3,620 research outputs found
Obstructive sleep apnea after myocardial infarction.
- Author
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2010
- Field of study
Urinary endogenous sex hormone levels and the risk of postmenopausal breast cancer
- Author
- Publication venue
- Nature Publishing Group
- Publication date
- 01/01/2003
- Field of study
To assess the relation between urinary endogenous sex steroid levels and the risk of postmenopausal breast cancer, a nested caseâcohort study was conducted within a large cohort (the DOM cohort) in the Netherlands (nÂŒ9 349). Until the end of follow-up (1
January 1996), 397 postmenopausal breast cancer cases were identified and a subcohort of 424 women was then taken from all
eligible women. Women using hormones were excluded, leaving 364 breast cancer cases and 382 women in the subcohort for the
analyses. Concentrations of oestrone, oestradiol, testosterone, 5a-androstane-3a, 17b-diol and creatinine were measured in first morning urine samples, which had been stored since enrolment at -201C. A Cox proportional Hazards model was used, with Barlowâs adjustment for caseâcohort sampling, to estimate breast cancer risk in quartiles of each of the, creatinine corrected, hormone levels, the lowest quartile being the reference group. Women with higher levels of all four of the hormones were at
increased risk for postmenopausal breast cancer (highest vs lowest quartile: incidence rate ratio for oestrone (IRRoestrone=2.5, 95% CI: 1.6â3.8; IRRoestradiol=1.5, 95% CI: 1.0â2.3; IRRtestosterone=1.6, 95% CI: 1.0â2.4; IRR5a-androstane-3a, 17b-diol=1.7, 95%
CI: 1.1â2.7). In conclusion, women with higher excretion levels of both oestrogens and androgens have an increased risk of breast
cancer
Brane-World Gravity
- Author
- A Albrecht
- A Bayntun
- A Campos
- A Campos
- A Campos
- A Cardoso
- A Cardoso
- A Cardoso
- A Chamblin
- A Chamblin
- A Chamblin
- A Feinstein
- A Hebecker
- A Karch
- A Kehagias
- A Lue
- A Lue
- A Lue
- A Lue
- A Lukas
- A Lukas
- A Lukas
- A Mazumdar
- A Mennim
- A Mennim
- A Mennim
- A Neronov
- A Neronov
- A Padilla
- A PĂ©rez-Lorenzana
- AA Coley
- AA Coley
- AD Linde
- AJ Tolley
- AJ Tolley
- AJ Tolley
- AR Liddle
- AR Liddle
- AR Liddle
- AS Majumdar
- AS Majumdar
- AV Frolov
- AV Toporensky
- B Boisseau
- B Gumjudpai
- B Gumjudpai
- B Leong
- B Leong
- B Wang
- C BarcelĂł
- C BarcelĂł
- C BarcelĂł
- C BarcelĂł
- C Bruck van de
- C Bruck van de
- C Charmousis
- C Charmousis
- C Charmousis
- C Charmousis
- C Charmousis
- C Charmousis
- C Deffayet
- C Deffayet
- C Deffayet
- C Deffayet
- C Germani
- C Germani
- C Germani
- C Gordon
- C Rham de
- C Rham de
- C Rham de
- C Rham de
- C Rham de
- C Rham de
- C-M Chen
- CJ Hogan
- CP Burgess
- CP Burgess
- CP Burgess
- CP Burgess
- CP Burgess
- CS Rhodes
- D Baumann
- D Baumann
- D Baumann
- D Clancy
- D Gorbunov
- D Ida
- D Langlois
- D Langlois
- D Langlois
- D Langlois
- D Langlois
- D Langlois
- D Langlois
- D Langlois
- D Langlois
- D Langlois
- D Langlois
- D Langlois
- D Seery
- D Seery
- D Wands
- D Wands
- DJH Chung
- DJH Chung
- DS Gorbunov
- E Anderson
- E Kiritsis
- E Leeper
- E Papantonopoulos
- E Papantonopoulos
- E Papantonopoulos
- E Papantonopoulos
- E Silverstein
- ED Stewart
- EJ Copeland
- EJ Copeland
- EJ Copeland
- EV Linder
- F Arroja
- F Quevedo
- G Calcagni
- G Dvali
- G Dvali
- G Dvali
- G Gabadadze
- G Huey
- G Huey
- G Kofinas
- G Kofinas
- G Kofinas
- G Kofinas
- GA Diamandis
- GF Giudice
- GFR Ellis
- GN Felder
- GR Dvali
- GW Gibbons
- H Collins
- H Collins
- H Ishihara
- H Kodama
- H Kodama
- H Kodama
- H Kudoh
- H Stoica
- H Yoshino
- HA Bridgman
- HA Bridgman
- HL Verlinde
- I Antoniadis
- I Antoniadis
- I Giannakis
- I Giannakis
- I Navarro
- I Savonije
- I Sawicki
- IP Neupane
- J Garriga
- J Garriga
- J Garriga
- J Garriga
- J Gray
- J Hewett
- J Khoury
- J Lesgourgues
- J Martin
- J Polchinski
- J Soda
- J Soda
- J Soda
- J Sollerman
- J Vinet
- J Vinet
- J Yokoyama
- JC Long
- JD Barrow
- JD Barrow
- JD Barrow
- JD Bratt
- JE Lidsey
- JE Lidsey
- JE Lidsey
- JE Lidsey
- JE Lidsey
- JJ Blanco-Pillado
- JL Hovdebo
- JM Aguirregabiria
- JM Cline
- JP Gregory
- JP Gregory
- K Akama
- K Ichiki
- K Ichiki
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Koyama
- K Maeda
- K Maeda
- K Maeda
- KE Kunze
- KT Inoue
- L Anchordoqui
- L Guzzo
- L Mendes
- L Randall
- L Randall
- LP Chimento
- M Bastero-Gil
- M Bouhmadi-LĂłpez
- M Bruni
- M CavagliĂ
- M Dorca
- M Gogberashvili
- M Govender
- M Kolanovic
- M Kunz
- M Minamitsuji
- M Minamitsuji
- M Minamitsuji
- M Peloso
- M Peloso
- M Rinaldi
- M Sasaki
- M Visser
- M Visser
- MC Bento
- MC Bento
- MC Bento
- MG Santos
- MJ Duff
- N Agarwal
- N Arkani-Hamed
- N Dadhich
- N Dadhich
- N Deruelle
- N Deruelle
- N Deruelle
- N Deruelle
- N Deruelle
- N Kaloper
- N Kaloper
- N Kaloper
- N Kaloper
- N Sago
- NE Mavromatos
- NE Mavromatos
- NJ Nunes
- O Corradini
- O Corradini
- O Corradini
- O Seto
- P Binétruy
- P Binétruy
- P Binétruy
- P Bostock
- P Bowcock
- P Brax
- P Brax
- P Brax
- P Horava
- P Kanti
- P Kanti
- P Kraus
- PJ Steinhardt
- PR Ashcroft
- PR Ashcroft
- R Allahverdi
- R Brustein
- R Casadio
- R Casadio
- R Durrer
- R Easther
- R Emparan
- R Emparan
- R Emparan
- R Gregory
- R Guedens
- R Guedens
- R Hawkins
- R Lazkoz
- R Maartens
- R Maartens
- R Maartens
- R Maartens
- R Maartens
- R Maartens
- RA Battye
- RE Kallosh
- RH Brandenberger
- RM Wald
- RP Geroch
- RR Caldwell
- S Fujii
- S Förste
- S Hannestad
- S Kachru
- S Kachru
- S Kanno
- S Kanno
- S Kanno
- S Kobayashi
- S Mizuno
- S Mizuno
- S Mukohyama
- S Mukohyama
- S Mukohyama
- S Mukohyama
- S Mukohyama
- S Mukohyama
- S Mukohyama
- S Nojiri
- S Nojiri
- S Nojiri
- S Nojiri
- S Tsujikawa
- S Tsujikawa
- SB Giddings
- SB Giddings
- SB Giddings
- SC Davis
- SL Dubovsky
- SP Alwis de
- SP Alwis de
- SS Gubser
- SS Seahra
- SS Seahra
- SW Hawking
- SW Hawking
- T Boehm
- T Giannantonio
- T Giannantonio
- T Giannantonio
- T Hiramatsu
- T Hiramatsu
- T Hiramatsu
- T Kobayashi
- T Kobayashi
- T MultamÀki
- T Shiromizu
- T Shiromizu
- T Shiromizu
- T Shiromizu
- T Shiromizu
- T Tanaka
- T Tanaka
- T Tanaka
- T Thiemann
- T Wiseman
- T Wiseman
- U Gen
- U Gen
- V Sahni
- V Sahni
- V Sahni
- V Sahni
- VA Rubakov
- VA Rubakov
- VF Mukhanov
- W Fang
- WD Goldberger
- Y Aghababaie
- Y Aghababaie
- Y Aghababaie
- Y Himemoto
- Y Himemoto
- Y Himemoto
- Y Himemoto
- Y Sendouda
- Y Sendouda
- Y Sendouda
- Y Shtanov
- Y Shtanov
- Y Shtanov
- Y-S Song
- Z Keresztes
- Z Keresztes
- ĂĂ Flanagan
- ĂĂ Flanagan
- Publication venue
- 'Living Reviews'
- Publication date
- 01/01/2010
- Field of study
The observable universe could be a 1+3-surface (the "brane") embedded in a
1+3+\textit{d}-dimensional spacetime (the "bulk"), with Standard Model
particles and fields trapped on the brane while gravity is free to access the
bulk. At least one of the \textit{d} extra spatial dimensions could be very
large relative to the Planck scale, which lowers the fundamental gravity scale,
possibly even down to the electroweak (⌠TeV) level. This revolutionary
picture arises in the framework of recent developments in M theory. The
1+10-dimensional M theory encompasses the known 1+9-dimensional superstring
theories, and is widely considered to be a promising potential route to quantum
gravity. At low energies, gravity is localized at the brane and general
relativity is recovered, but at high energies gravity "leaks" into the bulk,
behaving in a truly higher-dimensional way. This introduces significant changes
to gravitational dynamics and perturbations, with interesting and potentially
testable implications for high-energy astrophysics, black holes, and cosmology.
Brane-world models offer a phenomenological way to test some of the novel
predictions and corrections to general relativity that are implied by M theory.
This review analyzes the geometry, dynamics and perturbations of simple
brane-world models for cosmology and astrophysics, mainly focusing on warped
5-dimensional brane-worlds based on the Randall--Sundrum models. We also cover
the simplest brane-world models in which 4-dimensional gravity on the brane is
modified at \emph{low} energies -- the 5-dimensional Dvali--Gabadadze--Porrati
models. Then we discuss co-dimension two branes in 6-dimensional models.Comment: A major update of Living Reviews in Relativity 7:7 (2004)
"Brane-World Gravity", 119 pages, 28 figures, the update contains new
material on RS perturbations, including full numerical solutions of
gravitational waves and scalar perturbations, on DGP models, and also on 6D
models. A published version in Living Reviews in Relativit
Exploring the Relationship between Semantics and Space
- Author
- A Chatterjee
- André Aleman
- B Fierro
- BH Lee
- BH Lee
- C Mohr
- C Rinaldi
- CG Gross
- D Bowers
- Daniela Smirni
- E Bisiach
- E Eger
- F Doricchi
- G Jewell
- G Vigliocco
- GD Zannino
- Giacomo Koch
- GR Fink
- GR Fink
- HB Coslett
- HO Karnath
- J Danckert
- JG Snodgrass
- K Priftis
- KM Heilman
- L Buchanan
- Lisa Cipolotti
- M Cappelletti
- M Kinsbourne
- M Kinsbourne
- M Oliveri
- M Zorzi
- M Zorzi
- Massimiliano Oliveri
- MC Rinaldi
- ME Nicholls
- MH Fischer
- MH Fischer
- MH Fischer
- MM Mesulam
- O Bjoertomt
- P Vuilleumier
- Patrizia Turriziani
- PD Siakaluk
- PM Pexman
- PW Halligan
- R Dell'Acqua
- S Dehaene
- SM Göbel
- Sonia BonnĂŹ
- T Siman-Tov
- TC Cristescu
- W Gevers
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
The asymmetric distribution of human spatial attention has been repeatedly documented in both patients and healthy controls. Biases in the distribution of attention and/or in the mental representation of space may also affect some aspects of language processing. We investigated whether biases in attention and/or mental representation of space affect semantic representations. In particular, we investigated whether semantic judgments could be modulated by the location in space where the semantic information was presented and the role of the left and right parietal cortices in this task. Healthy subjects were presented with three pictures arranged horizontally (one middle and two outer pictures) of items belonging to the same semantic category. Subjects were asked to indicate the spatial position in which the semantic distance between the outer and middle pictures was smaller. Subjects systematically overestimated the semantic distance of items presented in the right side of space. We explored the neural correlates underpinning this bias using rTMS over the left and right parietal cortex. rTMS of the left parietal cortex selectively reduced this rightward bias. Our findings suggest the existence of an attentional and/or mental representational bias in semantic judgments, similar to that observed for the processing of space and numbers. Spatial manipulation of semantic material results in the activation of specialised attentional resources located in the left hemisphere
No relationship between circulating levels of sex steroids and mammographic breast density: the Prospect-EPIC cohort
- Author
- A McTiernan
- A Vermeulen
- Carla H van Gils
- Collaborative Group on Hormonal Factors in Breast Cancer
- D Albanes
- D Trichopoulos
- Diederick E Grobbee
- E Riboli
- E Riboli
- EJ Aiello
- ER Simpson
- F Clavel-Chapelon
- F Meyer
- FJ van Duijnhoven
- G Haars
- GA Greendale
- GA Greendale
- J Brisson
- J Cuzick
- JE Rossouw
- JJ Noh
- JW Byng
- JW Byng
- LK Boker
- Martijn Verheus
- MC Ocke
- MC Ocke
- NC Onland-Moret
- NF Boyd
- NF Boyd
- NF Boyd
- NR Shah
- Paulus AH van Noord
- Petra HM Peeters
- R Kaaks
- R Warren
- RM Tamimi
- RT Chlebowski
- RT Chlebowski
- S Rinaldi
- T Key
- VA McCormack
- Yvonne T van der Schouw
- Publication venue
- BioMed Central
- Publication date
- 01/01/2007
- Field of study
Infrared photovoltaic detector based on p-GeTe/n-Si heterojunction
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2020
- Field of study
GeTe is an important narrow bandgap semiconductor material and has found application in the fields of phase change storage as well as spintronics devices. However, it has not been studied for application in the field of infrared photovoltaic detectors working at room temperature. Herein, GeTe nanofilms were grown by magnetron sputtering technique and characterized to investigate its physical, electrical, and optical properties. A high-performance infrared photovoltaic detector based on GeTe/Si heterojunction with the detectivity of 8 Ă 1011 Jones at 850ânm light irradiation at room temperature was demonstrated
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
- 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
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- Akesson TPA
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- Aleksandrov IN
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- Allbrooke BMM
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- Chen X
- Chen Y-H
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- Cheng HJ
- Cheplakov A
- Cheremushkina E
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- Chevalerias TJA
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- Chiarella V
- Chiarelli G
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- Chisholm AS
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- Chow YS
- Chu MC
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- Chudoba J
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- Zheng Z
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- Zimine N
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- Zinonos Z
- Ziolkowski M
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- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fbâ1 of â s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at sâ=8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
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- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fbâ1 of protonâproton collision data at âs = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via tËâtÏË01 or tËâ bÏ˱1 âbW(â)ÏË01 , where ÏË01 (Ï˱1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of tË â tÏË01 . For a branching fraction of 100%, top squark masses in the range 270â645 GeV are excluded for ÏË01 masses below 30 GeV. For a branching fraction of 50% to either tË â tÏË01 or tË â bÏ˱1 , and assuming the Ï˱1 mass to be twice the ÏË01 mass, top squark masses in the range 250â550 GeV are excluded for ÏË01 masses below 60 GeV
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at âs = 7 TeV with the ATLAS detector
- Author
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- Dudziak F
- Duehrssen M
- Dueren M
- Duflot L
- Duguid L
- Dunford M
- Dwuznik M
- Ebke J
- Edson W
- Edwards NC
- Ehrenfeld W
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Moursli A
- El Moursli RC
- Ellert M
- Elles S
- Ellinghaus F
- Ellinghaus F
- Ellis N
- Ellis N
- Elmsheuser J
- Elmsheuser J
- Elsing M
- Elsing M
- Emeliyanov D
- Emeliyanov D
- Enari Y
- Enari Y
- Endner OC
- Endner OC
- Endo M
- Endo M
- Engelmann R
- Engelmann R
- Erdmann J
- Erdmann J
- Ereditato A
- Ereditato A
- Eriksson D
- Eriksson D
- Ernis G
- Ernis G
- Ernst J
- Ernst J
- Ernst M
- Ernst M
- Ernwein J
- Ernwein J
- Errede D
- Errede D
- Errede S
- Errede S
- Ertel E
- Ertel E
- Escalier M
- Escalier M
- Esch H
- Esch H
- Escobar C
- Escobar C
- Espinal Curull X
- Espinal Curull X
- Esposito B
- Esposito B
- Etienne F
- Etienne F
- Etienvre AI
- Etienvre AI
- Etzion E
- Etzion E
- Evans H
- Evans H
- Fabbri L
- Fabbri L
- Facini G
- Facini G
- Fajardo LSG
- Fajardo LSG
- Fakhrutdinov RM
- Fakhrutdinov RM
- Falciano S
- Falciano S
- Faltova J
- Faltova J
- Fang Y
- Fang Y
- Fanti M
- Fanti M
- Farbin A
- Farbin A
- Farilla A
- Farilla A
- Farooque T
- Farooque T
- Farrell S
- Farrell S
- Farrington SM
- Farrington SM
- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
- Fassnacht P
- Fassouliotis D
- Fassouliotis D
- Favareto A
- Favareto A
- Fayard L
- Fayard L
- Federic P
- Federic P
- Fedin OL
- Fedin OL
- Fedorko W
- Fedorko W
- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
- Feigl S
- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
- Feng H
- Fenyuk AB
- Fenyuk AB
- Fernando W
- Fernando W
- Ferrag S
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
- Ferrara V
- Ferrari A
- Ferrari A
- Ferrari P
- Ferrari P
- Ferrari R
- Ferrari R
- Ferrer A
- Ferrer A
- Ferrere D
- Ferrere D
- Ferretti C
- Ferretti C
- Fiascaris M
- Fiascaris M
- Fiedler F
- Fiedler F
- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
- Filthaut F
- Fincke-Keeler M
- Fincke-Keeler M
- Finelli KD
- Finelli KD
- Fiolhais MCN
- Fiolhais MCN
- Fiorini L
- Fiorini L
- Firan A
- Firan A
- Fischer J
- Fischer J
- Fisher MJ
- Fisher MJ
- Fitzgerald EA
- Fitzgerald EA
- Flechl M
- Flechl M
- Fleck I
- Fleck I
- Fleischmann P
- Fleischmann P
- Fleischmann S
- Fleischmann S
- Fletcher G
- Fletcher G
- Fletcher GT
- Fletcher GT
- Flick T
- Flick T
- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
- Flowerdew MJ
- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
- Fortin D
- Fournier D
- Fournier D
- Fox H
- Fox H
- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
- Franchino S
- Francis D
- Francis D
- Franklin M
- Franklin M
- Franz S
- Franz S
- Fraternali M
- Fraternali M
- Fratin S
- Fratina S
- French ST
- French ST
- Friedrich C
- Friedrich C
- Friedrich F
- Friedrich F
- Froidevaux D
- Froidevaux D
- Frost JA
- Frost JA
- Fukunaga C
- Fukunaga C
- Fulsom BG
- Fulsom BG
- Fuster J
- Fuster J
- Gabaldon C
- Gabaldon C
- Gabizon O
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadatsch S
- Gadomski S
- Gadomski S
- Gagliardi G
- Gagliardi G
- Gagnon P
- Gagnon P
- Galea C
- Galea C
- Galhardo B
- Galhardo B
- Gallas EJ
- Gallas EJ
- Gallo V
- Gallo V
- Gallop BJ
- Gallop BJ
- Gallus P
- Gallus P
- Galster G
- Galster G
- Gan KK
- Gan KK
- Gandrajula RP
- Gandrajula RP
- Gao J
- Gao YS
- Gao YS
- Gaob J
- Garberson F
- Garberson F
- Garcia Navarro JE
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia C
- Garcia JAB
- Garcia-Sciveres M
- Garcia-Sciveres M
- Gardner RW
- Gardner RW
- Garelli N
- Garelli N
- Garonne V
- Garonne V
- Garrido MDMC
- Gatti C
- Gatti C
- Gaudio G
- Gaudio G
- Gaur B
- Gaur B
- Gauthier L
- Gauthier L
- Gauzzi P
- Gauzzi P
- Gavrilenko IL
- Gavrilenko IL
- Gay C
- Gay C
- Gaycken G
- Gaycken G
- Gazis EN
- Gazis EN
- Ge P
- Ge P
- Gecse Z
- Gecse Z
- Gee CNP
- Gee CNP
- Geerts DAA
- Geerts DAA
- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
- Gellerstedt K
- Gemme C
- Gemme C
- Gemmell A
- Gemmell A
- Genest MH
- Genest MH
- Gentile S
- Gentile S
- George M
- George M
- George S
- George S
- Gerbaudo D
- Gerbaudo D
- Gershon A
- Gershon A
- Ghazlane H
- Ghazlane H
- Ghodbane N
- Ghodbane N
- Giacobbe B
- Giacobbe B
- Giagu S
- Giagu S
- Giangiobbe V
- Giangiobbe V
- Giannetti P
- Giannetti P
- Gianotti F
- Gianotti F
- Gibbard B
- Gibbard B
- Gibson SM
- Gibson SM
- Gilchriese M
- Gilchriese M
- Gillam TPS
- Gillam TPS
- Gillberg D
- Gillberg D
- Gillman AR
- Gillman AR
- Gingrich DM
- Gingrich M
- Giokaris N
- Giokaris N
- Giordani MP
- Giordani MP
- Giordano R
- Giordano R
- Giorgi FM
- Giorgi FM
- Giraud PF
- Giraud PF
- Giugni D
- Giugni D
- Giuliani C
- Giuliani C
- Giunta M
- Giunta M
- Gjelsten BK
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- Gkialas I
- Gkialas I
- Gladilin LK
- Gladilin LK
- Glasman C
- Glasman C
- Glatzer J
- Glatzer J
- Glazov A
- Glazov A
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- Goddard JR
- Godfrey J
- Godfrey J
- Godlewski J
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- Goeringer C
- Goeringer C
- Goessling C
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- Goldfarb S
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- Golubkov D
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- Gonalo R
- Goncalo R
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- Gonzalez Parra G
- Gonzalez Parra G
- Gonzalez BA
- Gonzalez-Sevilla S
- Gonzalez-Sevilla S
- Goossens L
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- Gorbounov PA
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- Gordon HA
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- Gorelov I
- Gorelov I
- Gorini B
- Gorini B
- Gorini E
- Gorini E
- Gorisek A
- Gorisek A
- Gornicki E
- Gornicki E
- Goshaw AT
- Goshaw AT
- Gostkin MI
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- Gouighri M
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- Goujdami D
- Goujdami D
- Goulette MP
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- Goussiou AG
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- Goy C
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- Gozpinar S
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- Grabas HMX
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- Graber L
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- Grafstroem P
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- Gramling J
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- Gramstad E
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- Grancagnolo F
- Grancagnolo S
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- Grancagnoloa F
- Grassi V
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- Gratchev V
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- Gray HM
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- Graziani E
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- Grebenyuk OG
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- Greenwood ZD
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- Gregersen K
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- Gregor IM
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- Grenier P
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- Griffiths J
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- Grillo AA
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- Grimm K
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- Grinstein S
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- Grishkevich YV
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- Griso SP
- Grivaz J-F
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- Grohs JP
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- Grohsjean A
- Gross AGE
- Gross E
- Grosse-Knetter J
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- Grossi GC
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- Groth-Jensen J
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- Grout ZJ
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- Grybel K
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- Guan L
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- Guescini F
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- Guest D
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- Gueta O
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- Guicheney C
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- Guido E
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- Gul U
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- Gunther J
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- Guo J
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- Gutierrez P
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- Gutschow C
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- Guttman N
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- Guyot C
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- Gwenlan C
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- Gwilliam CB
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- Haas A
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- Haddad N
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- Haefner P
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- Hajduk Z
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- Hanninger GN
- Hansen JB
- Hansen JD
- Hansen PH
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- Hard AS
- Harenberg T
- Harkusha S
- Harper D
- Harrington RD
- Harris OM
- Harrison PF
- Hartjes F
- Harvey A
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- Hasegawa Y
- Hassani S
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- Hawkings RJ
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- Haywood SJ
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- Henderson RCW
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- Hernandez Jimenez Y
- Hernandez DP
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- Herrera CM
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- Ideal E
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- Igonkina O
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- Ikegami Y
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- Kotov VM
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- Kowalski TZ
- Kozanecki W
- Kozhin AS
- Kral V
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- Laplace S
- Lapoire C
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- Le Dortz O
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- Luehring F
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- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of âs = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentreâofâmassframeisusedtosuppressthelargemultiâjetbackground.ThecrossâsectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
- Author
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- Zaidan R
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- Zambito S
- Zanello L
- Zanzi D
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- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
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- Zerwas D
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- Zhemchugov A
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- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
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