399 research outputs found
Metabolism of a synthetic compared with a natural therapeutic pulmonary surfactant in adult mice
- Author
- Publication venue
- Publication date
- 01/10/2018
- Field of study
Secreted pulmonary surfactant phosphatidylcholine (PC) has a complex intra-alveolar metabolism that involves uptake and recycling by alveolar type II epithelial cells, catabolism by alveolar macrophages, and loss up the bronchial tree. We compared the in vivo metabolism of animal-derived poractant alfa (Curosurf) and a synthetic surfactant (CHF5633) in adult male C57BL/6 mice. The mice were dosed intranasally with either surfactant (80 mg/kg body weight) containing universally 13C-labeled dipalmitoyl PC (DPPC) as a tracer. The loss of [U13C]DPPC from bronchoalveolar lavage and lung parenchyma, together with the incorporation of 13C-hydrolysis fragments into new PC molecular species, was monitored by electrospray ionization tandem mass spectrometry. The catabolism of CHF5633 was considerably delayed compared with poractant alfa, the hydrolysis products of which were cleared more rapidly. There was no selective resynthesis of DPPC and, strikingly, acyl remodeling resulted in preferential synthesis of polyunsaturated PC species. In conclusion, both surfactants were metabolized by similar pathways, but the slower catabolism of CHF5633 resulted in longer residence time in the airways and enhanced recycling of its hydrolysis products into new PC species
Structural insight into SUMO chain recognition and manipulation by the ubiquitin ligase RNF4
- Author
- A Hershko
- A Plechanovova
- A Plechanovova
- A Rojas-Fernandez
- AM Weissman
- AT Brunger
- AT Namanja
- CC Chang
- CH Cheng
- CM Hecker
- CM Pickart
- CW Liew
- D Reverter
- E Escobar-Cabrera
- ES Johnson
- F Ikeda
- FM Lin
- GNB Yip
- H Sun
- HD Ulrich
- HY Sun
- I Matic
- J Marchant
- J Prudden
- J Song
- J Song
- J Xia
- JD Schnell
- JH Hurley
- JL Battiste
- JS Thrower
- K Keusekotten
- L Deng
- M Ottiger
- M Zweckstetter
- MH Tatham
- MH Tatham
- MJ Eddins
- MJ Eddins
- MR Hansen
- MS Rodriguez
- N Sekiyama
- N Zhang
- O Kerscher
- O Kerscher
- Q Wang
- R Bruderer
- R Lescasse
- R Mahajan
- R Varadan
- RT Hay
- S-R Tzeng
- SC Panchal
- W Rieping
- W-C Huang
- XD Zhang
- Y Shen
- Y Xie
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2014
- Field of study
The small ubiquitin-like modifier (SUMO) can form polymeric chains that are important signals in cellular processes such as meiosis, genome maintenance and stress response. The SUMO-targeted ubiquitin ligase RNF4 engages with SUMO chains on linked substrates and catalyses their ubiquitination, which targets substrates for proteasomal degradation. Here we use a segmental labelling approach combined with solution nuclear magnetic resonance (NMR) spectroscopy and biochemical characterization to reveal how RNF4 manipulates the conformation of the SUMO chain, thereby facilitating optimal delivery of the distal SUMO domain for ubiquitin transfer
Effects of alirocumab on types of myocardial infarction: insights from the ODYSSEY OUTCOMES trial
- Author
- Abbas J
- Abbate A
- Abdullakutty J
- Abhyanakar AD
- Aboyans V
- Abrantes JAM
- Abu-Fadel M
- Acevedo M
- Adamkova V
- Adhyapak S
- Agarwal H
- Aggarwal R
- Aggarwal RK
- Aguirre A
- Ahmed H
- Ahremark U
- Ahuad Guerrero RA
- Aidar Ayoub JC
- Airaksinen JK
- Aitken D
- Akatova E
- Akhter F
- Ako J
- Akright L
- Akyea-Djamson A
- Al Joundi T
- Al-Windy NYY
- Alan D
- Alcocer Gamba MA
- Alexander JH
- Alexander K
- Alexandru TM
- Alings M
- Alonso Martin JJ
- Alvarisqueta AF
- Alves De Lima AE
- Amarasekera S
- Amarasena N
- Amir O
- Amlani M
- Amosova E
- Amuchastegui M
- Andersen K
- Andersen R
- Anderson J
- Ando K
- Angel Hominal M
- Annam S
- Anscombe R
- Apostolovic SR
- Appel K-F
- Arandjelovic A
- Araneda G
- Arango Benecke JL
- Arbel Y
- Arif I
- Armaganijan L
- Arroyo JAC
- Arstall MA
- Asanin MR
- Atar S
- Athyros V
- Auguadro C
- Ayala CAC
- Aylward PE
- Azizad MM
- Bagai A
- Bagriy A
- Bahit MC
- Bai F
- Balaguer Recena J
- Baldari D
- Balinovac J
- Ball E
- Bang LE
- Banuru S
- Barakovic F
- Baranov E
- Baranova E
- Barbarash OL
- Barbato E
- Barna OM
- Barone-Rochette G
- Barr C
- Barrucco R
- Bartels GL
- Bashir R
- Basson MMDV
- Bastos JM
- Bata I
- Batushkin V
- Bayat J
- Bayram Llamas EA
- Bayron C
- Beauloye C
- Bednarski J
- Behrens S
- Belhassane A
- Benedicto A
- Bengus CM
- Benov HO
- Berger R
- Berglund S
- Berk M
- Berland J
- Berli MA
- Berlowitz M
- Berman B
- Bernan A
- Berti S
- Bhagwat A
- Bhagwat R
- Bhansali P
- Bhatt DL
- Binder R
- Birchem J
- Bittner VA
- Blicharski T
- Blok T
- Blumberg EDS
- Boccara F
- Bodanese LC
- Bodi Peris V
- Boecker D
- Bojovski S
- Bokarev I
- Bokern MJJA
- Bonfanti AJC
- Bono JOE
- Bordonava AP
- Borse R
- Bortnick A
- Bos RJ
- Botas Rodriguez J
- Botelho A
- Botelho RV
- Botia DCL
- Bottcher M
- Bourgeois R
- Brabham D
- Braganza D
- Braun-Dullaeus R
- Breedveld RW
- Brennan JM
- Brodison A
- Bronzwaer PNA
- Brueren BRG
- Bruguera Cortada J
- Budaj A
- Bugan V
- Busmane A
- Bustamante Labarta MH
- Busz-Papiez B
- Butler R
- Bystryk L
- Caccavo A
- Caime GD
- Calabro P
- Camprubi Potau M
- Camsari A
- Caraco Y
- Carey C
- Carlson E
- Carnero GS
- Carranza Madrigal J
- Carrillo Calvillo J
- Carroll PA
- Cartasegna LR
- Carter L
- Caruso OC
- Cassimjee S
- Castadot M
- Cavallini C
- Cequier Fillat AR
- Cerqueira MJAG
- Cestari HG
- Cevc M
- Cha J
- Chae I-H
- Chaitman B
- Chalavarya G
- Chaleff F
- Chambilla JMC
- Chandna H
- Chane M
- Chang M
- Chaudhary S
- Chavez V-CER
- Chen D
- Chen J
- Chen Y
- Cheng S-C
- Cheng X
- Chiang C-E
- Chiang C-E
- Chizhov P
- Chopda M
- Chopra VK
- Christenson S
- Chu A
- Chua T
- Chumakova G
- Chumburidze V
- Civeira Murillo F
- Claeys M
- Clemmensen P
- Clerc J
- Cleveland D
- Clifford P
- Clifton S
- Coching RM
- Codutti OR
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- Colombo HR
- Colquhoun D
- Commerford PJ
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- Constantinescu MCA
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- Cuccia C
- Cui L
- Cyster HP
- Czerski T
- D'Urso M
- Daboul N
- Dagher G
- Dahl C
- Dai K
- Dalby AJ
- Dalby AJ
- Danchin N
- Dandillaya R
- Daniels C
- Das S
- Davidovic G
- Davidsen F
- Davies R
- Davis W
- De Berrazueta Fernandez JR
- De Cesare NB
- De Leo A
- De Luca G
- De Mora Martin M
- De Pellegrin A
- De Salazar DIM
- de Santos MON
- de Silva HA
- de Souza JA
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- Demirtas M
- Denham D
- Devarapalli SK
- DeVore AD
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- Dilic M
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- Dimov BI
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- Ding C
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- Dombrowski K
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- Dorobantu M
- Dorsel T
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- Drexel H
- Drzewiecka A
- Ducas J
- Ducrocq G
- Duda N
- Dujardin K
- Dukat A
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- Dzupina A
- Dzyak G
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- Fadlallah H
- Faes D
- Faggiano P
- Fairlamb J
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- Falukozy J
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- Fang W
- Fanghanel Salmon G
- Farhat N
- Farrar M
- Fausto Ovando SR
- Fazekas F
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- Feitosa GS
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- Fuchs S
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- Fujii K
- Fujimoto K
- Fujinaga H
- Fulop P
- Fulwani MC
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- Galvani M
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- Giordano JA
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- Gislason G
- Giuliano ME
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- Groenemeijer BE
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- Guardigli G
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- Gullestad L
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- Gusi Tragant G
- Guzman PN
- Haddad T
- Hagstrom E
- Hagstrom E
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- Halabi M
- Halcox J
- Hald F
- Haldis T
- Hall J
- Halvorsen S
- Hameed A
- Haniffa R
- Hanotin C
- Hansen O
- Haraguchi T
- Harding S
- Harkut P
- Harrington RA
- Harris B
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- Hart H
- Hata Y
- Hattler B
- Hedman A
- Heidenreich L
- Heinc P
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- Higashikata T
- Higuera JD
- Hii CLS
- Hirayama A
- Hirooka K
- Hlatky MA
- Hoag G
- Hodes Z
- Hoffer E
- Hoffman D
- Hong T
- Hoogslag PAM
- Hoppe U
- Horak D
- Horowitz J
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- Hrabar AD
- Hranai M
- Hsieh I-C
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- Irimpen A
- Istratoaie O
- Ito K
- Ivanov IG
- Ivanova R
- Ivanovic N
- Iyengar SS
- Izzo M
- Jacoby D
- Jafar Z
- Jaffrani N
- Jain D
- Janik M
- Janosik D
- Jaramillo N
- Jatin FGM
- Jaworska K
- Jayawardena J
- Jensen SA
- Jensen SA
- Jeong MH
- Jeppesen J
- Jeserich M
- Jiang W
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- Johansen PB
- Jonas M
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- Jortveit J
- Joshi AB
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- Jurgaitiene R
- Kadr H
- Kaewsuwanna P
- Kahali D
- Kaikkonen K
- Kaiser S
- Kalashetti S
- Kalil R
- Kamensky G
- Kamiya H
- Kandasamy B
- Kapin T
- Kaplan R
- Kapp IE
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- Kedev S
- Keen W
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- Kerkar P
- Khabeishvili G
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- Khaisheva L
- Khan A
- Khan A
- Khan M
- Khasanov N
- Khintibidze I
- Khurana S
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- Koike A
- Koldas L
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- Kornder J
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- Korol M
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- Kosmachova E
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- Kotha P
- Kouz S
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- Kozuma K
- Krasowski W
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- Kristensen KS
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- Zuniga JDH
- Zurakowski A
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- Zweiker R
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 01/01/2019
- Field of study
Aims The third Universal Definition of Myocardial Infarction (MI) Task Force classified MIs into five types: Type 1, spontaneous; Type 2, related to oxygen supply/demand imbalance; Type 3, fatal without ascertainment of cardiac biomarkers; Type 4, related to percutaneous coronary intervention; and Type 5, related to coronary artery bypass surgery. Low-density lipoprotein cholesterol (LDL-C) reduction with statins and proprotein convertase subtilisin–kexin Type 9 (PCSK9) inhibitors reduces risk of MI, but less is known about effects on types of MI. ODYSSEY OUTCOMES compared the PCSK9 inhibitor alirocumab with placebo in 18 924 patients with recent acute coronary syndrome (ACS) and elevated LDL-C (≥1.8 mmol/L) despite intensive statin therapy. In a pre-specified analysis, we assessed the effects of alirocumab on types of MI. Methods and results Median follow-up was 2.8 years. Myocardial infarction types were prospectively adjudicated and classified. Of 1860 total MIs, 1223 (65.8%) were adjudicated as Type 1, 386 (20.8%) as Type 2, and 244 (13.1%) as Type 4. Few events were Type 3 (n = 2) or Type 5 (n = 5). Alirocumab reduced first MIs [hazard ratio (HR) 0.85, 95% confidence interval (CI) 0.77–0.95; P = 0.003], with reductions in both Type 1 (HR 0.87, 95% CI 0.77–0.99; P = 0.032) and Type 2 (0.77, 0.61–0.97; P = 0.025), but not Type 4 MI. Conclusion After ACS, alirocumab added to intensive statin therapy favourably impacted on Type 1 and 2 MIs. The data indicate for the first time that a lipid-lowering therapy can attenuate the risk of Type 2 MI. Low-density lipoprotein cholesterol reduction below levels achievable with statins is an effective preventive strategy for both MI types.For complete list of authors see http://dx.doi.org/10.1093/eurheartj/ehz299</p
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
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- Zemaityte G
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Ziolkowski M
- Zoccoli A
- Zoch K
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fb−1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17−15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7−6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
Measurements of W+W−+ ≥ 1 jet production cross-sections in pp collisions at s = 13 TeV with the ATLAS detector
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- Abbott B
- Abbott DC
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- Abeling K
- Abhayasinghe DK
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- Zemaityte G
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- Zhang X
- Zhang Z
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- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Fiducial and differential cross-section measurements of W+W− production in
association with at least one hadronic jet are presented. These measurements are sensitive
to the properties of electroweak-boson self-interactions and provide a test of perturbative
quantum chromodynamics and the electroweak theory. The analysis is performed using
proton-proton collision data collected at p
s = 13TeV with the ATLAS experiment, corresponding
to an integrated luminosity of 139 fb−1. Events are selected with exactly one oppositely
charged electron-muon pair and at least one hadronic jet with a transverse momentum
of pT > 30 GeV and a pseudorapidity of |�| < 4.5. After subtracting the background
contributions and correcting for detector effects, the jet-inclusive W+W−+ � 1 jet fiducial
cross-section and W+W−+ jets differential cross-sections with respect to several kinematic
variables are measured. These measurements include leptonic quantities, such as the lepton
transverse momenta and the transverse mass of the W+W− system, as well as jet-related
observables such as the leading jet transverse momentum and the jet multiplicity. Limits on
anomalous triple-gauge-boson couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous amplitude is enhanced
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
- Author
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
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
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- Aad G
- Aakvaag E
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- Abeling K
- Abicht NJ
- Abidi SH
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- Zakharchuk N
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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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- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao T
- Zhao Y
- Zhao Z
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- 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 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
Measurements of sensor radiation damage in the ATLAS inner detector using leakage currents
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud A Abed
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
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- Zwalinski L
- Publication venue
- IOP
- Publication date
- 01/01/2021
- Field of study
Non-ionizing energy loss causes bulk damage to the silicon sensors of the ATLAS pixel and strip detectors. This damage has important implications for data-taking operations, charged-particle track reconstruction, detector simulations, and physics analysis. This paper presents simulations and measurements of the leakage current in the ATLAS pixel detector and semiconductor tracker as a function of location in the detector and time, using data collected in Run 1 (2010–2012) and Run 2 (2015–2018) of the Large Hadron Collider. The extracted fluence shows a much stronger |z|-dependence in the innermost layers than is seen in simulation. Furthermore, the overall fluence on the second innermost layer is significantly higher than in simulation, with better agreement in layers at higher radii. These measurements are important for validating the simulation models and can be used in part to justify safety factors for future detector designs and interventions.publishedVersio
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
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- Zhemchugov A
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- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
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- Zou W
- 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
Two-particle azimuthal correlations in photonuclear ultraperipheral Pb plus Pb collisions at 5.02 TeV with ATLAS
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- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
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- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
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- Alberghi GL
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- Weston TD
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- Whiteson D
- Wiedenmann W
- Wiel C
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- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams DM
- Williams HH
- Williams S
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- Windischhofer PJ
- Wingerter-Seez I
- Winklmeier F
- Winter BT
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- Wongel AF
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- Worm SD
- Wosiek BK
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- Wyatt TR
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- Xella S
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- Xiotidis I
- Xu D
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- Xu T
- Xu W
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- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamatani M
- Yamauchi H
- Yamazaki T
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- Yan J
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- Yang HJ
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- Yang X
- Yang Y
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- Yao W-M
- Yap YC
- Ye H
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- Yeletskikh I
- Yexley MR
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zagazeta LFG
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
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- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/07/2021
- Field of study
Two-particle long-range azimuthal correlations are measured in photonuclear collisions using
1.7
nb
−
1
of 5.02 TeV
Pb
+
Pb
collision data collected by the ATLAS experiment at the CERN Large Hadron Collider. Candidate events are selected using a dedicated high-multiplicity photonuclear event trigger, a combination of information from the zero-degree calorimeters and forward calorimeters, and from pseudorapidity gaps constructed using calorimeter energy clusters and charged-particle tracks. Distributions of event properties are compared between data and Monte Carlo simulations of photonuclear processes. Two-particle correlation functions are formed using charged-particle tracks in the selected events, and a template-fitting method is employed to subtract the nonflow contribution to the correlation. Significant nonzero values of the second- and third-order flow coefficients are observed and presented as a function of charged-particle multiplicity and transverse momentum. The results are compared with flow coefficients obtained in proton-proton and proton-lead collisions in similar multiplicity ranges, and with theoretical expectations. The unique initial conditions present in this measurement provide a new way to probe the origin of the collective signatures previously observed only in hadronic collision
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