216 research outputs found
Challenges and opportunities for smallholder livestock production in post-conflict South Kivu, eastern DR Congo
- Author
- Publication venue
- Springer Netherlands
- Publication date
- 01/01/2012
- Field of study
A survey on smallholder livestock production with emphasis on monogastric animals was conducted in 20 villages of seven so-called ‘groupements’ of South Kivu province in DR Congo, situated along a north to south-west axis with the town of Bukavu in the center. This land adjacent to Lake Kivu is located at elevations ranging around 900–1900 m asl, experiencing tropical highland climate. A diagnostic survey helped to rapidly obtain in-depth knowledge of constraints and opportunities in this environment. Correspondence analysis and multiple regression analysis were used to investigate the association of production constraints with particular livestock species and to understand the factors that govern the number of livestock that people owned (converted to tropical livestock units [TLU]), respectively. Responses of 112 informants demonstrated that livestock is an integral part of the region’s mixed farming systems. Low livestock numbers per household at present reflect the poverty as a consequence of recent violent conflicts. Currently, farmers focus on small livestock, like poultry, swine, cavies (i.e., Guinea pigs) and rabbits. Families keep livestock to accumulate household reserves that are strongly invested in children’s education. Major issues of animal husbandry were related to animal diseases and lack of feed resources, particularly in the dry season. Lack of feed or forages were unrelated to a particular livestock species. Livestock holdings depended on animal diversity, location, land size available and respondents’ education level. The potential introduction of improved forages is challenged by their dry-season tolerance, compatibility with cropping on small farms; and people’s readiness to cultivate forages
Substance use risk profiles and associations with early substance use in adolescence
- Author
- A Andersen
- A Caspi
- B Hibell
- BW Roberts
- C Brunelle
- CR Cloninger
- CR Cloninger
- CS Carver
- CY Chen
- DJ Wit De
- E Kuntsche
- E Kuntsche
- E Kuntsche
- ER Galaif
- F Smit
- Geertjan Overbeek
- GR Parra
- HZ Reinherz
- J Akse
- J Akse
- J Cohen
- Jeroen Lammers
- JH Lacey
- JH Steiger
- JJ Arnett
- JW Jaffee
- K Flory
- K Monshouwer
- K Monshouwer
- Karin Monshouwer
- KJ Sher
- KM Jackson
- KM Loewenthal
- L Hu
- L Pulkkinen
- LR Bergman
- M Galizio
- M Shall
- M Spoont
- M Zuckerman
- ML Cooper
- MM Dolcini
- Monique Malmberg
- N Breslau
- N Comeau
- ND Brener
- PA Woicik
- PJ Conrod
- PJ Conrod
- PJ Conrod
- PJ Conrod
- PL Ellickson
- PM Bentler
- PT Barrett
- PT Costa
- R Otten
- RA McCormick
- RA Peterson
- RC O’Connor
- RCME Engels
- Rutger C. M. E. Engels
- SB Eysenck
- SF Tapert
- SH Stewart
- SL Bailey
- SP Kremers
- SR Reis
- T Asparouhov
- TE Joiner
- TJ Dishion
- W Feigelman
- Wilma A. M. Vollebergh
- WW Hale III
- Z Harakeh
- Publication venue
- Springer US
- Publication date
- 01/01/2010
- Field of study
We examined whether anxiety sensitivity, hopelessness, sensation seeking, and impulsivity (i.e., revised version of the Substance Use Risk Profile Scale) would be related to the lifetime prevalence and age of onset of alcohol, tobacco, and cannabis use, and to polydrug use in early adolescence. Baseline data of a broader effectiveness study were used from 3,783 early adolescents aged 11–15 years. Structural equation models showed that hopelessness and sensation seeking were indicative of ever-used alcohol, tobacco or cannabis and for the use of more than one substance. Furthermore, individuals with higher levels of hopelessness had a higher chance of starting to use alcohol or cannabis at an earlier age, but highly anxiety sensitive individuals were less likely to start using alcohol use at a younger age. Conclusively, early adolescents who report higher levels of hopelessness and sensation seeking seem to be at higher risk for an early onset of substance use and poly substance use
Icelandic herring-eating killer whales feed at night
- Author
- A Dommasnes
- A Friedlaender
- A Friedlaender
- C Guinet
- F Thomsen
- Filipa I. P. Samarra
- FIP Samarra
- FIP Samarra
- FIP Samarra
- Gaëtan Richard
- GJ Óskarsson
- GL Thomas
- H Yurk
- I Huse
- IC Opzeeland Van
- Ivan D. Fedutin
- J Plötz
- JC Holst
- JHS Blaxter
- JK Ford
- JK Ford
- JKB Ford
- JM Casey
- KJ Benoit-Bird
- KS Norris
- KS Norris
- L Barrett-Lennard
- L Nøttestad
- L Peichl
- M Biuw
- M Hindell
- M Simon
- M Simon
- M Simon
- MA Bigg
- MA McDonald
- Marc Lammers
- MO Lammers
- MO Lammers
- OA Filatova
- OA Filatova
- OA Filatova
- OA Filatova
- Olga A. Filatova
- P Arranz
- P Miller
- Patrick J. Miller
- PJ Miller
- PJB Slater
- PJO Miller
- PJO Miller
- PJO Miller
- R Riesch
- R Riesch
- RB Tyson
- RM Sibly
- RW Baird
- RW Baird
- RW Baird
- RW Baird
- S Cerchio
- T Jaud
- T Schaffeld
- T Similä
- V Deecke
- VB Deecke
- VLG Todd
- VM Janik
- WT Fitch
- WW Au
- Z Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
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
- 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
- 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
- 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
- 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
- Bakalis C
- Baker OK
- Bakos E
- Bakshi Gupta D
- Balakrishnan V
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Baltes LM
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barakat M
- Barberio EL
- Barberis D
- Barbero M
- 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
- Baselga M
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Battulga D
- Bauce M
- Bauer M
- Bauer P
- Bazzano Hurrell LT
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HP
- Becker K
- Becot C
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belyaev NL
- Benchekroun D
- Bendebba F
- Benhammou Y
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Bergeaas Kuutmann E
- Berger N
- Bergmann B
- Beringer J
- Bernardi G
- Bernius C
- Bernlochner FU
- Bernon F
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- Berta P
- Berthold A
- Bertram IA
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- Betti A
- Bevan AJ
- Bhamjee M
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Bianco G
- Biebel O
- Bielski R
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- 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
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- Bomben M
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- Boonekamp M
- Booth CD
- Borbély AG
- Bordulev IS
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bouaouda K
- Bouchhar N
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
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- Britton D
- Britzger D
- Brock I
- Brooijmans G
- Brooks WK
- Brost E
- Brown LM
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- Bruckler TL
- Bruckman de Renstrom PA
- Bruni A
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- 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
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- Buxo Vazquez CJ
- Buzykaev AR
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- Caforio D
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- Cairo VMM
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- Calafiura P
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- Callea G
- Caloba LP
- Calvet D
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- Calvet TP
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- Camarda S
- Camarero Munoz D
- Camarri P
- Camerlingo MT
- Cameron D
- Camincher C
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- Canesse A
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- Capocasa F
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- Cardenas JCJ
- Cardillo F
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- Carlotto JI
- Carlson BT
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- Castiglia EG
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- Castillo Gimenez V
- Castillo FL
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- Catinaccio A
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- Cavaliere V
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- Cavasinni V
- Cekmecelioglu YC
- Celebi E
- Celli F
- Centonze MS
- Cepaitis V
- Cerny K
- Cerqueira AS
- Cerri A
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- Cervato B
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- Cesarini G
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- Chapman JD
- Chapon E
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chauhan C
- Chekanov S
- Chekulaev SV
- Chelkov GA
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- Cherepanova E
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- Clavijo Columbie JM
- Clawson SE
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- Coccaro A
- Coelho Barrue RF
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- Coimbra AEC
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- Curcio F
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- Denisov SP
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- Dumitriu AE
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- Dwyer BL
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- Dziedzic BS
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- Fleischmann P
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- Flores Sanz De Acedo L
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- Golubkov D
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- Gongadze A
- Gonnella F
- Gonski JL
- Gonzalez Fernandez S
- Gonzalez Lopez R
- Gonzalez Renteria C
- Gonzalez Rodrigues MV
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- Gonzalvo Rodriguez GR
- González Andana RY
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- Zhemchugov A
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- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
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- Zwalinski L
- 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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- Xu Z
- Yabsley B
- Yacoob S
- Yamaguchi N
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- 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
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
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- Aakvaag E
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- Abeling K
- Abicht NJ
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- Zhemchugov A
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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
Performance and calibration of quark/gluon-jet taggers using 140 fb⁻¹ of pp collisions at √s=13 TeV with the ATLAS detector
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- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
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- 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
- '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
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- Alfonsi F
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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
- Allendes Flores CA
- Allport PP
- Aloisio A
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- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
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- Carter JWS
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- Zhemchugov A
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- 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
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- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhulanov V
- Zimine NI
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- 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
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
- Aad G
- Aakvaag E
- Abbott B
- Abdelhameed S
- Abeling K
- Abicht NJ
- Abidi SH
- Aboelela M
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Ackermann A
- Adamczyk 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
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Aitbenchikh B
- Akbiyik M
- Akimov AV
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- Cherepanova E
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- Ciesla KM
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- de Renstrom PAB
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- Kersten S
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- Keszeghova L
- Khan RA
- Khanov A
- Kharlamov AG
- Kharlamova T
- Khoda EE
- Kholodenko M
- Khoo TJ
- Khoriauli G
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- Khwaira YAR
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- Kim D
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- Kirk J
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- Klein C
- Klein L
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- Klein SB
- Klein U
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- Klimentov A
- Klioutchnikova T
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- Knight TM
- Knue A
- Kobylianskii D
- Koch SF
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- Kodyš P
- Koeck DM
- Koenig PT
- Koffas T
- Kolay O
- Koletsou I
- Komarek T
- Kong AXY
- Kono T
- Konstantinidis N
- Kontaxakis P
- Konya B
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- Koperny S
- Korcyl K
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- Korotkova N
- Kortman B
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- 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
- Kramarenko VA
- Kramberger G
- Kramer P
- Krasny MW
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- Kraus AC
- Kraus JW
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- Kuday S
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- Kurdysh O
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- Kurova A
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- Kwan T
- Kyriacou NG
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- Lacasta C
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- Lad NN
- Ladygin E
- Lafarge A
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- Lahbabi FZ
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- Lambert JE
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- Lankford AJ
- Lanni F
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- Lanza A
- Lançon E
- Laporte JF
- Lari T
- Lassnig M
- Latonova V
- Latour BMD
- Laurier A
- Lawlor SD
- Lawrence Z
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- Lazzaroni M
- Le Boulicaut EM
- Le Pottier LT
- Le B
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- Lebedev A
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- Liberti B
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- Liu JB
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- Loiacono E
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- Longarini I
- Longo R
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- Lopez-canelas NA
- Lory AM
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- Loseva O
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- Love PA
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- Luehring F
- Luengo SIF
- Luise I
- Lukianchuk O
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- Lundberg O
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- Lutz MS
- Lux AB
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- Lysak R
- Lytken E
- Lyubushkin V
- Lyubushkina T
- Lyukova MM
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- Topolnicki KW
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- Zhemchugov A
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- 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
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