344 research outputs found
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Going "Rogue": Discourses of American Identity and Resistance on Twitter
- Author
- A Hahn
- A Light
- A Rennie
- A Runte
- A Scherman
- C Finney
- C Shirky
- D Brinkley
- DA Carbaugh
- DB Tindall
- HD Thoreau
- I Altman
- I Tyrrell
- J Ausserhofer
- JA Obar
- JR Vickery
- K DeLuca
- K Tracy
- KL Muñoz
- KM DeLuca
- KM DeLuca
- L Graves
- L Ross-Bryant
- M Foucault
- M Frome
- MJ Stoddart
- N Fairclough
- N Fairclough
- PC Pezzullo
- R Nash
- S Milan
- S Milan
- S Milan
- S Schwartz
- T Tudoroiu
- W Chen
- W Zelinsky
- Publication venue
- Palgrave Macmillan
- Publication date
- 01/01/2020
- Field of study
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at â=13TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akilli E
- Akimov AV
- Al Khoury K
- 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
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- Anastopoulos C
- 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
- 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
- Bakos E
- Balaji S
- Balasubramanian R
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barron U
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer P
- Bawa HS
- Bayirli A
- Beacham JB
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- Beauchemin PH
- Becherer F
- Bechtle P
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- Beddall AJ
- Bednyakov VA
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Belfkir M
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bello FAD
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
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- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Berthold A
- Bertram IA
- Bethke S
- Betti A
- Bevan AJ
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
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- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz NV
- Biglietti M
- Billoud TRV
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- Bingul A
- Bini C
- Biondi S
- Birch-sykes CJ
- Birman M
- Bisanz T
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- Blazek T
- Bloch I
- Blocker C
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- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Boeriu OEV
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bolanos GR
- Bold T
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borbély AG
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortoletto D
- Bosca SR
- Boscherini D
- Bosman M
- Bostanabad MG
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- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
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- Brandt G
- Brandt O
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- Brau JE
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- Brener R
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
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- Brooijmans G
- Brooks WK
- Brost E
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Bryngemark L
- BrĂŒers B
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buddenbrock SEV
- Bugge MK
- Bulekov O
- Bullard BA
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
- BĂŒscher V
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- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
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- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
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- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
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- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capriles FGD
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli T
- Carlino G
- Carlson BT
- Carlson EM
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carratta G
- CarrĂĄ S
- Carter JWS
- Carter TM
- Casado MP
- Casha AF
- Castiglia EG
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavasinni V
- Celebi E
- Celli F
- Cerny K
- Cerqueira AS
- Cerri A
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- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
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- Chapman JD
- Chargeishvili B
- Charlton DG
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- Chatterjee M
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- Chekulaev SV
- Chelkov GA
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen H
- Chen J
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalier L
- Chevalérias TJA
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
- Chow YS
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Ciaccio AD
- Ciaccio LD
- Cieri D
- Ciesla KM
- Cindro V
- CioarÄ IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
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- Clawson SE
- Clement C
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- Coadou Y
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- Coccaro A
- Cochran J
- Codina EP
- Cohen H
- Coimbra AEC
- Cole B
- Collot J
- Connell SH
- Connelly IA
- Conventi F
- Cooper-Sarkar AM
- Cormier F
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Coutinho YA
- Cowan G
- Cowley JW
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- Creager RA
- Crescioli F
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- Croft V
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- Cueto A
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- Cukierman AR
- Cunningham WR
- Czekierda S
- Czodrowski P
- Czurylo MM
- Da Costa AMMJ
- da Costa JBG
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Daalen TRV
- Dabrowski W
- Dachs F
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- Dahbi S
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- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Danninger M
- Dao V
- Darbo G
- Dartsi O
- Dattagupta A
- David C
- Davidek T
- Davis DR
- Dawson I
- de Andrade Filho LM
- De Asmundis R
- De Beurs M
- De Carvalho ALM
- De Castro S
- De Groot N
- de Jong P
- de la Hoz SG
- De la Torre H
- De Lima RT
- De Maria A
- De Pedis D
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santis M
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- De Vivie De Regie JB
- De K
- Dedovich DV
- Deiana AM
- Delgove D
- Deliot F
- Delitzsch CM
- DellâAcqua A
- DellâAsta L
- Delmastro M
- Delporte C
- Delsart PA
- Demers S
- Demichev M
- Demontigny G
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
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- Dette K
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- Deviveiros PO
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- Dias FA
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- Dickinson J
- Didenko M
- Diehl EB
- Dietrich J
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- Dominguez LP
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- Drechsler E
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- Dyckes GI
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- Facini G
- Fakhrutdinov RM
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- Falke PJ
- Falke S
- Faltova J
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- Fell A
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- Feng M
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- Fenyuk AB
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- Fleck I
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- Frost JA
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- Fusayasu T
- Fuster J
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- Gazis EN
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- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ 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 fbâ1 of sâ=13TeV protonâproton 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+0.38â0.36 , 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
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
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- Abbott B
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- Zhemchugov A
- Zheng J
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- Zhong D
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- Zhulanov V
- Zimine NI
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- Zoccoli A
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- Zorbas TG
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- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ 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 fbâ1 of proton-proton collision data recorded at a centre-of-mass energy of âs = 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
Measurement of the ttÂŻttÂŻ production cross section in pp collisions at âs=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- 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
- Akatsuka S
- Akbiyik M
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
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- Alfonsi F
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- Ali B
- Ali S
- Aliev M
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- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
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- Alunno Camelia E
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- Alviggi MG
- Amaral Coutinho Y
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- Anders JK
- Andrean SY
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- Angelidakis S
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- Zieminska D
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- Zoccoli A
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- Zorbas TG
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- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fbâ1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17â15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7â6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
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 âs = 13 TeV
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- Zhemchugov A
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into âÎœb are presented using 139 fbâ1 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 Ï = 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 ttÂŻ 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.]
Search for dark matter in events with missing transverse momentum and a Higgs boson decaying into two photons in pp collisions at root s=13 TeV with the ATLAS detector
- Author
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- Abbott B
- Abbott DC
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- Abhayasinghe DK
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- Zanzi D
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- Zemaityte G
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine N
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- Zinonos Z
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- Zorbas TG
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- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2021
- Field of study
A search for dark-matter particles in events with large missing transverse momentum and a Higgs boson candidate decaying into two photons is reported. The search uses 139 fbâ1 of proton-proton collision data collected at sâ = 13 TeV with the ATLAS detector at the CERN LHC between 2015 and 2018. No significant excess of events over the Standard Model predictions is observed. The results are interpreted by extracting limits on three simplified models that include either vector or pseudoscalar mediators and predict a final state with a pair of dark-matter candidates and a Higgs boson decaying into two photons
Two-particle azimuthal correlations in photonuclear ultraperipheral Pb plus Pb collisions at 5.02 TeV with ATLAS
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Abramowicz H
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- Abusleme Hoffman AC
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- Zakharchuk N
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- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
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- Zhang Z
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zorbas TG
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- Zou W
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/07/2021
- Field of study
Two-particle long-range azimuthal correlations are measured in photonuclear collisions using
1.7
nb
â
1
of 5.02 TeV
Pb
+
Pb
collision data collected by the ATLAS experiment at the CERN Large Hadron Collider. Candidate events are selected using a dedicated high-multiplicity photonuclear event trigger, a combination of information from the zero-degree calorimeters and forward calorimeters, and from pseudorapidity gaps constructed using calorimeter energy clusters and charged-particle tracks. Distributions of event properties are compared between data and Monte Carlo simulations of photonuclear processes. Two-particle correlation functions are formed using charged-particle tracks in the selected events, and a template-fitting method is employed to subtract the nonflow contribution to the correlation. Significant nonzero values of the second- and third-order flow coefficients are observed and presented as a function of charged-particle multiplicity and transverse momentum. The results are compared with flow coefficients obtained in proton-proton and proton-lead collisions in similar multiplicity ranges, and with theoretical expectations. The unique initial conditions present in this measurement provide a new way to probe the origin of the collective signatures previously observed only in hadronic collision
The ATLAS inner detector trigger performance in pp collisions at 13 TeV during LHC Run 2
- Author
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
The design and performance of the inner detector trigger for the high level trigger of the ATLAS experiment at the Large Hadron Collider during the 2016-2018 data taking period is discussed. In 2016, 2017, and 2018 the ATLAS detector recorded 35.6 fb(-1), 46.9 fb(-1), and 60.6 fb(-1) respectively of proton-proton collision data at a centre-of-mass energy of 13TeV. In order to deal with the very high interaction multiplicities per bunch crossing expected with the 13TeV collisions the inner detector trigger was redesigned during the long shutdown of the Large Hadron Collider from 2013 until 2015. An overview of these developments is provided and the performance of the tracking in the trigger for the muon, electron, tau and b-jet signatures is discussed. The high performance of the inner detector trigger with these extreme interaction multiplicities demonstrates how the inner detector tracking continues to lie at the heart of the trigger performance and is essential in enabling the ATLAS physics programme
Measurements of W+Wâ+ â„ 1 jet production cross-sections in pp collisions at sâ = 13 TeV with the ATLAS detector
- Author
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- Zemaityte G
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- Zhang X
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- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Fiducial and differential cross-section measurements of W+Wâ production in
association with at least one hadronic jet are presented. These measurements are sensitive
to the properties of electroweak-boson self-interactions and provide a test of perturbative
quantum chromodynamics and the electroweak theory. The analysis is performed using
proton-proton collision data collected at p
s = 13TeV with the ATLAS experiment, corresponding
to an integrated luminosity of 139 fbâ1. Events are selected with exactly one oppositely
charged electron-muon pair and at least one hadronic jet with a transverse momentum
of pT > 30 GeV and a pseudorapidity of |ïżœ| < 4.5. After subtracting the background
contributions and correcting for detector effects, the jet-inclusive W+Wâ+ ïżœ 1 jet fiducial
cross-section and W+Wâ+ jets differential cross-sections with respect to several kinematic
variables are measured. These measurements include leptonic quantities, such as the lepton
transverse momenta and the transverse mass of the W+Wâ system, as well as jet-related
observables such as the leading jet transverse momentum and the jet multiplicity. Limits on
anomalous triple-gauge-boson couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous amplitude is enhanced
Combination of searches for heavy spin-1 resonances using 139 fbâ1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
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- Aakvaag E
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
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- Abramowicz H
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- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ 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 fbâ1 of proton-proton collisions at
= 13 TeV collected during 2015â2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (ÏÎœ and ÏÏ) 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
- âŠ