538 research outputs found
Cellular Radiosensitivity: How much better do we understand it?
- Author
- Agrawal A
- Ahel I
- Ahnesorg P
- Ali A
- Anderson RM
- Awa AA
- Azzam E.I.
- Bailey SM
- Bakkenist CJ
- Beamish H
- Bedford JS
- Bedford JS
- Bender MA
- Berkovich E
- Biedermann KA
- Blunt T
- Booth C
- Bosma GC
- Breslin C
- Brown GL
- Brown JM
- Buck D
- Carney JP
- Cerosaletti K
- Cerosaletti K
- Chan DW
- Chan DW
- Chapman JD
- Chen P.C.
- Clements PM
- Cornforth MN
- Cornforth MN
- Cornforth MN
- Curtis SB
- Davis ME
- de Jager M
- Deans B
- Dianor II
- Ding Q
- Dizdaroglu M
- Doil C
- El-Khamisy SF
- El-Khamisy SF
- Emmerson PT
- Falck J
- Falck J
- Foray N
- Game JC
- Gao Y
- Gatti RA
- Georgakilas AG
- Germain M
- Godthelp BC
- Goffman TE
- Goldman M
- Goldstein L
- Goodarzi AA
- Goodarzi AA
- Goodhead DT
- Grawunder U
- Gueven N
- Gueven N
- Gueven N
- Hirano M
- Ho KS
- Ho KY
- Holliday R
- Hopfner KP
- Houldsworth J
- Huen MS
- Iliakis G
- Iliakis G
- Iliakis G
- Jackson SP
- Jazayeri A
- Jeggo PA
- Jeggo PA
- Jeggo PA
- Jeggo PA
- Joiner MC
- Joiner MC
- Kankura T
- Kastan MB
- Kato TA
- Kemp LM
- Kemp LM
- Khanna KK
- Kitagawa R
- Kolas NK
- Kozlov SV
- Krueger SA
- Kurz EU
- Lavin MF
- Lavin MF
- Lehmann AR
- Li Z
- Lindahl T
- Lisker R
- Little JB
- Liu N
- Liu Y
- Lobrich M
- Lockart RZ
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- Macklis RM
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- Marples B
- Martin F. Lavin
- Maser RS
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- Mothersill C
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- Neel JV
- Nelms BE
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- Nikjoo H
- O'Driscoll M
- O'Driscoll M
- Olive PL
- Olive PL
- Otake M
- Ouyang H
- Painter RB
- Pandita TK
- Parsons PA
- Paull TT
- Paull TT
- Paull TT
- Penny Jeggo
- Peters LJ
- Potten CS
- Pourquier P
- Pourquier P
- Purdy JA
- Radford IR
- Radford JR
- Ratnayake RK
- Resnick MA
- Riballo E
- Robins HI
- Rothkamm K
- Rothkamm K
- Rothkamm K
- Royal HD
- Samson L
- Savitsky K
- Sax K
- Sedgwick RP
- Shinohara A
- Shreeram S
- Singh NP
- Spivak G
- Stamato TD
- Stamato TD
- Stewart GS
- Stewart GS
- Stewart GS
- Strzelczyk JJ
- Sun Y
- Sun Y.
- Sutherland JC
- Taccioli GE
- Takashima H
- Tapio S
- Taylor AM
- Taylor AMR
- Teoule R
- Terasima T
- Thacker J
- Thacker J
- Thacker J
- Thierry-Chef I
- Thompson LH
- Thompson LH
- Uziel T
- van den Bosch M
- van der Schans GP
- Varon R
- von Sonntag C
- Walker JR
- Wall BF
- Wallach DF
- Waltes R
- Ward IM
- Ward JF
- Ward JF
- Weemaes CMR
- Whitmore GF
- Willetts NS
- Williams RS
- Wolff S
- Wolff S
- Wolff S
- Wolff S
- Woo SY
- Wood RD
- Wykes SM
- Wyman C
- Yoshimaru H
- Yoshimoto Y
- You Z
- Zdzienicka MZ
- Zdzienicka MZ
- Zdzienicka MZ
- Zhao W
- Zhou T
- Ziv Y
- Publication venue
- 'Informa UK Limited'
- Publication date
- 03/12/2009
- Field of study
Purpose: Ionizing radiation exposure gives rise to a variety of lesions in DNA that result in genetic instability and potentially tumorigenesis or cell death. Radiation extends its effects on DNA by direct interaction or by radiolysis of H2O that generates free radicals or aqueous electrons capable of interacting with and causing indirect damage to DNA. While the various lesions arising in DNA after radiation exposure can contribute to the mutagenising effects of this agent, the potentially most damaging lesion is the DNA double strand break (DSB) that contributes to genome instability and/or cell death. Thus in many cases failure to recognise and/or repair this lesion determines the radiosensitivity status of the cell. DNA repair mechanisms including homologous recombination (HR) and non-homologous end-joining (NHEJ) have evolved to protect cells against DNA DSB. Mutations in proteins that constitute these repair pathways are characterised by radiosensitivity and genome instability. Defects in a number of these proteins also give rise to genetic disorders that feature not only genetic instability but also immunodeficiency, cancer predisposition, neurodegeneration and other pathologies.
Conclusions: In the past fifty years our understanding of the cellular response to radiation damage has advanced enormously with insight being gained from a wide range of approaches extending from more basic early studies to the sophisticated approaches used today. In this review we discuss our current understanding of the impact of radiation on the cell and the organism gained from the array of past and present studies and attempt to provide an explanation for what it is that determines the response to radiation
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
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- Zhemchugov A
- Zheng S
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- Zieminska D
- Zilka B
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- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
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- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
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- Aubert B
- Auge E
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- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
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- Bacci C
- Bach AM
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- Bachy G
- Backes M
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- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
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- Baines JT
- Baker MD
- Baker OK
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- Banfi D
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- Bardin DY
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- Barnett BM
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- Baroncelli A
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- Barr AJ
- Barreiro F
- Barrera CO
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- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
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- Beauchemin PH
- Beccherle R
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- Beddall A
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- Benjamin DP
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- Biglietti M
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- Zhemchugov A
- Zheng S
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
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- Wraight K
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- Yajima K
- Yallup DP
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- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
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- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye H
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- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
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- Yu J
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- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
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- 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
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
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- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Knowledge brokering between researchers and policymakers in Fiji to develop policies to reduce obesity: a process evaluation
- Author
- A Booth
- AD Oxman
- AD Oxman
- B Swinburn
- Boyd Swinburn
- C Almeida
- C Mitton
- Canadian Health Research Foundation
- E Waters
- Gade Waqa
- H Mavoa
- Helen Mavoa
- J Lavis
- J Lomas
- J Negin
- J Parry
- J Sallis
- J Utter
- J Utter
- J Van Kammen
- Jimaima Schultz
- JL Denis
- JN Lavis
- JN Lavis
- JN Lavis
- JN Lavis
- JN Lavis
- JN Lavis
- JP Block
- JP Lane
- KF Fotu
- L Mannheimer
- L Millar
- L Peirson
- M Dobbins
- M Dobbins
- M Dobbins
- M Meyer
- M Reddy
- Marita McCabe
- Marj Moodie
- MH Cheng
- Ministry of Health
- MJ Aarts
- ML Gagnon
- P Kremer
- Peter Kremer
- R Armstrong
- R Greenhalgh
- R Hughes
- R Hughes
- R Landry
- Republic of Fiji Islands
- RP Saunders
- RR Friedman
- S Bowen
- S Bowen
- S Curtis
- S Innvaer
- SM Jansson
- T Coyne
- T Lang
- T Lang
- T Lobstein
- United Nations
- V Ward
- W Snowdon
- Wendy Snowdon
- WHO
- World Health Organisation
- World Health Organization
- Y Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2013
- Field of study
The importance of using research evidence in decision making at the policy level has been increasingly recognized. However, knowledge brokering to engage researchers and policymakers in government and non-government organizations is challenging. This paper describes and evaluates the knowledge exchange processes employed by the Translational Research on Obesity Prevention in Communities (TROPIC) project that was conducted from July 2009 to April 2012 in Fiji. TROPIC aimed to enhance: the evidence-informed decision making skills of policy developers; and awareness and utilization of local and other obesity-related evidence to develop policies that could potentially improve the nation’s food and physical activity environments. The specific research question was: Can a knowledge brokering approach advance evidence-informed policy development to improve eating and physical activity environments in Fiji. <br /
Analysis of arterial intimal hyperplasia: review and hypothesis
- Author
- A Bálint
- A Cano
- A Daoud
- A Desmouliere
- A Kamiya
- A Kamiya
- A Kumar
- A Mennander
- A Miyagawa-Hayashino
- A Navas-Acien
- A Tejani
- A Vink
- AC Newby
- AD Callow
- AJ Demetris
- AN Sidawy
- AO Ковалевский
- AR Tall
- AS Romer
- AW Ham
- B Russell
- BC Ward
- BG Charlton
- BG Charlton
- BH Walpoth
- BH Walpoth
- BJ Ballermann
- BL Langille
- BS Crawford
- C Patterson
- C Purcell
- C Purcell
- C Velican
- C Velican
- C Velican
- C Velican
- C Velican
- C Velican
- C Velican
- C Velican
- C Velican
- C Vermot-Desroches
- C Xu
- C Yutani
- CE Head
- CF Simpson
- CL Berry
- D Czarnecka
- D Skowasch
- D Velican
- D Velican
- D Velican
- D Velican
- D Zochodne
- DE Ingber
- DG Katritsis
- E Arciniegas
- E Sho
- E Sho
- E Sho
- E Sho
- EJ Wallitt
- ER Long
- ER O'Brien
- ER O'Brien
- F Bohorquez
- F Krotz
- F Versaci
- FH Sims
- FW Booth
- FW Booth
- FW Booth
- G Bauriedel
- G Gillett
- GA Ferns
- GK Hansson
- GL Kaluza
- GR Osborn
- H Davies
- H Fox
- H Luo
- H Masuda
- H Masuda
- H Miller
- H Nanjo
- H Shirwan
- H Sun
- H Wang
- H Wolinsky
- HB Wood
- HC Stary
- HC Stary
- HC Stary
- HC Stary
- HD Dellmann
- HR Augsburger
- HS Ahn
- I Asmussen
- I Huttner
- ID Goldberg
- J Alroy
- J Damuth
- J Garcia-Fernandez
- J Goodman
- J Hirvonen
- J Klitkou
- J Koulack
- J Martin
- J Niebauer
- J Wehner
- JA Iestra
- JB Stokes
- JC Biro
- JE Fortunato
- JE French
- JE Moore Jr
- JG Geraghty
- JG van Dam
- JJ Kastelein
- JO Whyte
- JS Allan
- JS Gill
- JS Hochman
- K Dean
- K Hoshina
- K Tohda
- K Wolkoff
- K Yamamoto
- K Yamamoto
- KM Downs
- KS Thomson
- L Matturri
- LC Junqueira
- LP Gartner
- M Baron
- M Beppu
- M Bergwerff
- M Bergwerff
- M Cipolla
- M Friedman
- M Friedman
- M Fukuchi
- M Herring
- M Horsella
- M Hosono
- M Ohkubo
- M Osada
- M Sanchez
- M Schillinger
- M Shah
- M Sho
- M Subotin
- M Sunamura
- M Susser
- M Valgimigli
- M Yamauchi
- MA Costa
- MC Deng
- MC Deng
- MC Dickson
- MC Fitzgerald
- MH Freitag
- MH Ross
- MH Sayegh
- MJ Hung
- ML Bots
- ML Rose
- MM Donners
- MP Cohen
- MR Garvin
- MS Cappell
- MSY Lee
- N Anitschkow
- N Anitschkow
- N Anitschkow
- N Hafeez
- N Jensen
- N Kipshidze
- NJ Elzenga
- NJ Kusnetzowsky
- NJ Mehta
- NL Tilney
- O Jarvinen
- P Carmeliet
- P Chandrasoma
- P Libby
- P Sapienza
- P Teirstein
- PB Dobrin
- PE DiCorleto
- PF Davies
- PI Hornick
- PJ Gallagher
- PM Heidger Jr
- PM Ridker
- PS Teirstein
- PT Cagle
- PW Serruys
- R Ciubotariu
- R Cooper
- R Friedl
- R Hoerbelt
- R Khan
- R Ross
- R Sheppard
- R Thoma
- R Thoma
- R Thoma
- R Virchow
- RA Armstrong
- RG Gerrity
- RH Kardon
- RJ Boucek
- RJ de Winter
- RL Bacon
- RN Mitchell
- RP Bolande
- RY Loyaga-Rendon
- S De Servi
- S Endo
- S Glagov
- S Glagov
- S Houser
- S Inoue
- S Islam
- S Kamiya
- S Kitamoto
- S Krus
- S Lindsay
- S Obayashi
- S Oguma
- S Oguma
- S Sartore
- SE Greenwald
- SE Nissen
- SF Gilbert
- SM Mojon-Azzi
- SM Schwartz
- SP Olesen
- SP Schmidt
- SR Opie
- SS Berman
- T Asakura
- T Brand
- T Dobzhansky
- T Fukushima
- T Gloe
- T Karino
- T Karino
- T Karino
- T Karino
- T Karino
- T Takagi
- T Takahashi
- T Yoro
- TE Starzl
- TL Brown
- TM Schiele
- TN Blankenship
- TS Kuhn
- V Lange
- V Nuzzo
- V Subbotin
- V Subbotin
- VG Cin
- Vladimir M Subbotin
- VM Paralkar
- VS Sottiurai
- VS Sottiurai
- VS Sottiurai
- VS Zhdanov
- W Kuehnel
- W Maier
- W Osika
- W Rosamond
- W Schurch
- WC Aird
- WD Shapiro
- WE Boden
- WE Stehbens
- WE Stehbens
- WE Stehbens
- WE Stehbens
- WE Stehbens
- WJ Weninger
- Y Ikari
- Y Miyao
- Y Nakashima
- Publication venue
- BioMed Central
- Publication date
- 01/01/2007
- Field of study
which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Background: Despite a prodigious investment of funds, we cannot treat or prevent arteriosclerosis and restenosis, particularly its major pathology, arterial intimal hyperplasia. A cornerstone question lies behind all approaches to the disease: what causes the pathology? Hypothesis: I argue that the question itself is misplaced because it implies that intimal hyperplasia is a novel pathological phenomenon caused by new mechanisms. A simple inquiry into arterial morphology shows the opposite is true. The normal multi-layer cellular organization of the tunica intima is identical to that of diseased hyperplasia; it is the standard arterial system design in all placentals at least as large as rabbits, including humans. Formed initially as one-layer endothelium lining, this phenotype can either be maintained or differentiate into a normal multi-layer cellular lining, so striking in its resemblance to diseased hyperplasia that we have to name it "benign intimal hyperplasia". However, normal or "benign " intimal hyperplasia, although microscopically identical to pathology, is a controllable phenotype that rarely compromises blood supply. It is remarkable that each human heart has coronary arteries in which a single-layer endothelium differentiates earl
Measurement of the cross-section for b-jets produced in association with a Z boson at root s=7 TeV with the ATLAS detector ATLAS Collaboration
- Author
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- Abdallah J
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
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- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2011
- Field of study
A measurement is presented of the inclusive cross-section for b-jet production in association with a Z boson in pp collisions at a centre-of-mass energy of root s = 7 TeV. The analysis uses the data sample collected by the ATLAS experiment in 2010, corresponding to an integrated luminosity of approximately 36 pb(-1). The event selection requires a Z boson decaying into high P-T electrons or muons, and at least one b-jet, identified by its displaced vertex, with transverse momentum p(T) > 25 GeV and rapidity vertical bar y vertical bar < 2.1. After subtraction of background processes, the yield is extracted from the vertex mass distribution of the candidate b-jets. The ratio of this cross-section to the inclusive Z cross-section (the average number of b-jets per Z event) is also measured. Both results are found to be in good agreement with perturbative QCD predictions at next-to-leading order
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
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- Abusleme Hoffman AC
- Acharya BS
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- Zeng JC
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- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
- Zhang DF
- Zhang J
- Zhang J
- Zhang K
- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
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- Aakvaag E
- Abbott B
- Abeling K
- Abicht NJ
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- Zhemchugov A
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- Zimine NI
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fb−1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17−15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7−6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
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