15 research outputs found
Composite anodes for lithium-ion batteries: status and trends
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- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
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- Field of study
Porous carbon spheres: Recent developments and applications
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Encapsulation of probiotics: insights into academic and industrial approaches
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- Publication date
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Pursuit of paired dijet resonances in the Run 2 dataset with ATLAS
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- Zhulanov V
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- Zinsser J
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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
New particles with large masses that decay into hadronically interacting particles are predicted by many models of physics beyond the Standard Model. A search for a massive resonance that decays into pairs of dijet resonances is performed using..
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
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- Zhemchugov A
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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
Measurement of the t t ¯ cross section and its ratio to the Z production cross section using pp collisions at s = 13.6 TeV with the ATLAS detector
- Author
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- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
- Zhang DF
- Zhang J
- Zhang J
- Zhang K
- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- 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
- 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
- Elsevier
- Publication date
- 01/12/2023
- Field of study
Tools for estimating fake/non-prompt lepton backgrounds with the ATLAS detector at the LHC
- Author
- Aad G
- Abbott B
- Abbott DC
- 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
- Asai K
- Asai S
- Asbah NA
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Auriol AD
- Austrup VA
- Avner G
- Avolio G
- Axiotis K
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahilo JJL
- Bahmani M
- Bailey AJ
- Bailey VR
- Baines JT
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- Bakos E
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- Balunas WK
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- Barton AE
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- Birch-sykes CJ
- Bird GA
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- Bugge MK
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- Bullard BA
- Burdin S
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- Calderini G
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- Callea G
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- Camerlingo MT
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- Camplani A
- Canale V
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- Cao Y
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- Cerri A
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- Cerutti F
- Cervelli A
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- Chadi Z
- Chakraborty D
- Chala M
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- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
- Chen H
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- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen X
- Chen Y
- Cheng CL
- Cheng HC
- Cheong S
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiedde N
- Chiodini G
- Chisholm AS
- Chitan A
- Chitishvili M
- 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
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- Coelli S
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- Coimbra AEC
- Cole B
- collaboration TA
- Collot J
- Columbie JMC
- Connell MP
- Connell SH
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- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cormier F
- Cornell SD
- Corpe LD
- Corradi M
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- Corrigan EE
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- Cortes-Gonzalez A
- Costa MJ
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- Cote BM
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- Cowan G
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- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
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- Crépé-Renaudin S
- Cueto A
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- Cui Z
- Cunningham WR
- Curcio F
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- Czurylo MM
- D'amen G
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- D'uffizi M
- 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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- Dahbi S
- Dai T
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- Dam M
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- Daneri MF
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- Dao V
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- Das SJ
- David C
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- Davis-Purcell B
- Dawson I
- de Andrade Filho LM
- De Araujo MV
- De Asmundis R
- De Beurs M
- De Biase N
- 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 Moura NMJN
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santo A
- De Sousa MJDCS
- De Souza EEP
- De K
- Dedovich DV
- Degens J
- Deiana AM
- Del Corso F
- Del Peso J
- Del Rio F
- Delegido AJG
- 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
- 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
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- Dinu I-M
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- HAL CCSD
- Publication date
- 29/11/2022
- Field of study
International audienceMeasurements and searches performed with the ATLAS detector at the CERN LHC often involve signatures with one or more prompt leptons. Such analysesare subject to `fake/non-prompt' lepton backgrounds, where either a hadron or a lepton from a hadron decay or an electron from a photon conversion satisfies the prompt-leptonselection criteria. These backgrounds often arise within a hadronic jet because of particle decays in the showering process, particle misidentification or particleinteractions with the detector material. As it is challenging to model these processes with high accuracy in simulation, their estimation typically uses data-driven methods.Three methods for carrying out this estimation are described, along with their implementation in ATLAS and their performance
Search for a new pseudoscalar decaying into a pair of muons in events with a top-quark pair at s=13 TeV with the ATLAS detector
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- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
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- Zenger DT
- Zenin O
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- Zerwas D
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- Zhang X
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- Zhang Y
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- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
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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
- American Physical Society (APS)
- Publication date
- 01/01/2023
- Field of study
A search for a new pseudoscalar Formula Presented-boson produced in events with a top-quark pair, where the Formula Presented-boson decays into a pair of muons, is performed using Formula Presented Formula Presented collision data collected with the ATLAS detector at the LHC, corresponding to an integrated luminosity of Formula Presented. The search targets the final state where only one top quark decays to an electron or muon, resulting in a signature with three leptons Formula Presented and Formula Presented. No significant excess of events above the Standard Model expectation is observed and upper limits are set on two signal models: Formula Presented and Formula Presented with Formula Presented, Formula Presented, where Formula Presented, in the mass ranges Formula Presented and Formula Presented
Observation of Wγγ triboson production in proton-proton 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
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- 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
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- 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-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Arnaez O
- 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
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- Atmasiddha PA
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- Auricchio S
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- Austrup VA
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- Axiotis K
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
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- Bahmani M
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- Bailey VR
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- Bakalis C
- Baker OK
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- Baldin EM
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- Balunas WK
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- Bandyopadhyay A
- Bansal S
- Barak L
- Barakat M
- Barberio EL
- Barberis D
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- Blumenthal J
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- Busch EL
- Bussey PJ
- Butler JM
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- Butterworth JM
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- Buzykaev AR
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- Cabras G
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- Caforio D
- Cai H
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- Calafiura P
- Calderini G
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- Caloba LP
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- Canale V
- Canesse A
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- Carlson BT
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- Cheremushkina E
- Cherepanova E
- Cheu E
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- Ciesla KM
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- Ciocio A
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- Yan J
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- Yao W-M
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- Yeo BK
- Yexley MR
- Yildiz HD
- Yin P
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- Younas S
- Young C
- Young CJS
- Yu Y
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- Yuan R
- Yue L
- Zaazoua M
- Zabinski B
- Zagazeta LFG
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
- Zhang DF
- Zhang J
- 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
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- 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
- Elsevier
- Publication date
- 01/12/2023
- Field of study
Fast b-tagging at the high-level trigger of the ATLAS experiment in LHC Run 3
- 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
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- 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
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- Alfonsi F
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- Alhroob M
- Ali B
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- Alibocus SW
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- Alimonti G
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allen JF
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- Aly M
- Ambler A
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- 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
- Anulli F
- Aoki M
- Aoki T
- Aparo MA
- Appelt C
- Apyan A
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
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- Argos FC
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- Tamir NM
- Tamlihat MA
- Tanaka A
- Tanaka J
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- Tao Z
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- Tarem S
- Tariq K
- Tarna G
- Tartarelli GF
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- Traeet A
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- Yildiz HD
- Yin P
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- Zagazeta LFG
- Zaid E
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- Zakharchuk N
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- Zang J
- Zanzi D
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- Zeng H
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- Zenger DT
- Zenin O
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- Zerwas D
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- Zhemchugov A
- Zheng J
- Zheng K
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- Zhong D
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- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
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- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- IOP Publishing
- Publication date
- 01/11/2023
- Field of study
The ATLAS experiment relies on real-time hadronic jet reconstruction and b-tagging to record fully hadronic events containing b-jets. These algorithms require track reconstruction, which is computationally expensive and could overwhelm the high-level-trigger farm, even at the reduced event rate that passes the ATLAS first stage hardware-based trigger. In LHC Run 3, ATLAS has mitigated these computational demands by introducing a fast neural-network-based b-tagger, which acts as a low-precision filter using input from hadronic jets and tracks. It runs after a hardware trigger and before the remaining high-level-trigger reconstruction. This design relies on the negligible cost of neural-network inference as compared to track reconstruction, and the cost reduction from limiting tracking to specific regions of the detector. In the case of Standard Model HH → bb̅bb̅, a key signature relying on b-jet triggers, the filter lowers the input rate to the remaining high-level trigger by a factor of five at the small cost of reducing the overall signal efficiency by roughly 2%