277 research outputs found
A Novel Class of Tyrosyl-DNA Phosphodiesterase 1 Inhibitors That Contains the Octahydro-2H-chromen-4-ol Scaffold.
- Author
- Publication venue
- 'MDPI AG'
- Publication date
- 01/09/2018
- Field of study
Tyrosyl-DNA phosphodiesterase 1 (Tdp1) is a DNA repair enzyme that mends topoisomerase 1-mediated DNA damage. Tdp1 is a current inhibition target for the development of improved anticancer treatments, as its inhibition may enhance the therapeutic effect of topoisomerase 1 poisons. Here, we report a study on the development of a novel class of Tdp1 inhibitors that is based on the octahydro-2H-chromene scaffold. Inhibition and binding assays revealed that these compounds are potent inhibitors of Tdp1, with IC50 and KD values in the low micromolar concentration range. Molecular modelling predicted plausible conformations of the active ligands, blocking access to the enzymatic machinery of Tdp1. Our results thus help establish a structural-activity relationship for octahydro-2H-chromene-based Tdp1 inhibitors, which will be useful for future Tdp1 inhibitor development work
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
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
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine NI
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- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
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- Alshehri AA
- Alstaty MI
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- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
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- Anders JK
- Anderson KJ
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- Andrei V
- Angelidakis S
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- Arduh FA
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- Armadans R Caminal
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- Zivkovic L
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- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
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
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- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
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- Abramowicz H
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- Abusleme Hoffman AC
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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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- Wyatt TR
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- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
- Zhai M
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- Zhang J
- Zhang K
- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- 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
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
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- Adamek L
- Addepalli Sv
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder Aa
- Afik Y
- Agaras Mn
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- Zeißner Sv
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- Zerradi S
- Zerwas D
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- Zhao P
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zimine Ni
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- 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
- Aranzabal N
- Arbiol Val SJ
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Assahsah J
- Assamagan K
- Astalos R
- Atashi S
- Atkin RJ
- Atkinson M
- 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
- Baines L
- Baker OK
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- Bakshi Gupta D
- Balakrishnan V
- Balasubramanian R
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- Ballabene E
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- Balunas WK
- Balz J
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- Bandyopadhyay A
- Bansal S
- Barak L
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- Barberio EL
- Barberis D
- Barbero M
- Barel MZ
- Barends KN
- Barillari T
- Barisits M-S
- Barklow T
- Baron Moreno DA
- Baron P
- Baroncelli A
- Barone G
- Barr AJ
- Barr JD
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- Barreiro F
- Barron U
- Barros Teixeira MG
- Barsov S
- Bartels F
- Bartoldus R
- Barton AE
- Bartos P
- Basan A
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- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
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- Battulga D
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- Bazzano Hurrell LT
- Beacham JB
- Beau T
- Beaucamp JY
- Beauchemin PH
- Becherer F
- Bechtle P
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- Beddall AJ
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begalli M
- Begel M
- Behera A
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- Beirer JF
- Beisiegel F
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- Bella G
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- Benchekroun D
- Bendebba F
- Benhammou Y
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
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- Berger N
- Bergmann B
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- Bernardi G
- Bernius C
- Bernlochner FU
- Bernon F
- Berrocal Guardia A
- Berry T
- Berta P
- Berthold A
- Bertram IA
- Bethke S
- Betti A
- Bevan AJ
- Bhalla NK
- Bhamjee M
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Bianco G
- Biebel O
- Bielski R
- Biglietti M
- Bindi M
- Bingul A
- Bini C
- Biondini A
- Birch-sykes CJ
- Bird GA
- Birman M
- Biros M
- Biryukov S
- Bisanz T
- Bisceglie E
- Biswal JP
- Biswas D
- Bitadze A
- Bjørke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
- Boehler M
- Boehm B
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbély AG
- Bordulev IS
- Borecka-Bielska HM
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bouaouda K
- Bouchhar N
- 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
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Britton D
- Britzger D
- Brock I
- Brooijmans G
- Brooks WK
- Brost E
- Brown LM
- Bruce LE
- Bruckler TL
- Bruckman de Renstrom PA
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Brüers B
- Buanes T
- Buat Q
- Buchin D
- Buckley AG
- Bulekov O
- Bullard BA
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burlayenko O
- 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
- Cabrera Urbán S
- Cadamuro L
- Caforio D
- Cai H
- Cai Y
- Cai Y
- Cairo VMM
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
- Calvet S
- Calvet TP
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- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capocasa F
- Capua M
- Carbone A
- Cardarelli R
- Cardenas JCJ
- Cardillo F
- Carducci G
- Carli T
- Carlino G
- Carlotto JI
- Carlson BT
- Carlson EM
- Carminati L
- Carnelli A
- Carnesale M
- Caron S
- Carquin E
- Carratta G
- Carrio Argos F
- Carrá S
- Carter JWS
- Carter TM
- Casado MP
- Caspar M
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cavaliere V
- Cavalli N
- Cavasinni V
- Cekmecelioglu YC
- Celebi E
- Celli F
- Centonze MS
- Cepaitis V
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervato B
- Cervelli A
- Cesarini G
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WY
- Chapman JD
- Chapon E
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chauhan C
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
- Chen H
- Chen H
- Chen J
- Chen J
- Chen M
- Chen S
- Chen SJ
- Chen X
- Chen X
- Chen Y
- Cheng CL
- Cheng HC
- Cheong S
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiedde N
- Chiodini G
- Chisholm AS
- Chitan A
- Chitishvili M
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
- Chow EYS
- Chowdhury T
- 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
- Clarry C
- 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
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- Connell MP
- Connell SH
- Connelly IA
- Conroy EI
- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cordeiro Oudot Choi A
- Corpe LD
- Corradi M
- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
- Costanza F
- Costanzo D
- Cote BM
- Cowan G
- Cranmer K
- Cremonini D
- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosby JE
- Crosetti G
- Crépé-Renaudin S
- Cueto A
- Cuhadar Donszelmann T
- Cui H
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- Zhemchugov A
- Zheng J
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- Zhong D
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- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
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- 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
Electron and photon energy calibration with the ATLAS detector using LHC Run 2 data
- Author
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- Abbott B
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- Abicht NJ
- Abidi SH
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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
- '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
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