32 research outputs found
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
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- 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
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- Alfonsi A
- Alfonsi F
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- Ali B
- Ali S
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- Allport PP
- Aloisio A
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- Alviggi MG
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- Amelung C
- Amidei D
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- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
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- Anders JK
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- Angelidakis S
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- Anisenkov AV
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- Aparo MA
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- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
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- Asada H
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- Asimakopoulou EM
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- Zhemchugov A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Direct constraint on the Higgs–charm coupling from a search for Higgs boson decays into charm quarks with the ATLAS detector
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- Ottino GJ
- Ouchrif M
- Ouellette J
- Ould-Saada F
- Outschoorn VIM
- Owen M
- Owen RE
- O’Keefe MW
- O’Neil DC
- O’neill AP
- O’Shea V
- Pardos CD
- Pascual JAG
- Paz IL
- Pena JJ
- Pietra MD
- Pino SAO
- Ponce JMI
- Pozo JAA
- Pree TAD
- Pretel JAF
- Ramos JM
- Renteria CG
- Rodriguez GRG
- Rojas JGRG
- Romero LM
- Rosende SJN
- Rozas AJ
- Sanchez FJM
- Santos SPAD
- Seabra LFO
- Sola JDB
- Solis AL
- Suarez PM
- Suarez RG
- Tame ZPA
- Toro RC
- Torregrosa EF
- Urbán SC
- Vazquez CJB
- Verzini MJA
- Volpe DD
- Walls FMG
- Yildiz HD
- Zagazeta LFG
- Åkesson TPA
- Öncel ÖO
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/08/2022
- Field of study
A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton–proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb−1. Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW, WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the (W/Z)Z(→cc¯) process and 3.8 (4.6) standard deviations for the (W/Z)W(→cq) process. The (W/Z)H(→cc¯) search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model cross-section times branching fraction for a Higgs boson with a mass of , corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier |κc|<8.5 (12.4), at the 95% confidence level. A combination with the ATLAS (W/Z)H,H→bb¯ analysis is performed, allowing the ratio κc/κb to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level
Anomaly detection search for new resonances decaying into a Higgs boson and a generic new particle X in hadronic final states using s=13 TeV pp collisions with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Achkar B
- 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
- Ahuja S
- Ai X
- Aielli G
- Aizenberg I
- 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
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Aly M
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amoroso S
- Amos KR
- Ananiev V
- Anastopoulos C
- Andana RYG
- 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
- Aoki T
- Aparo MA
- Appelt C
- Aranda CP
- Aranzabal N
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- Arcangeletti C
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- Arena E
- Argos FC
- Arguin J-F
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- Belotskiy K
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- Blue A
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- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
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- Budagov IA
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- Burgard CD
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- Burton CD
- Burzynski JC
- Busch EL
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- Butler JM
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- Butterworth JM
- Buttinger W
- Buzykaev AR
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- Cabras G
- Caforio D
- Cai H
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- Cairo VMM
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- Calafiura P
- Calderini G
- Calfayan P
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- Caloba LP
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- Camerlingo MT
- Cameron D
- Camincher C
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- Camplani A
- Canale V
- Canesse A
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- Cao Y
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- Capriles FGD
- Capua M
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- Cardenas JCJ
- Cardillo F
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- Carlino G
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- Carlson BT
- Carlson EM
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- Castiglia EG
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cavaliere V
- Cavalli N
- Cavasinni V
- Celebi E
- Celli F
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- Cerny K
- Cerqueira AS
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- Chen X
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- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
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- Chitan A
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- Chiu YH
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- Chowdhury T
- Christopher LD
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- Chwastowski JJ
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
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- Cormier F
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- Corpe LD
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- Czurylo MM
- Da Costa AMMJ
- da Costa JBG
- Da Cruz E Silva CB
- Da Fonseca Pinto JV
- Da Silva GG
- Da Via C
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- De Araujo MV
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- De Maria A
- De Moura NMJN
- de Renstrom PAB
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- De K
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- Deviveiros PO
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- Di Girolamo A
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- Dominguez LP
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- Drozdova M
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- Fleck I
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- Zhemchugov A
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- Zinsser J
- Ziolkowski M
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- 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
A search is presented for a heavy resonance
Y
decaying into a Standard Model Higgs boson
H
and a new particle
X
in a fully hadronic final state. The full Large Hadron Collider run 2 dataset of proton-proton collisions at..
Search for heavy long-lived multi-charged particles in the full LHC Run 2 pp collision data at s = 13 TeV using the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
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- Acharya BS
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- Zhemchugov A
- Zheng X
- Zheng Z
- Zhong D
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- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
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- Zormpa O
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/11/2023
- Field of study
A search for heavy long-lived multi-charged particles is performed using the ATLAS detector at the LHC. Data collected in 2015–2018 at √s = 13 TeV from pp collisions corresponding to an integrated luminosity of 139 fb−1 are examined. Particles producing anomalously high ionization, consistent with long-lived spin-½ massive particles with electric charges from |q| = 2e to |q| = 7e are searched for. No statistically significant evidence of such particles is observed, and 95% confidence level cross-section upper limits are calculated and interpreted as the lower mass limits for a Drell–Yan plus photon-fusion production mode. The least stringent limit, 1060 GeV, is obtained for |q| = 2e particles, and the most stringent one, 1600 GeV, is for |q| = 6e particles
Search for the Zγ decay mode of new high-mass resonances 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
- Acharya BS
- Adamczyk L
- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
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- Agheorghiesei C
- Agullo PM
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- Ahmadov F
- Ahmed WS
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- Ai X
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- Aizenberg I
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- Akimov AV
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- Akolkar NN
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- Aleksandrov IN
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- Burzynski JC
- Busch EL
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Büscher V
- Cadamuro L
- Caffaro AGG
- Caforio D
- Cai H
- Cai Y
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
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- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capocasa F
- Capriles FGD
- Capua M
- Carbone A
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- Cardenas JCJ
- Cardillo F
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- Carli T
- Carlino G
- Carlotto JI
- Carlson BT
- Carlson EM
- Carlson TI
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- Caspar M
- Castiglia EG
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cavaliere V
- Cavalli N
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- Celebi E
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- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
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- Chiodini G
- Chisholm AS
- Chitan A
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- Chizhov MV
- Choi ACO
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- Chwastowski JJ
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
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- Cooke HG
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- Cormier F
- Cornell SD
- Corpe LD
- Corradi M
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- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
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- D'Auria S
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- D'Onofrio A
- D'Onofrio M
- D'uffizi M
- Da Costa AMMJ
- da Costa JBG
- Da Fonseca Pinto JV
- Da Silva GG
- Da Via C
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- Dawson I
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- De Abreu Farias PCM
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- de Andrade Filho LM
- De Araujo MV
- De Asmundis R
- De Biase N
- De Carvalho ALM
- De Castro S
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- de Jong P
- de la Hoz SG
- De la Torre H
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- de Renstrom PAB
- De Sa RCL
- De Salvo A
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- De Sousa MJDCS
- De Souza EEP
- De K
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- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Gregorio G
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- Di Micco B
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- Dominguez LP
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- Drobac AS
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- Filipčič A
- Filmer EK
- Filthaut F
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- Fitzhugh PM
- Fleck I
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- Zhemchugov A
- Zheng J
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/12/2023
- Field of study
This letter presents a search for narrow, high-mass resonances in the Zγ final state with the Z boson decaying into a pair of electrons or muons. The
TeV pp collision data were recorded by the ATLAS detector at the CERN Large Hadron Collider and have an integrated luminosity of 140 fb−1. The data are found to be in agreement with the Standard Model background expectation. Upper limits are set on the resonance production cross section times the decay branching ratio into Zγ. For spin-0 resonances produced via gluon–gluon fusion, the observed limits at 95% confidence level vary between 65.5 fb and 0.6 fb, while for spin-2 resonances produced via gluon–gluon fusion (or quark–antiquark initial states) limits vary between 77.4 (76.1) fb and 0.6 (0.5) fb, for the mass range from 220 GeV to 3400 GeV
Luminosity determination in pp collisions at √s=13TeV using the ATLAS detector at the LHC
- Author
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- Zhemchugov A
- Zheng X
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Publication date
- 01/01/2023
- Field of study
Measurements of observables sensitive to colour reconnection in t(t)over-bar events with the ATLAS detector at √s=13TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Achkar B
- Adamczyk L
- Adamek L
- Addepalli SV
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- Aggarwal A
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- Agullo PM
- Ahmad A
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- Alberghi GL
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- Yeo BK
- Yexley MR
- Yildiz HD
- Yin P
- Yorita K
- Young C
- Young CJS
- Yuan M
- Yuan R
- Yue L
- Yue X
- Zaazoua M
- Zabinski B
- Zagazeta LFG
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zang J
- Zanzi D
- Zaplatilek O
- 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 P
- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang Y
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng X
- 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
- 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
- Publication date
- 01/01/2023
- Field of study
Performance of the reconstruction of large impact parameter tracks in the inner detector of ATLAS
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ahuja S
- Ai X
- Aielli G
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Algren M
- Alhroob M
- Ali B
- Ali HMJ
- Ali S
- Alibocus SW
- Aliev M
- Alimonti G
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allen JF
- Allport PP
- Aloisio A
- Alonso AG
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Aly M
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amos KR
- Ananiev V
- Anastopoulos C
- Andana RYG
- 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
- Aoki T
- Aparo MA
- Appelt C
- Apyan A
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Argos FC
- Arguin J
- Argyropoulos S
- Arling J
- Arnaez O
- Arneman DRV
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atashi S
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Auriol AD
- Austrup VA
- Avolio G
- Axiotis K
- Azuelos G
- 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
- Bakos E
- 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
- Barakat M
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barends KN
- Barillari T
- Barisits M
- Barklow T
- Baron P
- Baroncelli A
- Barone G
- Barr AJ
- Barr JD
- Barreiro F
- Barron U
- Barrue RFC
- Barsov S
- Bartels F
- Bartoldus R
- Barton AE
- Bartos P
- Basan A
- Baselga M
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Battulga D
- Bauce M
- Bauer M
- Bauer P
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HP
- Becker K
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bello FAD
- Bellos P
- Beloborodov K
- Belyaev NL
- Benchekroun D
- Bendebba F
- Benhammou Y
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berger N
- Bergmann B
- Beringer J
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Bernon F
- Berry T
- Berta P
- Berthold A
- Bertram IA
- Bethke S
- Betti A
- Bevan AJ
- Bhamjee M
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Bianco G
- Biebel O
- Bielski R
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
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- Birch-sykes CJ
- Bird GA
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- Bold T
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- Booth CD
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- Borecka-Bielska HM
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- Borissov G
- Bortoletto D
- Bosca SR
- Boscherini D
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- Burr JTP
- Burton CD
- Burzynski JC
- Busch EL
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Büscher V
- Cabras G
- Cadamuro L
- Caffaro AGG
- Caforio D
- Cai H
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- Cairo VMM
- Cakir IT
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- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
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- Camerlingo MT
- Cameron D
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- Canale V
- Canesse A
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- Cao Y
- Capocasa F
- Capriles FGD
- Capua M
- Carbone A
- Cardarelli R
- Cardenas JCJ
- Cardillo F
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- Carlino G
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- Carlson BT
- Carlson EM
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- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cavaliere V
- Cavalli N
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- Celebi E
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- Cerqueira AS
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- Cheremushkina E
- Cherepanova E
- Cheu E
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- Chevalier L
- Chiarella V
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- Chitan A
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- Chizhov MV
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- Chou Y
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- Ciaccio AD
- Ciaccio LD
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
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- Cormier F
- Cornell SD
- Corpe LD
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- Correia AMH
- Corriveau F
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- Cortes-Gonzalez A
- Costa MJ
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- Crescioli F
- Cristinziani M
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- Cueto A
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- Curcio F
- Czodrowski P
- Czurylo MM
- Da Costa AMMJ
- da Costa JBG
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Silva GG
- Da Via C
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- Dabrowski W
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- Dawson I
- Day-hall HA
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- de Andrade Filho LM
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- De Asmundis R
- De Biase N
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- De Castro S
- De Groot N
- de Jong P
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- De Maria A
- De Moura Junior NMJN
- de Renstrom PAB
- De Sa RCL
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- De Vivie De Regie JB
- Dedovich DV
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- Doglioni C
- Dolejsi J
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- Dominguez LP
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- Donato CD
- Donell DMM
- Dong B
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- Filmer EK
- Filthaut F
- Fiolhais MCN
- Fiorini L
- 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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- Forland BC
- Formica A
- Forti AC
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- Gavrilenko IL
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- Genest MH
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- Geyik ME
- Ghazali YE
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- Gingrich DM
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- Hawkings RJ
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- Iconomidou-Fayard L
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- Karentzos E
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- Konya B
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- 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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- Kraus JW
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- Kurdysh O
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- Leopold A
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- Liberatore M
- Liberti B
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- Lipniacka A
- Lister A
- Little JD
- Liu B
- Liu BX
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- Wilkens HG
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- Zagazeta LFG
- Zaid E
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- Zakharchuk N
- Zambito S
- Zang J
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- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger Jr DT
- Zenin O
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- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
- Zhang DF
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- Zhang Y
- Zhang Z
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- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
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- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Publication date
- 01/01/2023
- Field of study
Search for doubly charged Higgs boson production in multi-lepton final states using 139 fb-1 of proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Achkar B
- 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
- Ahnen JV
- Ahuja S
- Ai X
- Aielli G
- Aizenberg I
- 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
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- Alves FLL
- Alviggi MG
- Ambler A
- Amelung C
- Ames CG
- Amidei D
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- Amos KR
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- Ananiev V
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- 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
- Argos FC
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- Argyropoulos S
- Arling J
- Armbruster AJ
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- Asada H
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- Assahsah J
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- Burton CD
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- Cavaliere V
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- Chapman JD
- Chargeishvili B
- Charlton DG
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- Chekulaev SV
- Chelkov GA
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- Cheplakov A
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- Cherepanova E
- Cheu E
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- Chevalier L
- Chiarella V
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- Chiodini G
- Chisholm AS
- Chitan A
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- Costa MJ
- Costanza F
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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 Silva GG
- Da Via C
- Daalen TRV
- Dabrowski W
- Dado T
- Dahbi S
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- de Andrade Filho LM
- De Araujo MV
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- De Maria A
- de Renstrom PAB
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- De Souza EEP
- De Vivie De Regie JB
- Dedovich DV
- Degens J
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- Dell’Asta L
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- Delsart PA
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- Demichev M
- Denisov SP
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- Donaldson CP
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
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- 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
- Publication date
- 01/01/2023
- Field of study
Search for exclusive Higgs and Z boson decays to ωγ and Higgs boson decays to K ⁎ γ with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- 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
- Ahuja S
- Ai X
- Aielli G
- Aitbenchikh B
- Aizenberg I
- 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
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Aly M
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amos KR
- Ananiev V
- Anastopoulos C
- Andana RYG
- 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
- Aoki T
- Aparo MA
- Appelt C
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Argos FC
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Arnaez O
- Arnold H
- Artoni G
- Asada H
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- Asai S
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- Assamagan K
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- Astigarraga MEP
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- Avolio G
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- Azuelos G
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- Bachacou H
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- Backman F
- Badea A
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- Bailey VR
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- Baker OK
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- Baldin EM
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- Brock I
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- Buckley AG
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- Bugge MK
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- Bullard BA
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- Burgard CD
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- Burton CD
- Burzynski JC
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- Butterworth JM
- Buttinger W
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- Camincher C
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- Canale V
- Canesse A
- Cantero J
- Cao Y
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- Capriles FGD
- Capua M
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- Cardenas JCJ
- Cardillo F
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- Carlotto JI
- Carlson BT
- Carlson EM
- Carlson TI
- Carminati L
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- Cheng HC
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- Cheremushkina E
- Cherepanova E
- Cheu E
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- Chiarella V
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- Chiedde N
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- Christopher LD
- Chu KL
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- Chwastowski JJ
- Cieri D
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- da Costa JBG
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- de Andrade Filho LM
- De Araujo MV
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- Yin P
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- Younas S
- Young C
- Young CJS
- Yu Y
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- Yue L
- Zaazoua M
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- Zagazeta LFG
- Zaid E
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- Zakharchuk N
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- Zang J
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- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
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- Zerwas D
- Zhai M
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- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
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- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/12/2023
- Field of study
Searches for the exclusive decays of the Higgs boson to an ω meson and a photon or a K⁎ meson and a photon can probe flavour-conserving and flavour-violating Higgs boson couplings to light quarks, respectively. Searches for these decays, along with the analogous Z boson decay to an ω meson and a photon, are performed with a pp collision data sample corresponding to integrated luminosities of up to 134 fb−1 collected at √s=13 TeV with the ATLAS detector at the CERN Large Hadron Collider. The obtained 95% confidence-level upper limits on the respective branching fractions are B(H→ωγ)<5.5×10−4, B(H→K⁎γ)<2.2×10−4 and B(Z→ωγ)<3.9×10−6. The limits for H→ωγ and Z→ωγ are 370 times and 140 times the Standard Model expected values, respectively. The result for Z→ωγ corresponds to a two-orders-of-magnitude improvement over the limit obtained by the DELPHI experiment at LEP