122 research outputs found
Building generic anatomical models using virtual model cutting and iterative registration
- Author
- A Guimond
- A Guimond
- B Avants
- B Schmutz
- BD Argall
- Benedikt Hallgrímsson
- CG Small
- Christoph W Sensen
- CW Sensen
- D Ruckert
- DC Barratt
- E Kristensen
- E Maschino
- Eric Schmidt
- H Olafsdottir
- Jung Soh
- KT Rajamani
- LR Dice
- M Xiao
- Mei Xiao
- Oscar Meruvia-Pastor
- PA Yushkevich
- PM Thompson
- PV Bayly
- R Brandt
- S Schaefer
- S Schaefer
- S Zachow
- T Chen
- W Schroeder
- WS Rasband
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
Article deposited according to publisher policy posted on SHERPA/RoMEO, 30/07/2010.YesFunding provided by the Open Access Authors Fund
Cysteamine broadly improves the anti-plasmodial activity of artemisinins against murine blood stage and cerebral malaria
- Author
- A Fortin
- A Laroque
- A Nilsen
- AC Allison
- AM Dondorp
- AM Stickles
- Anny Fortin
- Bart De Spiegeleer
- BM Greenwood
- BM Kotecka
- C Amaratunga
- CM Smith
- EA Ashley
- EB Belldina
- F Ariey
- G Kokwaro
- G Min-Oo
- G Min-Oo
- G Min-Oo
- H Noedl
- IH Cheeseman
- J Berghout
- J Berghout
- J Straimer
- JA Gangoiti
- Jalal Hawari
- Kirsten Vandercruyssen
- KT Batty
- Mary M. Stevenson
- MB Isah
- MC Fidler
- Mifong Tam
- NA Malmquist
- Neda Moradin
- NJ White
- NX Thanh
- O Miotto
- Philippe Gros
- PN Soh
- R Dohil
- R Kleta
- R Longley
- RC Reddy
- RT Eastman
- S Krishna
- S Mishra
- S Mok
- S Torre
- Sabrina Torre
- SE Bongfen
- SK Mishra
- SM Taylor
- Susan Gauthier
- T Antoine
- T Efferth
- TJ Lamb
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
No evidence that genetic variation in the myeloid-derived suppressor cell pathway influences ovarian cancer survival
- Author
- Abrams SI
- Anton-Culver H
- Bandera EV
- Battaglia S
- Beckmann MW
- Berchuck A
- Bjørge L
- Bruegl A
- Campbell IG
- Campbell SP
- Cannioto R
- Chang-Claude J
- Chenevix-Trench G
- Clay AI
- Cramer D
- Dansonka-Mieszkowska A
- Dao F
- Diergaarde B
- Doerk T
- Doherty JA
- du Bois A
- Eccles D
- Eng KH
- Engelholm SA
- Etter JL
- Fasching PA
- Gayther SA
- Gentry-Maharaj A
- Glasspool RM
- Goode EL
- Goodman MT
- Gronwald J
- Harter P
- Hein A
- Heitz F
- Hillemmanns P
- Hogdall C
- Hu Q
- Huzarski T
- Høgdall EV
- Jensen A
- Johnatty SE
- Joseph J
- Jung A
- Karlan B
- Klapdor R
- Kluz T
- Konopka B
- Krüger Kjær S
- Kupryjanczyk J
- Lambrechts D
- Lester J
- Levine DA
- Liu S
- Lubiński J
- Lundvall L
- Mayor P
- McGuire V
- McNeish IA
- Menon U
- Minlikeeva A
- Modugno F
- Moysich KB
- Ness RB
- Odunsi K
- Orsulic S
- Paul J
- Pearce CL
- Pejovic T
- Pharoah P
- Ramus SJ
- Rossing MA
- Rothstein J
- Rübner M
- Schildkraut JM
- Schmalfeldt B
- Schwaab I
- Segal B
- Siddiqui N
- Sieh W
- Sobiczewski P
- Soh KT
- Song H
- Sucheston-Campbell LE
- Szender JB
- Terry KL
- Van Nieuwenhuysen E
- Vanderstichele A
- Vergote I
- Wallace PK
- Walsh CS
- Webb PM
- Wentzensen N
- Whittemore AS
- Wu AH
- Ziogas A
- Zsiros EZ
- Publication venue
- Publication date
- 01/03/2017
- Field of study
BACKGROUND: The precise mechanism by which the immune system is adversely affected in cancer patients remains poorly understood, but the accumulation of immune suppressive/pro-tumorigenic myeloid-derived suppressor cells (MDSCs) is thought to be one prominent mechanism contributing to immunologic tolerance of malignant cells in epithelial ovarian cancer (EOC). To this end, we hypothesized genetic variation in MDSC pathway genes would be associated with survival after EOC diagnoses. METHODS: We measured the hazard of death due to EOC within 10 years of diagnosis, overall and by invasive subtype, attributable to SNPs in 24 genes relevant in the MDSC pathway in 10,751 women diagnosed with invasive EOC. Versatile Gene-based Association study (VEGAS) and the Admixture Likelihood method (AML), were used to test gene and pathway associations with survival. RESULTS: We did not identify individual SNPs that were significantly associated with survival after correction for multiple testing (p<3.5 x 10-5), nor did we identify significant associations between the MDSC pathway overall, or the 24 individual genes and EOC survival. CONCLUSIONS: In this well-powered analysis, we observed no evidence that inherited variations in MDSC-associated SNPs, individual genes, or the collective genetic pathway contributed to EOC survival outcomes. IMPACT: Common inherited variation in genes relevant to MDSCs were not associated with survival in women diagnosed with invasive EOC
Research on information systems failures and successes: Status update and future directions
- Author
- A Bhattacherjee
- A Burton-Jones
- A Elbanna
- A Rai
- AD Brown
- AM Pettigrew
- Amany Elbanna
- AR Elbanna
- C Barclay
- C Maier
- C Maier
- C Soh
- CF Gibson
- D Kroenke
- DA Adams
- David Wastell
- Deborah Bunker
- DJ Bunker
- DM Strong
- EJ Garrity
- EL Glass
- G Fitzgerald
- G Johns
- G Pan
- G Walsham
- GG Gable
- H Barki
- H Klaus
- HC Lucas
- Helle Zinner Henriksen
- HK Klein
- J Caseley
- J Iivari
- J Lee
- J Scott
- JC Lee
- JS Jasperson
- K McGrath
- KB Hendricks
- KR Linberg
- KRT Larsen
- KT Yeo
- L Wallace
- LA Kappelman
- LB Mohr
- LJ Kirsch
- M Bergman
- M Igbaria
- M Keil
- M Martinsons
- M Zachariadis
- M. N. Ravishankar
- MA Shareef
- MD Myers
- Michael D. Myers
- MJ Ginzberg
- ML Markus
- ML Markus
- ML Markus
- MN Ravishankar
- N Cerpa
- N Melville
- N Pollock
- N Urbach
- NP Rana
- NP Rana
- O Volkoff
- O Volkoff
- P Bamberger
- P Beynon-Davies
- P Beynon-Davies
- P Lowry
- PB Seddon
- R Heeks
- R Heeks
- R Hirschheim
- R Sabherwal
- R Schmidt
- RR Nelson
- S Alter
- S Alter
- S Alter
- S Bruque
- S Clegg
- S Devaraj
- S Laumer
- S Laumer
- S Madon
- S Petter
- S Petter
- S Sherer
- SC Srivastava
- SC Srivastava
- SC Srivastava
- SC Srivastava
- SC Srivastava
- SC Srivastava
- SC Srivastava
- SC Srivastava
- Shirish C. Srivastava
- Sven Laumer
- T Barker
- T Klaus
- TB Lawrence
- TSH Teo
- U Kulkarni
- V McKinney
- W Al-Ahmad
- W Bussen
- WH DeLone
- WJ Orlikowski
- WJ Orlikowski
- YK Dwivedi
- YK Dwivedi
- YK Dwivedi
- Yogesh K. Dwivedi
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
The final publication is available at Springer via http://dx.doi.org/10.1007/s10796-014-9500-yInformation systems success and failure are among the most prominent streams in IS research. Explanations of why some IS fulfill their expectations, whereas others fail, are complex and multi-factorial. Despite the efforts to understand the underlying factors, the IS failure rate remains stubbornly high. A Panel session was held at the IFIP Working Group 8.6 conference in Bangalore in 2013 which forms the subject of this Special Issue. Its aim was to reflect on the need for new perspectives and research directions, to provide insights and further guidance for managers on factors enabling IS success and avoiding IS failure. Several key issues emerged, such as the need to study problems from multiple perspectives, to move beyond narrow considerations of the IT artifact, and to venture into underexplored organizational contexts, such as the public sector. © 2014 Springer Science+Business Media New York
Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- 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
- Aliev M
- 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
- Alvarez Piqueras D
- 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
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya S Tapia
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
- 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 Pozo
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Bakker PJ
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee Sw
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barkeloo JT
- Barklow T
- Barlow N
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- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
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- Barreiro Guimaraes da Costa J
- Barreiro F
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- Barton AE
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- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
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- Beddall A
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- Bednyakov VA
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- Behera A
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- Benary O
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- Berge D
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- Bergsten LJ
- Beringer J
- Berlendis S
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- Bernlochner FU
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- Berta P
- Bertella C
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- Bertsche C
- Besjes GJ
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- Bingul A
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- Bisanz T
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- Bjergaard DM
- Black JE
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- Bullock D
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- Burgard CD
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- Burmeister I
- Burr JTP
- Buschmann E
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund O Bessidskaia
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- Cabrera Urban S
- Caforio D
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- Cairo VMM
- Cakir I Turk
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- Calafiura P
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- Calderini G
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- Caloba LP
- Calvente Lopez S
- Calvet D
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- Camincher C
- Campana S
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- Campoverde A
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- Cantero J
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- Caprini I
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- Capua M
- Carbone RM
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- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
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- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo LR Flores
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
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- Ceradini F
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- Chekulaev SV
- Chelkov GA
- Chelstowska MA
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- Cheplakov A
- Cheremushkina E
- Cheu E
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- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
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- Christodoulou V
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- Collaboration ATLAS
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- Zhemchugov A
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- 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 τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-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 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ 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
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armbruster AJ
- Armitage LJ
- Armstrong A
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- Arnold H
- Arratia M
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- Artamonov A
- Artoni G
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- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlas Collaboration
- Atlay NB
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- Baca MJ
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- Barranco Navarro L
- Barreiro Guimarães Da Costa J
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- Black JE
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- Bloch I
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- Blumenschein U
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- Zhemchugov A
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- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
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- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković 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 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ 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 57.0−5.9 +6.0 (stat.) −3.3 +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
Measurement of differential cross sections and W + /W − cross-section ratios for W boson production in association with jets at √s =8 TeV with the ATLAS detector
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- Zalieckas J
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- Zemla A
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- Zeng Q
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- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
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- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
This paper presents a measurement of the W boson production cross section and the W + /W − cross-section ratio, both in association with jets, in proton--proton collisions at s √ =8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb −1 . Differential cross sections for events with one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles and the missing transverse momentum in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W + /W − the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proto
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
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- Acharya BS
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- 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
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- Alvarez 
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- Amadio BT
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- Yang Y
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- Yao W
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz H
- Yorita K
- Yoshihara K
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- Young CJS
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- Yue X
- Yuen SPY
- Yusuff I
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- Zacharis G
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- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
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- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zerwas D
- Zgubič M
- Zhang D
- Zhang DF
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur 
- Zwalinski L
- Ženiš T
- Živković 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 calorimeter’s performance during the years 2008–2012 using cosmic-ray muon events and proton–proton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fb−1. 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 proton–proton 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 proton–proton collisions at √s = 13 TeV
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- Aad G
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- Abdinov O
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- Abhayasinghe DK
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- Zhemchugov A
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- Zwalinski L
- 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 proton–proton 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 τ -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 fb−1
Search for pairs of highly collimated photon-jets in pp collisions at √s = 13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
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- Zhemchugov A
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- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
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- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- Zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/08/2018
- Field of study
Results of a search for the pair production of photon-jets—collimated groupings of photons—in the ATLAS detector at the Large Hadron Collider are reported. Highly collimated photon-jets can arise from the decay of new, highly boosted particles that can decay to multiple photons collimated enough to be identified in the electromagnetic calorimeter as a single, photonlike energy cluster. Data from proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 36.7 fb−1, were collected in 2015 and 2016. Candidate photon-jet pair production events are selected from those containing two reconstructed photons using a set of identification criteria much less stringent than that typically used for the selection of photons, with additional criteria applied to provide improved sensitivity to photon-jets. Narrow excesses in the reconstructed diphoton mass spectra are searched for. The observed mass spectra are consistent with the Standard Model background expectation. The results are interpreted in the context of a model containing a new, high-mass scalar particle with narrow width, X, that decays into pairs of photon-jets via new, light particles, a. Upper limits are placed on the cross section times the product of branching ratios σ×B(X→aa)×B(a→γγ)2 for 200 GeV<mX<2 TeV and for ranges of ma from a lower mass of 100 MeV up to between 2 and 10 GeV, depending upon mX. Upper limits are also placed on σ×B(X→aa)×B(a→3π0)2 for the same range of mX and for ranges of ma from a lower mass of 500 MeV up to between 2 and 10 GeV
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