183 research outputs found
Residual sleepiness after N(2)O sedation: a randomized control trial [ISRCTN88442975]
- Author
- Publication venue
- BioMed Central
- Publication date
- 01/05/2004
- Field of study
BACKGROUND: Nitrous oxide (N(2)O) provides sedation for procedures that result in constant low-intensity pain. How long do individuals remain sleepy after receiving N(2)O? We hypothesized that drug effects would be apparent for an hour or more. METHODS: This was a randomized, double blind controlled study. On three separate occasions, volunteers (N = 12) received 100% oxygen or 20% or 40% N(2)O for 30 min. Dependent measures included the multiple sleep latency test (MSLT), a Drug Effects/Liking questionnaire, visual analogue scales, and five psychomotor tests. Repeated measures analysis of variance was performed with drug and time as factors. RESULTS: During inhalation, drug effects were apparent based on the questionnaire, visual analogue scales, and psychomotor tests. Three hours after inhaling 100% oxygen or 20% N(2)O, subjects were sleepier than if they breathed 40% N(2)O. No other drug effects were apparent 1 hour after inhalation ceased. Patients did not demonstrate increased sleepiness after N(2)O inhalation. CONCLUSION: We found no evidence for increased sleepiness greater than 1 hour after N(2)O inhalation. Our study suggests that long-term effects of N(2)O are not significant
The Evolution of Compact Binary Star Systems
- Author
- A Ahmad
- A Blaauw
- A Bragaglia
- A Burrows
- A Burrows
- A Burrows
- A Büning
- A Cooray
- A Corongiu
- A Duquennoy
- A Gianninas
- A Heger
- A Kashi
- A Kusenko
- A Massevitch
- A Menon
- A Nebot Gómez-Morán
- A Noriega-Crespo
- A Noutsos
- A Palacios
- A Skumanich
- A Stroeer
- A Stroeer
- A Tornambé
- A Ulla
- A Wongwathanarat
- AA Zdziarski
- AC Fabian
- AE Rosenbush
- AG Kuranov
- AG Kuranov
- AG Lyne
- AG Lyne
- AG Lyne
- AG Massevich
- AG Massevitch
- AG Riess
- AH Prestwich
- AI Bogomazov
- AI Karakas
- AJ Farmer
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- AJ Faulkner
- AJ Loveridge
- AJ Ruiter
- AJ Ruiter
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- AL Kraus
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- AM Cherepashchuk
- AM Cherepashchuk
- AM Cherepashchuk
- AR King
- AR King
- AS Endal
- AS Oliveira
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- AV Tutukov
- AV Tutukov
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- AW Hotan
- B Külebi
- B Külebi
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paxton
- B Paxton
- B Voss
- B Wang
- B Warner
- B Warner
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- B Willems
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- D Bhattacharya
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- E Bear
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- JP Cox
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- K Nomoto
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- K Takahashi
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- KS Thorne
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- L Bildsten
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- L Chomiuk
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- L Dessart
- L Guillemot
- L Kreidberg
- L Mahy
- L Mestel
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- MA Ruderman
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- N Andersson
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- O Birnholtz
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- P Amaro-Seoane
- P Amaro-Seoane
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- P Höflich
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- P Kahabka
- P Lorén-Aguilar
- P Madau
- P Munar-Adrover
- P Podsiadlowski
- P Podsiadlowski
- P Podsiadlowski
- P Podsiadlowski
- P Rodríguez-Gil
- P Ruiz-Lapuente
- P Szypryt
- PA Crowther
- PA Crowther
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- PC Peters
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- R Pakmor
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- S Jones
- S Jones
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- S Mohamed
- S Neo
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- S Nissanke
- S Oslowski
- S Perlmutter
- S Rappaport
- S Rappaport
- S Rappaport
- S Refsdal
- S Repetto
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- S Shah
- S Shah
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- S Starrfield
- S Starrfield
- S Starrfield
- S Taubenberger
- S Toonen
- S Toonen
- S Vennes
- S Vereshchagin
- S Yu
- S Yu
- S-B Qian
- S-C Yoon
- S-C Yoon
- S-C Yoon
- S-C Yoon
- SA Colgate
- SA Sim
- SB Anderson
- SB Popov
- SC Vila
- SE Thorsett
- SE Timpano
- SE Woosley
- SE Woosley
- SE Woosley
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- SF Portegies Zwart
- SF Portegies Zwart
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- SL Larson
- SL Shapiro
- SN Shore
- SP Littlefair
- SS Kumar
- T Abel
- T Bulik
- T Dermine
- T Fragos
- T Kupfer
- T Linden
- T Linden
- T Nugis
- T Pan
- T Shahbaz
- T Wettig
- T-W Wong
- TA Prince
- TB Littenberg
- TE Woods
- TE Woods
- TE Woods
- TF Cartwright
- TJ Maccarone
- TM Tauris
- TM Tauris
- TM Tauris
- TR Marsh
- TR Marsh
- TR Marsh
- TR Marsh
- TR Marsh
- TR Marsh
- U Heber
- V Gokhale
- V Kalogera
- V Kalogera
- V Kalogera
- V Kalogera
- V Kalogera
- V Kalogera
- VA Brumberg
- VG Kornilov
- VG Kornilov
- VM Kaspi
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- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VN Mironovskii
- VS Petrov
- VV Davydov
- W Benz
- W Fong
- W Li
- W Li
- W-R Hamann
- WE Kerzendorf
- WE Kerzendorf
- WK Rose
- WM Farr
- WM Sparks
- WM Wolf
- WR Brown
- WR Brown
- X Meng
- X Wang
- X Zhang
- X-J Xu
- X-J Xu
- Y Osaki
- YA Fadeyev
- YA Fadeyev
- YB Zel’dovich
- YV Baryshev
- Z Barkat
- Z Han
- Z Han
- Z Han
- Z Han
- Z Han
- Z Kopal
- Z Li
- Z-W Liu
- ZW Liu
- ÉÉ Flanagan
- Publication venue
- 'Living Reviews'
- Publication date
- 03/01/2007
- Field of study
We review the formation and evolution of compact binary stars consisting of
white dwarfs (WDs), neutron stars (NSs), and black holes (BHs). Binary NSs and
BHs are thought to be the primary astrophysical sources of gravitational waves
(GWs) within the frequency band of ground-based detectors, while compact
binaries of WDs are important sources of GWs at lower frequencies to be covered
by space interferometers (LISA). Major uncertainties in the current
understanding of properties of NSs and BHs most relevant to the GW studies are
discussed, including the treatment of the natal kicks which compact stellar
remnants acquire during the core collapse of massive stars and the common
envelope phase of binary evolution. We discuss the coalescence rates of binary
NSs and BHs and prospects for their detections, the formation and evolution of
binary WDs and their observational manifestations. Special attention is given
to AM CVn-stars -- compact binaries in which the Roche lobe is filled by
another WD or a low-mass partially degenerate helium-star, as these stars are
thought to be the best LISA verification binary GW sources.Comment: 105 pages, 18 figure
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
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asawatavonvanich T
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Ayoub MK
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- 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
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barsov S
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertram IA
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhattacharya DS
- Bhattarai P
- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
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- Wang WX
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
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- Washbrook A
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- Weston TD
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- Whallon NL
- Wharton AM
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- White AS
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- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
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- Wingerter-Seez I
- Winkels E
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- Wittgen M
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- Wraight K
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- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
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- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
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- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
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- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
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- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
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- Zahreddine J
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- Zakharchuk N
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- Zanzi D
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- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
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- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
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- Zhou MS
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- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
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- 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
Targeted high throughput sequencing in clinical cancer Settings: formaldehyde fixed-paraffin embedded (FFPE) tumor tissues, input amount and tumor heterogeneity
- Author
- A Gnirke
- A Weise
- AW Briggs
- B Timmermann
- Berger MSL F Michael
- Bernd Timmermann
- BS Taylor
- C Greenman
- CA Macintosh
- D Aird
- DG Bostwick
- DT Okou
- DW Bell
- DW Parsons
- E Hodges
- ED Pleasance
- ED Pleasance
- G Bartsch
- Georg Bartsch
- Georg Schaefer
- GJ Porreca
- Hans Lehrach
- Helmut Klocker
- HM Wood
- Holger Sültmann
- Irmgard Verdorfer
- J Clark
- J Yu
- L Ding
- LD Wood
- M Aihara
- M Barry
- Martin Kerick
- Melanie Isau
- Michal R Schweiger
- MR Schweiger
- MR Schweiger
- N Navin
- PM Krawitz
- R Mehra
- R Mehra
- R Yatani
- Ralf Herwig
- RB Shah
- S Jones
- SB Ng
- SP Shah
- Sylvia Krobitsch
- T Shiraishi
- T Sjoblom
- TJ Albert
- TJ Ley
- W Horninger
- W Lee
- W Liu
- WA Sakr
- Z Kan
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>Massively parallel sequencing technologies have brought an enormous increase in sequencing throughput. However, these technologies need to be further improved with regard to reproducibility and applicability to clinical samples and settings.</p> <p>Methods</p> <p>Using identification of genetic variations in prostate cancer as an example we address three crucial challenges in the field of targeted re-sequencing: Small nucleotide variation (SNV) detection in samples of formalin-fixed paraffin embedded (FFPE) tissue material, minimal amount of input sample and sampling in view of tissue heterogeneity.</p> <p>Results</p> <p>We show that FFPE tissue material can supplement for fresh frozen tissues for the detection of SNVs and that solution-based enrichment experiments can be accomplished with small amounts of DNA with only minimal effects on enrichment uniformity and data variance.</p> <p>Finally, we address the question whether the heterogeneity of a tumor is reflected by different genetic alterations, e.g. different foci of a tumor display different genomic patterns. We show that the tumor heterogeneity plays an important role for the detection of copy number variations.</p> <p>Conclusions</p> <p>The application of high throughput sequencing technologies in cancer genomics opens up a new dimension for the identification of disease mechanisms. In particular the ability to use small amounts of FFPE samples available from surgical tumor resections and histopathological examinations facilitates the collection of precious tissue materials. However, care needs to be taken in regard to the locations of the biopsies, which can have an influence on the prediction of copy number variations. Bearing these technological challenges in mind will significantly improve many large-scale sequencing studies and will - in the long term - result in a more reliable prediction of individual cancer therapies.</p
Year in review in Intensive Care Medicine 2010: III. ARDS and ALI, mechanical ventilation, noninvasive ventilation, weaning, endotracheal intubation, lung ultrasound and paediatrics
- Author
- A Beda
- A Boyer
- A Jubran
- A Jubran
- A Lyazidi
- A Perren
- A Roch
- A Sapru
- AB Benson
- AD Cornet
- Alexandre Mebazaa
- AW Reske
- B Cabello
- B Clouzeau
- B Peeters
- B Walter
- C Chrysostomou
- C Dupuis
- C Karagiannidis
- C Milesi
- D Luca De
- D Macrae
- D Vlasselaers
- Daniel De Backer
- DG Tingay
- Duncan Macrae
- E Kondili
- ED Wildschut
- ED Wildschut
- Elie Azoulay
- F Remérand
- G Via
- GA Iotti
- Giorgio Conti
- Giuseppe Citerio
- Goran Hedenstierna
- H Prigent
- Haibo Zhang
- Herwig Gerlach
- HR Carlisle
- J Lopez-Herce
- J Phua
- J Rapoport
- JA Farias
- JA Tan
- Jan Wernerman
- JC Ejike
- JC Preiser
- Jean Chastre
- Jean-Charles Preiser
- Jerôme Pugin
- JJ Zimmerman
- JM Iglesias
- JM Kaplan
- JM Tadié
- Jordi Mancebo
- JP Kress
- K Sarafidis
- KR Plumpton
- L Blanch
- L Gattinoni
- L Vignaux
- LD Straney
- LM Heunks
- LN Segal
- M Fartoukh
- M González
- M Katayama
- M Rocco
- M Younes
- Marc Bonten
- Massimo Antonelli
- Michael Joannidis
- N Fathali
- NF O’Brien
- P Tissieres
- PC Garcia
- PE Cogo
- R Carrai
- R Costa
- R Giraud
- RS Agbeko
- S Isgrò
- S Jaber
- S Leteurtre
- S Naghib
- S Sud
- Salvatore M. Maggiore
- SD Mentzelopoulos
- SL Jan
- SM Chapman
- T Jack
- T Schaible
- U Lucangelo
- UG Kyle
- W Pollock
- Y Skrobik
- Z Szkulmowski
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2011
- Field of study
SCOPUS: re.jinfo:eu-repo/semantics/publishe
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek 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
- Alexandre D
- 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
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- 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
- Aparisi Pozo JA
- Aperio Bella L
- Arabidze G
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Ayoub MK
- Azoulay AM
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Bakshi Gupta D
- Balaji S
- 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-S
- Barkeloo J
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- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimarães da Costa J
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- Blazek T
- Bloch I
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- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
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- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
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- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Borecka-Bielska HM
- Borisov A
- Borissov G
- Bortfeldt J
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- Bouhova-Thacker EV
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- Breaden Madden WD
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- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brost E
- Broughton JH
- Bruckman de Renstrom PA
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- Bruni A
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- Brunt BH
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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
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- Burghgrave B
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- Burmeister I
- Burr JTP
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- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
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- Buttinger W
- Buzatu A
- Buzykaev AR
- Bührer F
- Büscher V
- Cabras G
- Cabrera Urbán S
- Caforio D
- Cai H
- Cairo VMM
- 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
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Cameron D
- Caminal Armadans R
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Cano Bret M
- Cantero J
- Cao T
- Cao Y
- Capeans Garrido MDM
- Caprini I
- Caprini M
- Capua M
- Carbone RM
- Cardarelli R
- Cardillo FC
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carrá S
- Carter JWS
- Casadei D
- Casado MP
- Casha AF
- 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
- Ceradini F
- Cerda Alberich L
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chafaq A
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- Chan SK
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- Chan WY
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- Chargeishvili B
- Charlton DG
- Chau CC
- Chavez Barajas CA
- Che S
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- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen B
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- Chen CH
- Chen H
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- Chen SJ
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- Cheng HJ
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- Cheremushkina E
- Cherkaoui El Moursli R
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- Chevalier L
- Chevalérias TJA
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- Chiarelli G
- Chiodini G
- Chisholm AS
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- Chiu I
- Chiu YH
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- Christodoulou V
- Chu MC
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
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- Cindro V
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- Conventi F
- Cooper-Sarkar AM
- Cormier F
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- Corrigan EE
- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
- Costanza F
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- Cottin G
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- Crawley SJ
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- Cueto A
- Cuhadar Donszelmann T
- Cukierman AR
- Czekierda S
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- Demers S
- Demichev M
- Denisov SP
- Denysiuk D
- Derendarz D
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- Derue F
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- Devesa MR
- Deviveiros PO
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- Dhaliwal S
- Di Bello FA
- Di Ciaccio A
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- Di Clemente WK
- Di Donato C
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- Duckeck G
- Ducourthial A
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- Duffield EM
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- Dunford M
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- Duschinger D
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- Dyckes G
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- Epland MB
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- Etienvre AI
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- Faisca Rodrigues Pereira RM
- Fakhrutdinov RM
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- 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
- Ziolkowski M
- 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
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 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 t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
Dynamic endothelial cell rearrangements drive developmental vessel regression
- Author
- A van Impel
- Aida P. Lima
- Anan Ragab
- Andre Rosa
- AP Meeson
- BL Roman
- Brigid L. M. Hogan
- C Xu
- CA Franco
- Claudio A. Franco
- D Stenzel
- DE Conway
- E Kochhan
- F le Noble
- Felicia M. Lopes
- Holger Gerhardt
- IB Lobov
- IB Lobov
- Ilse Geudens
- K Bentley
- L Herwig
- L Jakobsson
- LD Covassin
- Li-Kun Phng
- LK Phng
- M Ehling
- M Martin
- M Potente
- Martin L. Jones
- Miguel O. Bernabeu
- MO Bernabeu
- ND Lawson
- P Carmeliet
- P Friedl
- P Rorth
- P Vitorino
- Peter V. Coveney
- Q Chen
- RS Udan
- Russell T. Collins
- S Arima
- S Hughes
- S Rao
- T Alon
- Thomas Mathivet
- V Bryja
- Y Sato
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/04/2015
- Field of study
Patterning of functional blood vessel networks is achieved by pruning of superfluous connections. The cellular and molecular principles of vessel regression are poorly understood. Here we show that regression is mediated by dynamic and polarized migration of endothelial cells, representing anastomosis in reverse. Establishing and analyzing the first axial polarity map of all endothelial cells in a remodeling vascular network, we propose that balanced movement of cells maintains the primitive plexus under low shear conditions in a metastable dynamic state. We predict that flow-induced polarized migration of endothelial cells breaks symmetry and leads to stabilization of high flow/shear segments and regression of adjacent low flow/shear segments.status: publishe
Observation of Electroweak Production of a Same-Sign W Boson Pair in Association with Two Jets in pp Collisions root 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
- Adam L
- 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
- Akesson TPA
- Akilli E
- Akimov A
- 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 M
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambler A
- 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 A
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Arabidze G
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Ayoub MK
- Azoulay AM
- Azuelos G
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- Bloch I
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- Blumenschein U
- Blunier S
- Bobbink GJ
- Bobrovnikov VS
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- Bocci A
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- Buttinger W
- Buzatu A
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- Cabras G
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- Caforio D
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- Calace N
- Calafiura P
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- Calderini G
- Calfayan P
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- Calvet D
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- Castillo FL
- Castillo IS
- Castillo LRF
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- Chiu I
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- Christodoulou V
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- de Renstrom PAB
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- Zou R
- Zu Theenhausen HM
- Zur Nedden M
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 18/10/2019
- Field of study
This Letter presents the observation and measurement of electroweak production of a same-sign
W
boson pair in association with two jets using
36.1
fb
−
1
of proton-proton collision data recorded at a center-of-mass energy of
√
s
=
13
TeV
by the ATLAS detector at the Large Hadron Collider. The analysis is performed in the detector fiducial phase-space region, defined by the presence of two same-sign leptons, electron or muon, and at least two jets with a large invariant mass and rapidity difference. A total of 122 candidate events are observed for a background expectation of
69
±
7
events, corresponding to an observed signal significance of 6.5 standard deviations. The measured fiducial signal cross section is
σ
fid
=
2.89
+
0.51
−
0.48
(
stat
)
+
0.29
−
0.28
(
syst
)
fb
Search for excited electrons singly produced in proton–proton collisions at \sqrt{s} = 13 TeV with the ALAS experiment at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Abulaiti Y
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zibell A
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- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
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- Zorbas TG
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- Zwalinski L
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2019
- Field of study
A search for excited electrons produced in pp collisions at s√ = 13 TeV via a contact interaction qq¯→ee∗ is presented. The search uses 36.1 fb −1 of data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron into an electron and a pair of quarks ( eqq¯ ) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a W boson ( νW ) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying W boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the pp→ee∗→eeqq¯ and pp→ee∗→eνW production cross sections as a function of the excited electron mass me∗ at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter Λ of the model as a function of me∗ . For me∗<0.5 TeV , the lower bound for Λ is 11 TeV . In the special case of me∗=Λ , the values of me∗<4.8 TeV are excluded. The presented limits on Λ are more stringent than those obtained in previous searches
Dijet Resonance Search with Weak Supervision Using root S=13 TeV pp Collisions in the ATLAS Detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Acharya BS
- Achkar B
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- Alberghi GL
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- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
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- Whitmore BW
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- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
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- Yabsley B
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- Yallup DP
- Yamaguchi N
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- Yamamoto A
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- Yamazaki T
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- Yan J
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- Yao W-M
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- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yin P
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- Young C
- Young CJS
- Yu J
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- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
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- Zhang G
- Zhang J
- Zhang K
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- Zhao P
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- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhou MS
- Zhou N
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- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
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- Zhulanov V
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 25/09/2020
- Field of study
This Letter describes a search for narrowly resonant new physics using a machine-learning anomaly
detection procedure that does not rely on signal simulations for developing the analysis selection. Weakly
supervised learning is used to train classifiers directly on data to enhance potential signals. The targeted
topology is dijet events and the features used for machine learning are the masses of the two jets. The
resulting analysis is essentially a three-dimensional search A → BC, for mA ∼ OðTeVÞ, mB; mC ∼
Oð100 GeVÞ and B, C are reconstructed as large-radius jets, without paying a penalty associated with
a large trials factor in the scan of the masses of the two jets. The full run 2 ffiffi
s p ¼ 13 TeV pp collision
dataset of 139 fb−1 recorded by the ATLAS detector at the Large Hadron Collider is used for the search.
There is no significant evidence of a localized excess in the dijet invariant mass spectrum between 1.8 and
8.2 TeV. Cross-section limits for narrow-width A, B, and C particles vary with mA, mB, and mC. For
example, when mA ¼ 3 TeV and mB ≳ 200 GeV, a production cross section between 1 and 5 fb is
excluded at 95% confidence level, depending on mC. For certain masses, these limits are up to 10 times
more sensitive than those obtained by the inclusive dijet search. These results are complementary to the
dedicated searches for the case that B and C are standard model boson
- …