287 research outputs found
Active fixturing: literature review and future research directions
- Author
- A.A. Popov
- Abele E
- Anonymous
- Arzanpour S
- Bakker OJ
- Bakker OJ
- Bakker OJ
- Bakker OJ
- Bakker OJ
- Behzadi MR
- Benhabib B
- Bi ZM
- Bi ZM
- Boyle I
- Brecher C
- Bukowski A
- Cecil J
- Chaipradabgiat T
- Chakraborty D
- Chakraborty D
- Chan KC
- Chang M
- Culpepper ML
- Daimon M
- Dashchenko AI
- De Meter EC
- de Meter EC
- Deiab IM
- Deiab IM
- Deng H
- Deng H
- Denkena B
- Du H
- Du H
- Fang B
- Fleischer J
- Gao Y
- Geldart M
- Govender E
- Gupta S
- Hameed RA
- Hargrove SK
- Hazen BF
- Hurtado JN
- Izquierdo LE
- Jonsson M
- Kals HJJ
- Kang X
- Kaya N
- Kong Z
- Kurz K
- Lee J
- Leopold J
- Li B
- Li B
- Li Q
- Liao YG
- Mannan MA
- Mc Keown CM
- Meshreki M
- Mittal RO
- Motlagh HE
- Munro C
- Nee AYC
- Nee AYC
- Nee AYC
- Nikov TT
- O.J. Bakker
- Padmanaban KP
- Papastathis TN
- Papastathis TN
- Papastathis TN
- Park EJ
- Phuah HL
- Rai JK
- Rashid A
- Rashid A
- Ratchev S
- Ratchev S
- Rong Y
- Ryll M
- Ryll M
- S.M. Ratchev
- Sah S
- Shirinzadeh B
- Shirinzadeh B
- Siva Kumar K
- Siva Kumar K
- Sudsang A
- T.N. Papastathis
- Tao ZJ
- Tao ZJ
- Tian Z
- Tol UA
- Trappey JC
- Tuffentsammer K
- Varadarajan KM
- Vishnupriyan S
- Wagner R
- Walczyk DF
- Wang H
- Wang Y
- Wang YF
- Wiens GJ
- Yeh JH
- Yeung KY
- Zhang D
- Zhang XM
- Zhang Y
- Zhong ZW
- Publication venue
- 'Informa UK Limited'
- Publication date
- 01/01/2013
- Field of study
Fixtures are used to fixate, position and support workpieces and represent a crucial tool in manufacturing. Their performance determines the result of the whole manufacturing process of a product. There is a vast amount of research done on automatic fixture layout synthesis and optimisation and fixture design verification. Most of this work considers fixture mechanics to be static and the fixture elements to be passive. However, a new generation of fixtures has emerged that has actuated fixture elements for active control of the partâfixture system during manufacturing operations to increase the end product quality. This paper analyses the latest studies in the field of active fixture design and its relationship with flexible and reconfigurable fixturing systems. First, a brief introduction is given on the importance of research of fixturing systems. Secondly, the basics of workholding and fixture design are visited, after which the state-of-the-art in active fixturing and related concepts is presented. Fourthly, partâfixture dynamics and design strategies which take these into account are discussed. Fifthly, the control strategies used in active fixturing systems are examined. Finally, some final conclusions and prospective future research directions are presented
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
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- Zivkovic L
- Zobernig G
- Zoccoli A
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- 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 fbâ1 of â 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
A Bayesian Model for Detection of Highorder Interactions Among Genetic Variants in Genome-Wide Association Studies
- Author
- A Platt
- A Tovchigrechko
- AG Jones
- AM Burroughs
- Babu Valliyodan
- BW de Jong
- C Lu
- C Yang
- CL Snyder
- DM Weinreich
- Dong Xu
- F Johannes
- G Hemani
- H Ando
- Haiying Shi
- Henry T. Nguyen
- HY Lin
- J Rozas
- J Zhang
- JF Zhang
- Jing Zhang
- JR Zhang
- Juexin Wang
- JW Dudley
- JW Dudley
- JY Zhao
- K Van Steen
- M Rashid
- M Zhang
- MJ Hills
- ML Selley
- MS Breen
- MZ Xie
- QJ Song
- R Tibshirani
- RJ Weselake
- S Prabhu
- S Purcell
- S Rawsthorne
- T Joshi
- TA Manolio
- TF Hansen
- TFC Mackay
- Trupti Joshi
- W Zhang
- WH Wei
- XA Wan
- XJ Guo
- XL He
- XQ Huang
- Y Wang
- Y Zhang
- Y Zhang
- Yanchun Liang
- YN Zheng
- ZM Qi
- Publication venue
- ScholarWorks @ Georgia State University
- Publication date
- 01/01/2015
- Field of study
Background: A central question for disease studies and crop improvements is how genetics variants drive phenotypes. Genome Wide Association Study (GWAS) provides a powerful tool for characterizing the genotypephenotype relationships in complex traits and diseases. Epistasis (gene-gene interaction), including high-order interaction among more than two genes, often plays important roles in complex traits and diseases, but current GWAS analysis usually just focuses on additive effects of single nucleotide polymorphisms (SNPs). The lack of effective computational modelling of high-order functional interactions often leads to significant under-utilization of GWAS data. Results: We have developed a novel Bayesian computational method with a Markov Chain Monte Carlo (MCMC) search, and implemented the method as a Bayesian High-order Interaction Toolkit (BHIT) for detecting epistatic interactions among SNPs. BHIT first builds a Bayesian model on both continuous data and discrete data, which is capable of detecting high-order interactions in SNPs related to caseâcontrol or quantitative phenotypes. We also developed a pipeline that enables users to apply BHIT on different species in different use cases. Conclusions: Using both simulation data and soybean nutritional seed composition studies on oil content and protein content, BHIT effectively detected some high-order interactions associated with phenotypes, and it outperformed a number of other available tools. BHIT is freely available for academic users at http://digbio.missouri.edu/BHIT/
Immunophenotype and molecular characterisation of adenocarcinoma of the small intestine
- Author
- A Goel
- A Rashid
- A Rullier
- A Umar
- AC Wolff
- B Liu
- BG O'Riordan
- BH von Rahden
- CA Moskaluk
- DK McGregor
- H Blaker
- H Wang
- H Wang
- J L Abbruzzese
- J Pozadzides
- JA McKay
- JM DeSesso
- JR Howe
- K Hibi
- L Mirabelli-Primdahl
- L Zhu
- LM Ellis
- M J Overman
- M Paez-Ribes
- M Planck
- MA Jenkins
- MJ Lee
- MQ Zhang
- MQ Zhang
- NS Goldstein
- PL Dahia
- R A Wolff
- R Gryfe
- RW Werling
- S Bamford
- S Kopetz
- S Wen
- TS Loy
- V Stambolic
- WM Brueckl
- XP Zhou
- Y Yarden
- ZM Chen
- Publication venue
- Nature Publishing Group
- Publication date
- Field of study
Laparoscopy in management of appendicitis in high-, middle-, and low-income countries: a multicenter, prospective, cohort study.
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- Abantanga F
- Abbas M
- Abbo O
- Abd El Galeel A
- Abd El Hameed OS
- Abd El Hamid N
- Abd El Salam Y
- Abd El Slam M
- Abd El-Salam F
- Abd Elrasoul Y
- Abd-Elrasoul Y
- Abdallah E
- Abdel-Wahab NYE
- AbdelFattah I
- Abdelgelil A
- Abdelghany S
- Abdelkader M
- Abdelkareem A
- Abdelraheim M
- Abdelshafy M
- Abdulgawad M
- Abdullah AAN
- Abdullah NAN
- Abebe NS
- Abebe NS
- Aber A
- Abington E
- Aboarab A
- Aboraya M
- Aboraya M
- Abouelnasr A
- Abouzahra A
- Abozaid M
- Abozeid K
- Abozyed MAF
- Abudeeb H
- Abuseif M
- Acharya P
- Adams R
- Adebanjo A
- Adekoya A
- Adel A
- Adel A
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- Ademuyiwa AO
- Adeniran J
- Adeniyi A
- Adesanya O
- Adesina A
- Adesuyi A
- Adeyeye A
- Adham W
- Afandy A
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- Agarwal A
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- Aguilera M
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- Al-Faifi JJ
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- Al-Hasani RKMJ
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- Al-Mousa M
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- Al-Obaedi O
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- Zapata Ponze De Leon M
- Zardab A
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- Zerihun AB
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
BACKGROUND: Appendicitis is the most common abdominal surgical emergency worldwide. Differences between high- and low-income settings in the availability of laparoscopic appendectomy, alternative management choices, and outcomes are poorly described. The aim was to identify variation in surgical management and outcomes of appendicitis within low-, middle-, and high-Human Development Index (HDI) countries worldwide. METHODS: This is a multicenter, international prospective cohort study. Consecutive sampling of patients undergoing emergency appendectomy over 6Â months was conducted. Follow-up lasted 30Â days. RESULTS: 4546 patients from 52 countries underwent appendectomy (2499 high-, 1540 middle-, and 507 low-HDI groups). Surgical site infection (SSI) rates were higher in low-HDI (OR 2.57, 95% CI 1.33-4.99, pâ=â0.005) but not middle-HDI countries (OR 1.38, 95% CI 0.76-2.52, pâ=â0.291), compared with high-HDI countries after adjustment. A laparoscopic approach was common in high-HDI countries (1693/2499, 67.7%), but infrequent in low-HDI (41/507, 8.1%) and middle-HDI (132/1540, 8.6%) groups. After accounting for case-mix, laparoscopy was still associated with fewer overall complications (OR 0.55, 95% CI 0.42-0.71, pâ<â0.001) and SSIs (OR 0.22, 95% CI 0.14-0.33, pâ<â0.001). In propensity-score matched groups within low-/middle-HDI countries, laparoscopy was still associated with fewer overall complications (OR 0.23 95% CI 0.11-0.44) and SSI (OR 0.21 95% CI 0.09-0.45). CONCLUSION: A laparoscopic approach is associated with better outcomes and availability appears to differ by country HDI. Despite the profound clinical, operational, and financial barriers to its widespread introduction, laparoscopy could significantly improve outcomes for patients in low-resource environments. TRIAL REGISTRATION: NCT02179112
Combined measurement of differential and total cross sections in the HâŻââŻÎłÎł and the HâŻââŻZZ*âŻââŻ4â decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouzeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
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- Zwalinski L
- Ălvarez Piqueras D
- Ă kesson TPA
- Ć filigoj T
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fbâ1 of 13 TeV protonâproton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured Hâγγ and HâZZ*(â4â event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0â5.9 +6.0 (stat.) â3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Search for High-Mass Resonances Decaying to ÏÎœ in pp Collisions at âs=13 TeV with the ATLAS Detector
- Author
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- Yildirim E
- Yildiz H Duran
- Yorita K
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- Yuen SPY
- Yusuff I
- Zabinski B
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- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
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- Zhang F
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- Zhang J
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- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to ÏÎœ using proton-proton collisions at âs=13 TeV produced by the Large Hadron Collider is presented. Only Ï-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fbâ1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible ÏÎœ production cross section. Heavy WâČ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2â3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Operation and performance of the ATLAS Tile Calorimeter in Run 1
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouelfadl 
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez 
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor 
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Argos FC
- Arguin J-
- Argyropoulos S
- Armadans R
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME
- Atkin RJ
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- AÌlvarez Piqueras D
- AÌkesson TPA
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahilo JJL
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M
- Barkeloo J
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro GuimaraÌes da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batlamous S
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
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- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
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- Behera A
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- Bell AS
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- Belyaev NL
- Benary O
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- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
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- Beresford L
- Beretta M
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- Bergeaas Kuutmann E
- Berger N
- Bergsten LJ
- Beringer J
- Berlendis S
- Bernard NR
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertram IA
- Besjes GJ
- Bessidskaia Bylund O
- Bessner M
- Besson N
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- Bingul A
- Bini C
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- Bisanz T
- Biswal JP
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- Bjergaard DM
- Black JE
- Black KM
- Blair RE
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blunier D
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
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- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
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- Boonekamp M
- Borisov A
- Borissov G
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- Bostanabad M
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- Boumediene D
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- Boveia A
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- Breaden Madden WD
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- Briglin DL
- Britton D
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- Brock I
- Brock R
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- Brooks T
- Brooks WK
- Brost E
- Broughton JH
- Brown H
- Bruckman de Renstrom PA
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- Bruni A
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- Bruno S
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- Buat Q
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- Buckley AG
- Budagov IA
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- Bullock D
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burka K
- Burke S
- Burmeister I
- Burr JTP
- Busato E
- Buschmann E
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- BuÌhrer F
- BuÌscher D
- BuÌscher V
- Cabras G
- Cabrera UrbaÌn S
- Caforio D
- Cai H
- Cairo VMM
- Cakir I
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
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- Camacho Toro R
- Camarda S
- Camarri P
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- Caminal 
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
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- Cantero J
- Cao T
- Cao Y
- Capeans Garrido MDM
- Caprini I
- Caprini M
- Capua M
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- Cardillo FC
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- CarraÌ S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
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- Cerda Alberich L
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
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- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Chavez Barajas CA
- Che S
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- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
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- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
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- Chitan A
- Chiu I
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- Christodoulou V
- Chu MC
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- Cindro V
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- Ciocio A
- Cirotto F
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- Cuhadar Donszelmann T
- Cukierman AR
- Cunha 
- Curatolo M
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- Czodrowski P
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- Davydov Y
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- De Benedetti A
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
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- De Salvo A
- De Sanctis U
- De Santo A
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- Debenedetti C
- Dedovich DV
- Dehghanian N
- Del Gaudio M
- Del Peso J
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- Denysiuk D
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- Deterre C
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- Deviveiros PO
- Dewhurst A
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- Dubreuil A
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- Dumitriu AE
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- Etienvre AI
- Etzion E
- Evans H
- Ezhilov A
- Ezzi M
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- Falke PJ
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- Fassi F
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- Fassouliotis D
- Faucci Giannelli M
- Favareto A
- Fawcett WJ
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- Fenyuk AB
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- Ferreira de Lima DE
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- Fiolhais MCN
- Fiorini L
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- Fisher WC
- Flaschel N
- Fleck I
- Fleischmann P
- Fletcher RRM
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- Flierl BM
- Flores Castillo LR
- Flores LM
- Fomin N
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- Formica A
- Forti AC
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- FoÌrster FA
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- Francavilla P
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- Fressard-Batraneanu SM
- Freund B
- Freund WS
- Froidevaux D
- Frost JA
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- Furelos D
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- Galea C
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- GarciÌa Navarro JE
- GarciÌa Pascual JA
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- Girolamo A
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- Giugni D
- Giuli F
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- Gkialas I
- Gkougkousis EL
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- Gorbounov PA
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- Goshaw AT
- Gostkin MI
- Gottardo CA
- Goudet CR
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- Goussiou AG
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- Hawkings RJ
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- Kuwertz ES
- Kuze M
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- La Rotonda L
- La Ruffa F
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- Lanfermann MC
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- Law AT
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- LeBlanc M
- LeCompte T
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- Lee CA
- Lee GR
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- Leight WA
- Leisos A
- Leite MAL
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- Liberti B
- Liblong A
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- Limosani A
- Lin CY
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- Lindquist BE
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- Lopez 
- Lopez JA
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- Ma Y
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- Martyniuk AC
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- Mc Kee SP
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- McKay MA
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- Zwalinski L
- ZÌenisÌ T
- ZÌivkovicÌ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The Tile Calorimeter is the hadron calorimeter covering the central region of the ATLAS experiment at the Large Hadron Collider. Approximately 10,000 photomultipliers collect light from scintillating tiles acting as the active material sandwiched between slabs of steel absorber. This paper gives an overview of the calorimeterâs performance during the years 2008â2012 using cosmic-ray muon events and protonâproton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fbâ1. The signal reconstruction methods, calibration systems as well as the detector operation status are presented. The energy and time calibration methods performed excellently, resulting in good stability of the calorimeter response under varying conditions during the LHC Run 1. Finally, the Tile Calorimeter response to isolated muons and hadrons as well as to jets from protonâproton collisions is presented. The results demonstrate excellent performance in accord with specifications mentioned in the Technical Design Report
Performance of missing transverse momentum reconstruction with the ATLAS detector using protonâproton collisions at âs = 13 TeV
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in protonâproton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying Ï -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fbâ1
Measurement of the tÂŻtZ and tÂŻtW cross sections in proton-proton collisions at âs=13âTeV with the ATLAS detector
- Author
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- Aad G
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- Abbott DC
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (tÂŻt) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1ââfbâ1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The tÂŻtZ and tÂŻtW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are ÏtÂŻtZ=0.95±0.08stat±0.10systâpb and ÏtÂŻtW=0.87±0.13stat±0.14systâpb in agreement with the Standard Model predictions. The measurement of the tÂŻtZ cross section is used to set constraints on effective field theory operators which modify the tÂŻtZ vertex
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