411 research outputs found
Icodextrin as salvage therapy in peritoneal dialysis patients with refractory fluid overload
- Author
- Publication venue
- BioMed Central
- Publication date
- 01/12/2001
- Field of study
BACKGROUND: Icodextrin is a high molecular weight, starch-derived glucose polymer, which is capable of inducing sustained ultrafiltration over prolonged (12–16 hour) peritoneal dialysis (PD) dwells. The aim of this study was to evaluate the ability of icodextrin to alleviate refractory, symptomatic fluid overload and prolong technique survival in PD patients. METHODS: A prospective, open-label, pre-test/post-test study was conducted in 17 PD patients (8 females/9 males, mean age 56.8 ± 2.9 years) who were on the verge of being transferred to haemodialysis because of symptomatic fluid retention that was refractory to fluid restriction, loop diuretic therapy, hypertonic glucose exchanges and dwell time optimisation. One icodextrin exchange (2.5 L 7.5%, 12-hour dwell) was substituted for a long-dwell glucose exchange each day. RESULTS: Icodextrin significantly increased peritoneal ultrafiltration (885 ± 210 ml to 1454 ± 215 ml, p < 0.05) and reduced mean arterial pressure (106 ± 4 to 96 ± 4 mmHg, p < 0.05), but did not affect weight, plasma albumin concentration, haemoglobin levels or dialysate:plasma creatinine ratio. Diabetic patients (n = 12) also experienced improved glycaemic control (haemoglobin Alc decreased from 8.9 ± 0.7% to 7.9 ± 0.7%, p < 0.05). Overall PD technique survival was prolonged by a mean of 11.6 months (95% CI 6.0–17.3 months). On multivariate Cox proportional hazards analysis, extension of technique survival by icodextrin was only significantly predicted by baseline net daily peritoneal ultrafiltration (adjusted HR 2.52, 95% CI 1.13–5.62, p < 0.05). CONCLUSIONS: Icodextrin significantly improved peritoneal ultrafiltration and extended technique survival in PD patients with symptomatic fluid overload, especially those who had substantially impaired peritoneal ultrafiltration
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
- Author
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- Wolters H
- Wong VWS
- Woods NL
- Worm SD
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- Wozniak KW
- Wraight K
- Wu SL
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- Yexley MR
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- Yildiz HD
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- Zemaityte G
- Zeng JC
- Zenin O
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- Zhang B
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- Zhang J
- Zhang L
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- Zhang R
- Zhang S
- Zhang X
- Zhang Y
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- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- 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
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- 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
Improvement of adynamic bone disease after renal transplantation
- Author
- A. Borelli
- Bianchi ML
- Bover JA
- Casez JP
- Coco M
- Cruz EAS
- Cueto-Manzano AM
- David-Neto E
- E. David-Neto
- Faugere MC
- Garcia-Carrasco M
- Heaf JG
- Jorgetti V
- Julian BA
- K.A. Abdallah
- L.E. Ianhez
- L.M. dos Reis
- L.M. Pereira
- Lo Cascio V
- Melsen F
- Moshe L
- Ott SM
- P.H.S. Corrêa
- Parfitt AM
- Parker CR
- R.C. Pereira
- R.M.A. Moysés
- Rojas E
- Salusky IB
- Sprague SM
- Torres A
- V. Jorgetti
- Weinstein RS
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
CKD-MBD after kidney transplantation
- Author
- A Delucchi
- A Mussa
- A Siirtola
- A Sweatt
- AC Hokken-Koelega
- AE Kruse
- AM Cueto-Manzano
- AM D'Alessandro
- AW Root
- BA Julian
- BD Parker
- BM Chavers
- C Movsowitz
- C Ponticelli
- C Schafer
- CF Helvig
- CH June
- CP Sanchez
- DB Allen
- DS Milliner
- EA Cruz
- EM Ruth
- F Velasquez-Forero
- FJ Maritz
- G Lehmann
- G Ortoft
- H Holdaas
- H Valta
- HD McIntyre
- HP Bryer
- I Bhan
- I Helenius
- I Helenius
- I Szwarc
- J Aubia
- J Bacchetta
- J Bacchetta
- J Bacchetta
- J Oh
- JM Quesada
- JM Saland
- Justine Bacchetta
- JW Coburn
- JW Groothoff
- JW Groothoff
- JW Pritchett
- K Borchhardt
- K Bostrom
- K Lippuner
- KA Borchhardt
- Katherine Wesseling-Perry
- KDIGO Work Group
- LA Soyka
- LK Bachrach
- LT Weber
- M Ajmal
- M Burrows
- M Garabedian
- M Hristova
- MB Ishitani
- MF Holick
- MJ van Summeren
- ML Bianchi
- MM Mitsnefes
- MM Sarwal
- MM Sarwal
- MR Rubin
- N Koh
- N Leca
- NX Chen
- O Alvarez-Garcia
- OM Gutierrez
- P Evenepoel
- P Evenepoel
- Q Cui
- R Amerling
- R Grenda
- RC Shroff
- RG Carlini
- RN Fine
- RW Chesney
- S Ahmed
- S Jono
- S Moe
- S Patel
- S Seiler
- S Tuchman
- SL Fan
- SM Bartosh
- SM Moe
- SM Moe
- SM Moe
- T Schinke
- TJ Hahn
- TL Clemens
- TR Srinivas
- W Grotz
- W Gwinner
- WB Wehrenberg
- WG Goodman
- Y Bilginer
- Y Imanishi
- Publication venue
- Springer-Verlag
- Publication date
- Field of study
Successful kidney transplantation corrects many of the metabolic abnormalities associated with chronic kidney disease (CKD); however, skeletal and cardiovascular morbidity remain prevalent in pediatric kidney transplant recipients and current recommendations from the Kidney Disease Improving Global Outcomes (KDIGO) working group suggest that bone disease—including turnover, mineralization, volume, linear growth, and strength—as well as cardiovascular disease be evaluated in all patients with CKD. Although few studies have examined bone histology after renal transplantation, current data suggest that bone turnover and mineralization are altered in the majority of patients and that biochemical parameters are poor predictors of bone histology in this population. Dual energy X-ray absorptiometry (DXA) scanning, although widely performed, has significant limitations in the pediatric transplant population and values have not been shown to correlate with fracture risk; thus, DXA is not recommended as a tool for the assessment of bone density. Newer imaging techniques, including computed tomography (quantitative CT (QCT), peripheral QCT (pQCT), high resolution pQCT (HR-pQCT) and magnetic resonance imaging (MRI)), which provide volumetric assessments of bone density and are able to discriminate bone microarchitecture, show promise in the assessment of bone strength; however, future studies are needed to define the value of these techniques in the diagnosis and treatment of renal osteodystrophy in pediatric renal transplant recipients
C.E.R.A. maintains stable hemoglobin in Latin American patients on dialysis
- Author
- A Roche
- AM Cueto-Manzano
- B Canaud
- B Spinowitz
- Beatriz Espinoza
- Carlos Henríquez
- CE Halstenson
- D Fliser
- DE Leaf
- Elizabeth De Francesco-Daher
- Emma Schwedt
- F Carrera
- F Locatelli
- F Locatelli
- G Garcia–Garcia
- IC Macdougall
- Ignacio Villanueva
- JP Ebben
- KDOQI
- Kleyton Bastos
- Luis Antonio Lucarelli
- M Munoz
- ML Thorp
- ND Vaziri
- NW Levin
- R Paniagua
- R Pecoits-Filho
- Ricardo Correa-Rotter
- Roberto Pecoits Filho
- Ruben Schiavelli
- S Fishbane
- W Sulowicz
- W Yang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alunno Camelia E
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Aranzabal N
- Araujo Ferraz V
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Arrubarrena Tame ZP
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Backman F
- Badea A
- Bagnaia P
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Bakos E
- Bakshi Gupta D
- Balaji S
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barends KN
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- Barreiro F
- Barron U
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bashta I
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer P
- Bawa HS
- Bayirli A
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HP
- Becker K
- Becot C
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirao Da Cruz E Silva C
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Berthold A
- Bertram IA
- Bessidskaia Bylund O
- Bethke S
- Betti A
- Bevan AJ
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Biebel O
- Bielski R
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birch-sykes CJ
- Bird GA
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjørke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbély AG
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bouquet R
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Breaden Madden WD
- Brendlinger K
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Bruckman de Renstrom PA
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Bryngemark L
- Brüers B
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Bugge MK
- Bulekov O
- Bullard BA
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buxo Vazquez CJ
- Buzykaev AR
- Büscher V
- Cabras G
- Cabrera Urbán S
- Caforio D
- Cai H
- Cairo VMM
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cano Bret M
- Cantero J
- Cao Y
- Capua M
- Carbone A
- Cardarelli R
- Cardillo F
- Carducci G
- Carli T
- Carlino G
- Carlson BT
- Carlson EM
- Carminati L
- Carnesale M
- Carney RMD
- Caron S
- Carquin E
- Carratta G
- Carrá S
- Carter JWS
- Carter TM
- Casadei D
- Casado MP
- Casha AF
- Castiglia EG
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- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zgubič M
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- 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 N
- Zhou Y
- Zhu C
- Zhu CG
- 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
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- 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
- Author
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- Abbott B
- Abbott DC
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- Abeling K
- Abhayasinghe DK
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- Zhang X
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- Zhao Y
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- 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 sensor radiation damage in the ATLAS inner detector using leakage currents
- Author
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- Abbott B
- Abbott DC
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- Abhayasinghe DK
- Abidi SH
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- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerwas D
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhuang X
- 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
- 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
Performance of the upgraded PreProcessor of the ATLAS Level-1 Calorimeter Trigger
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
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- Acharya BS
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- Zimmermann S
- Zinonos Z
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- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2020
- Field of study
The PreProcessor of the ATLAS Level-1 Calorimeter Trigger prepares the analogue trigger signals sent from the ATLAS calorimeters by digitising, synchronising, and calibrating them to reconstruct transverse energy deposits, which are then used in further processing to identify event features. During the first long shutdown of the LHC from 2013 to 2014, the central components of the PreProcessor, the Multichip Modules, were replaced by upgraded versions that feature modern ADC and FPGA technology to ensure optimal performance in the high pile-up environment of LHC Run 2. This paper describes the features of the newMultichip Modules along with the improvements to the signal processing achieved.ANPCyTYerPhI, ArmeniaAustralian Research CouncilBMWFW, AustriaAustrian Science Fund (FWF)Azerbaijan National Academy of Sciences (ANAS)SSTC, BelarusNational Council for Scientific and Technological Development (CNPq)Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP)Natural Sciences and Engineering Research Council of CanadaCanada Foundation for InnovationNational Natural Science Foundation of China (NSFC)Departamento Administrativo de Ciencia, Tecnología e Innovación ColcienciasMinistry of Education, Youth & Sports - Czech Republic
Czech Republic GovernmentCzech Republic GovernmentDNRF, DenmarkDanish Natural Science Research CouncilCentre National de la Recherche Scientifique (CNRS)CEA-DRF/IRFU, FranceFederal Ministry of Education & Research (BMBF)Max Planck SocietyGreek Ministry of Development-GSRTRGC and Hong Kong SAR, ChinaIsrael Science FoundationBenoziyo Center, IsraelIstituto Nazionale di Fisica Nucleare (INFN)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)
Japan Society for the Promotion of ScienceCNRST, MoroccoRCN, NorwayPortuguese Foundation for Science and TechnologyMNE/IFA, RomaniaMES of RussiaMESTD, SerbiaMSSR, SlovakiaSlovenian Research Agency - SloveniaMIZS, SloveniaSpanish GovernmentSRC, SwedenWallenberg Foundation, SwedenSNSF Geneva, SwitzerlandMinistry of Science and Technology, TaiwanMinistry of Energy & Natural Resources - TurkeyScience & Technology Facilities Council (STFC)United States Department of Energy (DOE)National Science Foundation (NSF)BCKDF, CanadaCANARIE, CanadaCRC, CanadaEuropean Research Council (ERC)European Union (EU)French National Research Agency (ANR)German Research Foundation (DFG)Alexander von Humboldt FoundationGreek NSRF, GreeceBSF-NSF, IsraelGerman-Israeli Foundation for Scientific Research and DevelopmentLa Caixa Banking Foundation, SpainCERCA Programme Generalitat de Catalunya, SpainPROMETEO, SpainGenT Programmes Generalitat Valenciana, SpainGoran Gustafssons Stiftelse, SwedenRoyal Society of LondonLeverhulme TrustNRC, CanadaCERNANID, ChileChinese Academy of SciencesMinistry of Science and Technology, ChinaSRNSFG, GeorgiaHGF, GermanyNetherlands Organization for Scientific Research (NWO)
Netherlands GovernmentMinistry of Science and Higher Education, PolandNCN, PolandNRCKI, Russia FederationJINRDST/NRF, South AfricaSERI, Geneva, SwitzerlandCantons of Bern and Geneva, SwitzerlandCompute Canada, CanadaHorizon 2020Marie Sklodowska-Curie ActionsEuropean Cooperation in Science and Technology (COST)EU-ESF, Greec
Measurement of the energy asymmetry in t(t)over-barj production at 13 TeV with the ATLAS experiment and interpretation in the SMEFT framework
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- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
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- Zhemchugov A
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 28/04/2022
- Field of study
A measurement of the energy asymmetry in jet-associated top-quark pair production is presented using 139fb−1
139
fb
-
1
of data collected by the ATLAS detector at the Large Hadron Collider during pp collisions at s=13TeV
s
=
13
TeV
. The observable measures the different probability of top and antitop quarks to have the higher energy as a function of the jet scattering angle with respect to the beam axis. The energy asymmetry is measured in the semileptonic ttˉ
t
t
¯
decay channel, and the hadronically decaying top quark must have transverse momentum above 350GeV
350
GeV
. The results are corrected for detector effects to particle level in three bins of the scattering angle of the associated jet. The measurement agrees with the SM prediction at next-to-leading-order accuracy in quantum chromodynamics in all three bins. In the bin with the largest expected asymmetry, where the jet is emitted perpendicular to the beam, the energy asymmetry is measured to be −0.043±0.020
-
0.043
±
0.020
, in agreement with the SM prediction of −0.037±0.003
-
0.037
±
0.003
. Interpreting this result in the framework of the Standard Model effective field theory (SMEFT), it is shown that the energy asymmetry is sensitive to the top-quark chirality in four-quark operators and is therefore a valuable new observable in global SMEFT fits
- …