performance.
To enable such efforts in the wider scientific community, the datasets used in this paper are made publicly available.</jats:p
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