318 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 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
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- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
A state-of-the-art review of curve squeal noise: Phenomena, mechanisms, modelling and mitigation
- Author
- A Matsumoto
- A Pieringer
- A Pieringer
- A. Pieringer
- AD Monk-Steel
- AH Wickens
- C Collette
- C Glocker
- CF Logston
- CJC Jones
- CJM Ruiten Van
- D Anderson
- D Curley
- DI Fletcher
- DI Fletcher
- DJ Fourie
- DJ Thompson
- DJ Thompson
- DJ Thompson
- DT Eadie
- DT Eadie
- DT Eadie
- E Kopp
- E Schneider
- EA Gallardo-Hernandez
- F Krüger
- FG Beer De
- G Squicciarini
- G Xie
- H Harrison
- H Ouyang
- H Stappenbeck Von
- I Zenzerovic
- I. Zenzerovic
- Inaki Merideno
- J Jiang
- J Jiang
- J Jiang
- JF Barman
- JF Brunel
- JF Brunel
- JF Garcia
- JG Giménez
- JJ Kalker
- JJ Sinou
- JR Koch
- K Kraft
- KL Johnson
- M Hiensch
- M Nakai
- M Nakai
- M Nakai
- MA Heckl
- MA Heckl
- MA Heckl
- MA Heckl
- MJ Rudd
- N Hoffmann
- N Hoffmann
- N Vincent
- NM Ghazaly
- NM Kinkaid
- O Chiello
- O Polach
- PJ Remington
- PJ Remington
- PJ Vermeulen
- R Illingworth
- R Stefanelli
- S Bruni
- S Bühler
- SS Hsu
- U Fingberg
- W Lang
- W Zhang
- X Liu
- X Liu
- X Liu
- X Liu
- Y Suda
- Z. Y. SHEN
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
[EN] Curve squeal is an intense tonal noise occurring when a rail vehicle negotiates a sharp curve. The phenomenon can be considered to be chaotic, with a widely differing likelihood of occurrence on different days or even times of day. The term curve squeal may include several different phenomena with a wide range of dominant frequencies and potentially different excitation mechanisms. This review addresses the different squeal phenomena and the approaches used to model squeal noise; both time-domain and frequency-domain approaches are discussed and compared. Supporting measurements using test rigs and field tests are also summarised. A particular aspect that is addressed is the excitation mechanism. Two mechanisms have mainly been considered in previous publications. In many early papers the squeal was supposed to be generated by the so-called falling friction characteristic in which the friction coefficient reduces with increasing sliding velocity. 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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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- Zenger DT
- Zenin O
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- Zerwas D
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- Zhemchugov A
- Zheng Z
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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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- Wosiek BK
- Wraight K
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- Wyatt TR
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- Xella S
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- Yao W-M
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- Yexley MR
- Yildiz H Duran
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yuan M
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zagazeta LF Gutierrez
- Zaid E
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaplatilek O
- Zeissner S
- Zeitnitz C
- Zeng JC
- Zenger DT
- Zenin O
- Zenis T
- 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 N
- Zimmermann S
- Zinsser J
- Ziolkowski M
- 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
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
- Abreu H
- Abud A Abed
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- Abusleme Hoffman AC
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
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- Zimmermann S
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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
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
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
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- Zemaityte G
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- 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
- 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
- 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
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- 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
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- 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
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- 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
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asawatavonvanich T
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Austrup VA
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Backman F
- Bagnaia P
- Bahilo JJL
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
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- Zenin O
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- Zhang Z
- Zhang Z
- Zhao P
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
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- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
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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- Zhemchugov A
- Zheng Z
- Zhong D
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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
- '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
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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- 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
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- Carter Tm
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- Casha Af
- Castiglia Eg
- Castillo Garcia L
- Castillo Gimenez V
- Castillo Fl
- Castro Nf
- Catinaccio A
- Catmore Jr
- Cavaliere V
- Cavalli N
- Cavasinni V
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- 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
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- Chen B
- Chen C
- Chen H
- Chen H
- Chen J
- Chen J
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- Chen Sj
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- 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
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- Cirotto F
- Citron Zh
- Citterio M
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- Ciungu Bm
- Clark A
- Clark Pj
- Clavijo Columbie Jm
- Clawson Se
- Clement C
- Clercx J
- Clissa L
- Coadou Y
- Cobal M
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- 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
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- 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
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- Dandoy Jr
- Daneri Mf
- Danninger M
- Dao V
- Darbo G
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- Das Sj
- Dattagupta A
- David C
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- 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
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- De Vivie De Regie Jb
- De K
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- Degens J
- Deiana Am
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- Del Peso J
- Del Rio F
- Deliot F
- Delitzsch Cm
- Dell'Acqua A
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- 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
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- Djama F
- Djobava T
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- Dodsworth D
- Doglioni C
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- Donadelli M
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- Donini J
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- Doria A
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- 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
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- 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
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- Ellajosyula V
- Ellert M
- Ellinghaus F
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- Emeliyanov D
- Emerman A
- Enari Y
- Ene I
- Epari S
- Erdmann J
- Ereditato A
- Erland Pa
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- Escalier M
- Escobar C
- Etzion E
- Evans G
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- Ezhilov A
- Ezzarqtouni S
- Fabbri F
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- Facini G
- Fadeyev V
- Fakhrutdinov Rm
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- Falke Pj
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- Faltova J
- Fan Y
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- Farooque T
- Farrington Sm
- Fassi F
- Fassouliotis D
- Faucci Giannelli M
- Fawcett Wj
- Fayard L
- Fedin Ol
- Fedotov G
- Feickert M
- Feligioni L
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- Fenyuk Ab
- Ferencz L
- Ferguson Sw
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- Ferrere D
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- Filipčič A
- Filmer Ek
- Filthaut F
- Fiolhais Mcn
- Fiorini L
- Fischer F
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- Fitschen T
- Fleck I
- Fleischmann P
- Flick T
- Flores Castillo Lr
- Flores L
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- Follega Fm
- Fomin N
- Foo Jh
- Forland Bc
- Formica A
- Forti Ac
- Fortin E
- Fortman Aw
- Foti Mg
- Fountas L
- Fournier D
- Fox H
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- Francescato S
- Franchini M
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- Francis D
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- Frattari G
- Freegard Ac
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- Freund Ws
- Fritzsche N
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- Froidevaux D
- Frost Ja
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- Fullana Torregrosa E
- Fuster J
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- Gadow P
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- Gessinger-Befurt P
- Ghasemi Bostanabad M
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- Gkialas I
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- Gnesi I
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- Gocke B
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- Golubkov D
- Gombas Jp
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- Gonzalvo Rodriguez Gr
- González Andana Ry
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- Goossens L
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- Gorbounov Pa
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- Goshaw At
- Gostkin Mi
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- Lopez Solis A
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- Lucio Alves Fl
- Lucotte A
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- Luise I
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- Lund-Jensen B
- Lundberg O
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- Lyubushkin V
- Lyubushkina T
- Ma H
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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
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- Aparo MA
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- Åkesson TPA
- Öncel ÖO
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- 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
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