267 research outputs found
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
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- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
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- Zhemchugov A
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- Zhulanov V
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Search for pair production of squarks or gluinos decaying via sleptons or weak bosons in final states with two same-sign or three leptons with the ATLAS detector
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- Yue L
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- Zakharchuk N
- Zambito S
- Zamora Saa JA
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
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- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
- 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
- 'Springer Science and Business Media LLC'
- Publication date
- 15/02/2024
- Field of study
A search for pair production of squarks or gluinos decaying via sleptons or weak bosons is reported. The search targets a final state with exactly two leptons with same-sign electric charge or at least three leptons without any charge requirement. The analysed data set corresponds to an integrated luminosity of 139 fb−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Multiple signal regions are defined, targeting several SUSY simplified models yielding the desired final states. A single control region is used to constrain the normalisation of the WZ + jets background. No significant excess of events over the Standard Model expectation is observed. The results are interpreted in the context of several supersymmetric models featuring R-parity conservation or R-parity violation, yielding exclusion limits surpassing those from previous searches. In models considering gluino (squark) pair production, gluino (squark) masses up to 2.2 (1.7) TeV are excluded at 95% confidence level
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Aakvaag E
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboelela M
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Ackermann A
- Adam Bourdarios C
- Adamczyk L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Aktas S
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Alegria ZL
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- 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
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amirie KJ
- Amor Dos Santos SP
- Amos KR
- An S
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
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- Zhemchugov A
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- Zimine NI
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Software Performance of the ATLAS Track Reconstruction for LHC Run 3
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- Zhao Y
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- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
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- Zhou Y
- Zhu CG
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- Zhu Y
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- 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
- 'Springer Science and Business Media LLC'
- Publication date
- 02/04/2024
- Field of study
Charged particle reconstruction in the presence
of many simultaneous proton–proton (pp) collisions in the
LHC is a challenging task for the ATLAS experiment’s reconstruction software due to the combinatorial complexity. This
paper describes the major changes made to adapt the software
to reconstruct high-activity collisions with an average of 50 or
more simultaneous pp interactions per bunch crossing (pileup) promptly using the available computing resources. The
performance of the key components of the track reconstruction chain and its dependence on pile-up are evaluated, and
the improvement achieved compared to the previous software
version is quantified. For events with an average of 60 pp collisions per bunch crossing, the updated track reconstruction
is twice as fast as the previous version, without significant
reduction in reconstruction efficiency and while reducing the
rate of combinatorial fake tracks by more than a factor two
Corrigendum to "Search for flavour-changing neutral-current couplings between the top quark and the photon with the ATLAS detector at √s=13 TeV" (Physics Letters B, 842 (2023), 137379)
- Author
- Aad G
- Abbott B
- Abbott Dc
- Abed Abud A
- Abeling K
- Abidi Sh
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman Ac
- Acharya Bs
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Addepalli Sv
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder Aa
- Afik Y
- Agaras Mn
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra Ja
- Ahmad A
- Ahmadov F
- Ahmed Ws
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akimov Av
- Al Khoury K
- Alberghi Gl
- Albert J
- Albicocco P
- Alconada Verzini Mj
- Alderweireldt S
- Aleksa M
- Aleksandrov In
- Alexa C
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- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
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- Alimonti G
- Allaire C
- Allbrooke Bmm
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- Aloisio A
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- Amelung C
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- Behera A
- Behr Jk
- Beirao Da Cruz E Silva C
- Beirer Jf
- Beisiegel F
- Belfkir M
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev Nl
- Benchekroun D
- Benhammou Y
- Benjamin Dp
- Benoit M
- Bensinger Jr
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Bergmann B
- Beringer J
- Berlendis S
- Bernardi G
- Bernius C
- Bernlochner Fu
- Berry T
- Berta P
- Berthold A
- Bertram Ia
- Bessidskaia Bylund O
- Bethke S
- Betti A
- Bevan Aj
- Bhatta S
- Bhattacharya Ds
- Bhattarai P
- Bhopatkar Vs
- Bi R
- Bi R
- Bianchi Rm
- Biebel O
- Bielski R
- Biesuz Nv
- Biglietti M
- Billoud Trv
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Biondini A
- Birch-sykes Cj
- Bird Ga
- Birman M
- Bisanz T
- Biswas D
- Bitadze A
- Bjørke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink Gj
- Bobrovnikov Vs
- Boehler M
- Bogavac D
- Bogdanchikov Ag
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth Cd
- Borbély Ag
- Borecka-Bielska Hm
- Borgna Ls
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola Jd
- Bouaouda K
- Boudreau J
- Bouhova-Thacker Ev
- Boumediene D
- Bouquet R
- Boveia A
- Boyd J
- Boye D
- Boyko Ir
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau Je
- Breaden Madden Wd
- Brendlinger K
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Brickwedde B
- Britton D
- Britzger D
- Brock I
- Brooijmans G
- Brooks Wk
- Brost E
- Bruckman de Renstrom Pa
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Brüers B
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley Ag
- Budagov Ia
- Bugge Mk
- Bulekov O
- Bullard Ba
- Burdin S
- Burgard Cd
- Burger Am
- Burghgrave B
- Burr Jtp
- Burton Cd
- Burzynski Jc
- Busch El
- Bussey Pj
- Butler Jm
- Buttar Cm
- Butterworth Jm
- Buttinger W
- Buxo Vazquez Cj
- Buzykaev Ar
- Büscher V
- Cabras G
- Cabrera Urbán S
- Caforio D
- Cai H
- Cai Y
- Cairo Vmm
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba Lp
- Calvet D
- Calvet S
- Calvet Tp
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Camerlingo Mt
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cano Bret M
- Cantero J
- Cao Y
- Capocasa F
- Capua M
- Carbone A
- Cardarelli R
- Cardenas Jcj
- Cardillo F
- Carli T
- Carlino G
- Carlson Bt
- Carlson Em
- Carminati L
- Carnesale M
- Caron S
- Carquin E
- Carratta G
- Carrá S
- Carter Jws
- Carter Tm
- Casado Mp
- Casha Af
- Castiglia Eg
- Castillo Garcia L
- Castillo Gimenez V
- Castillo Fl
- Castro Nf
- Catinaccio A
- Catmore Jr
- Cavaliere V
- Cavalli N
- Cavasinni V
- Celebi E
- Celli F
- Centonze Ms
- Cerny K
- Cerqueira As
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin Sa
- Chadi Z
- Chakraborty D
- Chala M
- Chan J
- Chan Ws
- Chan Wy
- Chapman Jd
- Chargeishvili B
- Charlton Dg
- Charman Tp
- Chatterjee M
- Chekanov S
- Chekulaev Sv
- Chelkov Ga
- Chen A
- Chen B
- Chen B
- Chen C
- Chen H
- Chen H
- Chen J
- Chen J
- Chen S
- Chen Sj
- Chen X
- Chen X
- Chen Y
- Cheng Cl
- Cheng Hc
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm As
- Chitan A
- Chiu Yh
- Chizhov Mv
- Choi K
- Chomont Ar
- Chou Y
- Chow Eys
- Chowdhury T
- Christopher Ld
- Chu Kl
- Chu Mc
- Chu X
- Chudoba J
- Chwastowski Jj
- Cieri D
- Ciesla Km
- Cindro V
- Ciocio A
- Cirotto F
- Citron Zh
- Citterio M
- Ciubotaru Da
- Ciungu Bm
- Clark A
- Clark Pj
- Clavijo Columbie Jm
- Clawson Se
- Clement C
- Clercx J
- Clissa L
- Coadou Y
- Cobal M
- Coccaro A
- Coelho Barrue Rf
- Coelho Lopes De Sa R
- Coelli S
- Cohen H
- Coimbra Aec
- Cole B
- Collot J
- Conde Muiño P
- Connell Sh
- Connelly Ia
- Conroy Ei
- Conventi F
- Cooke Hg
- Cooper-Sarkar Am
- Cormier F
- Corpe Ld
- Corradi M
- Corrigan Ee
- Corriveau F
- Cortes-Gonzalez A
- Costa Mj
- Costanza F
- Costanzo D
- Cote Bm
- Cowan G
- Cowley Jw
- Cranmer K
- Crescioli F
- Crépé-Renaudin S
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosetti G
- Cueto A
- Cuhadar Donszelmann T
- Cui H
- Cui Z
- Cukierman Ar
- Cunningham Wr
- Curcio F
- Czodrowski P
- Czurylo Mm
- D'Amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- D'Onofrio A
- D'Onofrio M
- D'Uffizi M
- Da Cunha Sargedas De Sousa Mj
- Da Fonseca Pinto Jv
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damp J
- Dandoy Jr
- Daneri Mf
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Das Sj
- Dattagupta A
- David C
- Davidek T
- Davis Dr
- Davis-Purcell B
- Dawson I
- De Asmundis R
- De Beurs M
- De Castro S
- De Groot N
- de Jong P
- De la Torre H
- De Maria A
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Vivie De Regie Jb
- De K
- Dedovich Dv
- Degens J
- Deiana Am
- Del Corso F
- Del Peso J
- Del Rio F
- Deliot F
- Delitzsch Cm
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delsart Pa
- Demers S
- Demichev M
- Denisov Sp
- Derendarz D
- Derue F
- Dervan P
- Desch K
- Dette K
- Deutsch C
- Deviveiros Po
- Di Bello Fa
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
- Di Nardo R
- Diaconu C
- Dias Do Vale T
- Dias Fa
- Diaz Capriles Fg
- Diaz Ma
- Didenko M
- Diehl Eb
- Diehl L
- Diez Pardos C
- Dimitriadi C
- Dimitrievska A
- Ding W
- Dingfelder J
- Dinu I
- Dittmeier Sj
- Dittus F
- Díez Cornell S
- Djama F
- Djobava T
- Djuvsland Ji
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Donadelli M
- Dong B
- Donini J
- Dopke J
- Doria A
- Dova Mt
- Doyle At
- Draguet Ma
- Drechsler E
- Dreyer E
- Drivas-koulouris I
- Drobac As
- du Pree Ta
- Du D
- Dubinin F
- Dubovsky M
- Duchovni E
- Duckeck G
- Ducu Oa
- Duda D
- Dudarev A
- Duflot L
- Dumitriu Ae
- Dunford M
- Dungs S
- Dunne K
- Duperrin A
- Duran Yildiz H
- Durglishvili A
- Dührssen M
- Dülsen C
- Düren M
- Dwyer Bl
- Dyckes Gi
- Dyndal M
- Dysch S
- Dziedzic Bs
- Eckerova B
- Eggleston Mg
- Egidio Purcino De Souza E
- Ehrke Lf
- Eigen G
- Einsweiler K
- Ekelof T
- Ekman Pa
- El Ghazali Y
- El Jarrari H
- El Moussaouy A
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot Aa
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Emerman A
- Enari Y
- Ene I
- Epari S
- Erdmann J
- Ereditato A
- Erland Pa
- Errenst M
- Escalier M
- Escobar C
- Etzion E
- Evans G
- Evans H
- Evans Mo
- Ezhilov A
- Ezzarqtouni S
- Fabbri F
- Fabbri L
- Facini G
- Fadeyev V
- Fakhrutdinov Rm
- Falciano S
- Falke Pj
- Falke S
- Faltova J
- Fan Y
- Fang Y
- Fanourakis G
- Fanti M
- Faraj M
- Farbin A
- Farilla A
- Farooque T
- Farrington Sm
- Fassi F
- Fassouliotis D
- Faucci Giannelli M
- Fawcett Wj
- Fayard L
- Fedin Ol
- Fedotov G
- Feickert M
- Feligioni L
- Fell A
- Fellers De
- Feng C
- Feng M
- Fenton Mj
- Fenyuk Ab
- Ferencz L
- Ferguson Sw
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrere D
- Ferretti C
- Fiedler F
- Filipčič A
- Filmer Ek
- Filthaut F
- Fiolhais Mcn
- Fiorini L
- Fischer F
- Fisher Wc
- Fitschen T
- Fleck I
- Fleischmann P
- Flick T
- Flores Castillo Lr
- Flores L
- Flores M
- Follega Fm
- Fomin N
- Foo Jh
- Forland Bc
- Formica A
- Forti Ac
- Fortin E
- Fortman Aw
- Foti Mg
- Fountas L
- Fournier D
- Fox H
- Francavilla P
- Francescato S
- Franchini M
- Franchino S
- Francis D
- Franco L
- Franconi L
- Franklin M
- Frattari G
- Freegard Ac
- Freeman Pm
- Freund Ws
- Fritzsche N
- Froch A
- Froidevaux D
- Frost Ja
- Fu Y
- Fujimoto M
- Fullana Torregrosa E
- Fuster J
- Gabrielli A
- Gabrielli A
- Gadow P
- Gagliardi G
- Gagnon Lg
- Gallardo Ge
- Gallas Ej
- Gallop Bj
- Gamboa Goni R
- Gan Kk
- Ganguly S
- Gao J
- Gao Y
- Garay Walls Fm
- Garcia B
- Garcia-Sciveres M
- García Navarro Je
- García Pascual Ja
- García C
- Gardner Rw
- Garg D
- Garg Rb
- Gargiulo S
- Garner Ca
- Garonne V
- Gasiorowski Sj
- Gaspar P
- Gaudio G
- Gauzzi P
- Gavrilenko Il
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis En
- Geanta Aa
- Gee Cm
- Geisen J
- Geisen M
- Gemme C
- Genest Mh
- Gentile S
- George S
- George Wf
- Geralis T
- Gerlach Lo
- Gessinger-Befurt P
- Ghasemi Bostanabad M
- Ghneimat M
- Ghosal A
- Ghosh A
- Ghosh A
- Giacobbe B
- Giagu S
- Giangiacomi N
- Giannetti P
- Giannini A
- Gibson Sm
- Gignac M
- Gil Dt
- Gilbert Ak
- Gilbert Bj
- Gillberg D
- Gilles G
- Gillwald Nek
- Ginabat L
- Gingrich Dm
- Giordani Mp
- Giraud Pf
- Giugliarelli G
- Giugni D
- Giuli F
- Gkialas I
- Gladilin Lk
- Glasman C
- Gledhill Gr
- Glisic M
- Gnesi I
- Go Y
- Goblirsch-Kolb M
- Gocke B
- Godin D
- Goldfarb S
- Golling T
- Gololo Mgd
- Golubkov D
- Gombas Jp
- Gomes A
- Gomez Delegido Aj
- Goncalves Gama R
- Gonçalo R
- Gonella G
- Gonella L
- Gongadze A
- Gonnella F
- Gonski Jl
- Gonzalez Fernandez S
- Gonzalez Lopez R
- Gonzalez Renteria C
- Gonzalez Suarez R
- Gonzalez-Sevilla S
- Gonzalvo Rodriguez Gr
- González Andana Ry
- González de la Hoz S
- Goossens L
- Gorasia Na
- Gorbounov Pa
- Gorini B
- Gorini E
- Gorišek A
- Goshaw At
- Gostkin Mi
- Gottardo Ca
- Gouighri M
- Goumarre V
- Goussiou Ag
- Govender N
- Goy C
- Grabowska-Bold I
- Graham K
- Gramstad E
- Grancagnolo S
- Grandi M
- Gratchev V
- Gravila Pm
- Gravili Fg
- Gray Hm
- Greco M
- Grefe C
- Gregor Im
- Grenier P
- Grieco C
- Grillo Aa
- Grimm K
- Grinstein S
- Grivaz J-
- Gross E
- Grosse-Knetter J
- Grud C
- Grummer A
- Grundy Jc
- Guan L
- Guan W
- Gubbels C
- Guerrero Rojas Jgr
- Guerrieri G
- Guescini F
- Gugel R
- Guhit Jam
- Guida A
- Guillemin T
- Guilloton E
- Guindon S
- Guo F
- Guo J
- Guo L
- Guo Y
- Gupta R
- Gurbuz S
- Gustavino G
- Guth M
- Gutierrez Zagazeta Lf
- Gutierrez P
- Gutschow C
- Guyot C
- Gwenlan C
- Gwilliam Cb
- Haaland Es
- Haas A
- Habedank M
- Haber C
- Hadavand Hk
- Hadef A
- Hadzic S
- Haleem M
- Haley J
- Hall Jj
- Hallewell Gd
- Halser L
- Hamano K
- Hamdaoui H
- Hamer M
- Hamity Gn
- Han J
- Han K
- Han L
- Han L
- Han S
- Han Yf
- Hanagaki K
- Hance M
- Hangal Da
- Hank Md
- Hankache R
- Hansen Jb
- Hansen Jd
- Hansen Ph
- Hara K
- Harada D
- Harenberg T
- Harkusha S
- Harris Yt
- Harrison Pf
- Hartman Nm
- Hartmann Nm
- Hasegawa Y
- Hasib A
- Haug S
- Hauser R
- Havranek M
- Hawkes Cm
- Hawkings Rj
- Hayashida S
- Hayden D
- Hayes C
- Hayes Rl
- Hays Cp
- Hays Jm
- Hayward Hs
- He F
- He Y
- He Y
- Heath Mp
- Hedberg V
- Heggelund Al
- Hehir Nd
- Heidegger C
- Heidegger Kk
- Heidorn Wd
- Heilman J
- Heim S
- Heim T
- Heinemann B
- Heinlein Jg
- Heinrich Jj
- Heinrich L
- Hejbal J
- Helary L
- Held A
- Hellesund S
- Helling Cm
- Hellman S
- Helsens C
- Henderson Rcw
- Henkelmann L
- Henriques Correia Am
- Herde H
- Hernández Jiménez Y
- Herr H
- Herrmann Mg
- Herrmann T
- Herten G
- Hertenberger R
- Hervas L
- Hessey Np
- Hibi H
- Higón-Rodriguez E
- Hillier Sj
- Hinchliffe I
- Hinterkeuser F
- Hirose M
- Hirose S
- Hirschbuehl D
- Hiti B
- Hobbs J
- Hobincu R
- Hod N
- Hodgkinson Mc
- Hodkinson Bh
- Hoecker A
- Hofer J
- Hohn D
- Holm T
- Holzbock M
- Hommels Lbah
- Honan Bp
- Hong J
- Hong Tm
- Hong Y
- Honig Jc
- Hooberman Bh
- Hopkins Wh
- Horii Y
- Hou S
- Howarth J
- Hoya J
- Hönle A
- Hrabovsky M
- Hryn'Ova T
- Hrynevich A
- Hsu Pj
- Hsu S-
- Hu Q
- Hu Yf
- Huang Dp
- Huang S
- Huang X
- Huang Y
- Huang Y
- Huang Z
- Hubacek Z
- Huebner M
- Huegging F
- Huffman Tb
- Huhtinen M
- Huiberts Sk
- Hulsken R
- Huseynov N
- Huston J
- Huth J
- Hyneman R
- Hyrych S
- Iacobucci G
- Iakovidis G
- Ibragimov I
- Iconomidou-Fayard L
- Iengo P
- Iguchi R
- Iizawa T
- Ikegami Y
- Ilg A
- Ilic N
- Imam H
- Ingebretsen Carlson T
- Introzzi G
- Iodice M
- Ippolito V
- Ishino M
- Islam W
- Issever C
- Istin S
- Ito H
- Iturbe Ponce Jm
- Iuppa R
- Ivina A
- Izen Jm
- Izzo V
- Jacka P
- Jackson P
- Jacobs Rm
- Jaeger Bp
- Jagfeld Cs
- Jakobs K
- Jakoubek T
- Jamieson J
- Janas Kw
- Jarlskog G
- Jaspan Ae
- Javurkova M
- Javůrek T
- Jäkel G
- Jeanneau F
- Jeanty L
- Jejelava J
- Jenni P
- Jessiman Ce
- Jézéquel S
- Jia J
- Jia X
- Jia X
- Jia Z
- Jiang Y
- Jiggins S
- Jimenez Pena J
- Jin S
- Jinaru A
- Jinnouchi O
- Jivan H
- Johansson P
- Johns Ka
- Johnson Ca
- Jones Dm
- Jones E
- Jones Rwl
- Jones Tj
- Jovicevic J
- Ju X
- Junggeburth Jj
- Juste Rozas A
- Kabana S
- Kaczmarska A
- Kado M
- Kagan H
- Kagan M
- Kahn A
- Kahn A
- Kahra C
- Kaji T
- Kajomovitz E
- Kakati N
- Kalderon Cw
- Kamenshchikov A
- Kang Nj
- Kano Y
- Kar D
- Karava K
- Kareem Mj
- Karentzos E
- Karkanias I
- Karpov Sn
- Karpova Zm
- Kartvelishvili V
- Karyukhin An
- Kasimi E
- Kato C
- Katzy J
- Kaur S
- Kawade K
- Kawagoe K
- Kawaguchi T
- Kawamoto T
- Kawamura G
- Kay Ef
- Kaya Fi
- Kazakos S
- Kazanin Vf
- Ke Y
- Keaveney Jm
- Keeler R
- Kehris Gv
- Keller Js
- Kelly As
- Kelsey D
- Kempster Jj
- Kendrick J
- Kennedy Ke
- Kepka O
- Kerridge Bp
- Kersten S
- Kerševan Bp
- Keszeghova L
- Ketabchi Haghighat S
- Khandoga M
- Khanov A
- Kharlamov Ag
- Kharlamova T
- Khoda Ee
- Khoo Tj
- Khoriauli G
- Khubua J
- Khwaira Yar
- Kiehn M
- Kilgallon A
- Kim E
- Kim Yk
- Kimura N
- Kirchhoff A
- Kirchmeier D
- Kirfel C
- Kirk J
- Kiryunin Ae
- Kishimoto T
- Kisliuk Dp
- Kitsaki C
- Kivernyk O
- Klassen M
- Klein C
- Klein L
- Klein M
- Klein Mh
- Klein U
- Klimek P
- Klimentov A
- Klimpel F
- Klingl T
- Klioutchnikova T
- Klitzner Ff
- Kluit P
- Kluth S
- Kneringer E
- Knight Tm
- Knue A
- Kobayashi D
- Kobayashi R
- Kocian M
- Kodama T
- Kodyš P
- Koeck Dm
- Koenig Pt
- Koffas T
- Kolb M
- Koletsou I
- Komarek T
- Kong Axy
- Kono T
- Konstantinidis N
- Konya B
- Kopeliansky R
- Koperny S
- Korcyl K
- Kordas K
- Koren G
- Korn A
- Korn S
- Korolkov I
- Korotkova N
- Kortman B
- Kortner O
- Kortner S
- Kostecka Wh
- Kostyukhin Vv
- Kotsokechagia A
- Kotwal A
- Koulouris A
- Kourkoumeli-Charalampidi A
- Kourkoumelis C
- Kourlitis E
- Kovanda O
- Kowalewski R
- Kozanecki W
- Kozhin As
- Köhler Nm
- Köneke K
- Kramarenko Va
- Kramberger G
- Kramer P
- Krasny Mw
- Krasznahorkay A
- Kremer Ja
- Kretzschmar J
- Kreul K
- Krieger P
- Krieter F
- Krishnamurthy S
- Krishnan A
- Krivos M
- Krizka K
- Kroeninger K
- Kroha H
- Kroll J
- Kroll J
- Krowpman Ks
- Kruchonak U
- Krumnack N
- Kruse Mc
- Krüger H
- Krzysiak Ja
- Kubota A
- Kuchinskaia O
- Kuday S
- Kuechler D
- Kuechler Jt
- Kuehn S
- Kuhl T
- Kukhtin V
- Kulchitsky Y
- Kuleshov S
- Kumar M
- Kumari N
- Kuna M
- Kupco A
- Kupfer T
- Kupich A
- Kuprash O
- Kurashige H
- Kurchaninov Ll
- Kurochkin Ya
- Kurova A
- Kuwertz Es
- Kuze M
- Kvam Ak
- Kvita J
- Kwan T
- Kwok Kw
- Lacasta C
- Lacava F
- Lacker H
- Lacour D
- Lad Nn
- Ladygin E
- Laforge B
- Lagouri T
- Lai S
- Lakomiec Ik
- Lalloue N
- Lambert Je
- Lammers S
- Lampl W
- Lampoudis C
- Lancaster An
- Lançon E
- Landgraf U
- Landon Mpj
- Lang Vs
- Langenberg Rj
- Lankford Aj
- Lanni F
- Lantzsch K
- Lanza A
- Lapertosa A
- Laporte Jf
- Lari T
- Lasagni Manghi F
- Lassnig M
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- Lawrence Z
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- Zakharchuk N
- Zambito S
- Zang J
- Zanzi D
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- Zeitnitz C
- Zeißner Sv
- Zeng Jc
- Zenger Dt
- Zenin O
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- Zerradi S
- Zerwas D
- Zhang B
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- Zhang X
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- Zhao P
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu Y
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- Zhukov K
- Zhulanov V
- Zimine Ni
- Zinsser J
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- Zorbas Tg
- Zormpa O
- Zou W
- Zwalinski L
- Ženiš T
- Živković L
- Publication venue
- ELSEVIER
- Publication date
- 01/01/2023
- Field of study
Performance and calibration of quark/gluon-jet taggers using 140 fb⁻¹ of 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
- Adam Bourdarios C
- Adamczyk L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- 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
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amor Dos Santos SP
- Amos KR
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Anulli F
- Aoki M
- Aoki T
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Appelt C
- Apyan A
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- Arbiol Val SJ
- Arcangeletti C
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- Arena E
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- Assahsah J
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- Booth CD
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- Bordulev IS
- Borecka-Bielska HM
- Borissov G
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- Britzger D
- Brock I
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- Cavaliere V
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- Centonze MS
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- Chapon E
- Chargeishvili B
- Charlton DG
- Charman TP
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- Chekulaev SV
- Chelkov GA
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- Chwastowski JJ
- Cieri D
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- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
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- Zhong D
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- 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
- 'IOP Publishing'
- Publication date
- 01/02/2024
- Field of study
The identification of jets originating from quarks and gluons, often referred to as quark/gluon tagging,
plays an important role in various analyses performed at the Large Hadron Collider, as Standard Model measurements and searches for new particles decaying to quarks often rely on suppressing a large gluon-induced background. This paper describes the measurement of the efficiencies of quark/gluon taggers developed within the ATLAS Collaboration, using √s=13 TeV proton–proton collision data with an integrated luminosity of 140 fb-1 collected by the ATLAS experiment. Two taggers with high performances in rejecting jets from gluon over jets from
quarks are studied: one tagger is based on requirements on the number of inner-detector tracks associated with the
jet, and the other combines several jet substructure observables using a boosted decision tree. A method is established to determine the quark/gluon fraction in data, by using quark/gluon-enriched subsamples defined by the jet
pseudorapidity. Differences in tagging efficiency between data and simulation are provided for jets with transverse
momentum between 500 GeV and 2 TeV and for multiple tagger working points
Search for resonant production of dark quarks in the dijet final state 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
- Adam Bourdarios C
- Adamczyk L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Aktas S
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Alegria ZL
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- 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
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amor Dos Santos SP
- Amos KR
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Anulli F
- Aoki M
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- Aparo MA
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- Buzykaev AR
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- Cabrera Urbán S
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- Cai Y
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- Cairo VMM
- Cakir O
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- Calderini G
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- Camerlingo MT
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- Castillo FL
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- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
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- Zhu CG
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- Zhu Y
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- 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
- 'Springer Science and Business Media LLC'
- Publication date
- 16/02/2024
- Field of study
This paper presents a search for a new Z′ resonance decaying into a pair of dark quarks which hadronise into dark hadrons before promptly decaying back as Standard Model particles. This analysis is based on proton-proton collision data recorded at s
s
= 13 TeV with the ATLAS detector at the Large Hadron Collider between 2015 and 2018, corresponding to an integrated luminosity of 139 fb−1. After selecting events containing large-radius jets with high track multiplicity, the invariant mass distribution of the two highest-transverse-momentum jets is scanned to look for an excess above a data-driven estimate of the Standard Model multijet background. No significant excess of events is observed and the results are thus used to set 95% confidence-level upper limits on the production cross-section times branching ratio of the Z′ to dark quarks as a function of the Z′ mass for various dark-quark scenarios
Electron and photon energy calibration with the ATLAS detector using LHC Run 2 data
- Author
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- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
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- Zhemchugov A
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/02/2024
- Field of study
This paper presents the electron and photon energy calibration obtained with the ATLAS detector using 140 fb-1 of LHC proton-proton collision data recorded at √(s) = 13 TeV between 2015 and 2018. Methods for the measurement of electron and photon energies are outlined, along with the current knowledge of the passive material in front of the ATLAS electromagnetic calorimeter. The energy calibration steps are discussed in detail, with emphasis on the improvements introduced in this paper. The absolute energy scale is set using a large sample of Z-boson decays into electron-positron pairs, and its residual dependence on the electron energy is used for the first time to further constrain systematic uncertainties. The achieved calibration uncertainties are typically 0.05% for electrons from resonant Z-boson decays, 0.4% at ET ∼ 10 GeV, and 0.3% at ET ∼ 1 TeV; for photons at ET ∼ 60 GeV, they are 0.2% on average. This is more than twice as precise as the previous calibration. The new energy calibration is validated using J/ψ → ee and radiative Z-boson decays
Accuracy versus precision in boosted top tagging with the ATLAS detector
- Author
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- Aakvaag E
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- Abdelhameed S
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- Chen Y
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- Cheng HC
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- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
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- Zhemchugov A
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- IOP Publishing
- Publication date
- 01/08/2024
- Field of study
Abstract
The identification of top quark decays where the top quark has a large momentum transverse to the beam axis, known as top tagging, is a crucial component in many measurements of Standard Model processes and searches for beyond the Standard Model physics at the Large Hadron Collider.
Machine learning techniques have improved the performance of top tagging algorithms, but the size of the systematic uncertainties for all proposed algorithms has not been systematically studied.
This paper presents the performance of several machine learning based top tagging algorithms on a dataset constructed from simulated proton-proton collision events measured with the ATLAS detector at √
s
= 13 TeV.
The systematic uncertainties associated with these algorithms are estimated through an approximate procedure that is not meant to be used in a physics analysis, but is appropriate for the level of precision required for this study.
The most performant algorithms are found to have the largest uncertainties, motivating the development of methods to reduce these uncertainties without compromising performance.
To enable such efforts in the wider scientific community, the datasets used in this paper are made publicly available.</jats:p
Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb−1 of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si157.svg"><mml:mrow><mml:msqrt><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msqrt><mml:mo linebreak="goodbreak" linebreakstyle="after">=</mml:mo><mml:mn>13</mml:mn></mml:mrow></mml:math> TeV pp collision data
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- Zeng H
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- Zenger DT
- Zenin O
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- Zerwas D
- Zhai M
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- Zhao H
- Zhao P
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- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
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- 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 BV
- Publication date
- 01/07/2024
- Field of study
Results from a wide range of searches targeting different experimental signatures with and without missing transverse momentum (
) are used to constrain a Two–Higgs-Doublet Model (2HDM) with an additional pseudo-scalar mediating the interaction between ordinary and dark matter (2HDM + a). The analyses use up to 139 fb−1 of proton–proton collision data at a centre-of-mass energy
TeV recorded with the ATLAS detector at the Large Hadron Collider during 2015–2018. The results from three of the most sensitive searches are combined statistically. These searches target signatures with large
and a leptonically decaying Z boson; large
and a Higgs boson decaying to bottom quarks; and production of charged Higgs bosons in final states with top and bottom quarks, respectively. Constraints are derived for several common and new benchmark scenarios in the 2HDM + a
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