90 research outputs found
Non-Anatomic Proximal Realignment for Recurrent Patellar Dislocation Does Not Sufficiently Prevent Redislocation
- Author
- Abraham E
- Amis AA
- Arendt EA
- Balcarek P
- Bauer FC
- Bicos J
- Chrisman OD
- Colvin AC
- Davis DK
- Deie M
- Dejour H
- Fithian DC
- Frosch S
- Hughston JC
- Insall J
- Insall J
- Jan Schmitt
- Julia Seibold
- Juliusson R
- Karl Schüttler
- Kujala UM
- Madigan R
- Maenpaa H
- Markus D Schofer
- Markus Geßlein
- Nomura E
- Nomura E
- Ostermeier S
- Ostermeier S
- Sallay PI
- Scuderi G
- Sillanpaa PJ
- Susanne Fuchs-Winkelmann
- Tegner Y
- Thomas J Heyse
- Turgay Efe
- White BJ
- Zeichen J
- Publication venue
- Bentham Open
- Publication date
- 14/02/2013
- Field of study
Several operative techniques have been described for recurrent patellar dislocation. Clinical results vary depending on the procedure and indication. The present study aimed to evaluate the clinical outcome of Insall’s proximal realignment for recurrent patellar dislocation at mid-term follow-up. Forty-five patients were reviewed with a mean follow-up period of 49 months after having undergone Insall’s procedure. Outcome measures included reports of redislocations, complications, patient-reported outcome scores (Kujala, Tegner activity scale) and subjective assessment. No statistically significant improvements (p < 0.05) in patient-reported outcome measures were noted. Sixteen patients (35%) had poor to fair results using the Kujala score. Subjective assessment revealed that 12 patients (27%) were dissatisfied with the outcome of their surgery and would not undergo the same procedure. Ten patients (22%) had suffered from redislocation at the latest follow-up. In 4 cases (9%), intra-articular knee hematoma occurred which required arthroscopic intervention. The overall mid-term outcome of the present study shows low patient satisfaction. Non-anatomic realignment for recurrent patellar dislocation does not adequately prevent redislocation
Purification and Structural Characterization of Siderophore (Corynebactin) from Corynebacterium diphtheriae
- Author
- A Schafer
- A Thieken
- AM Albrecht-Gary
- Amy E. Krafft
- CA Kunkle
- CF Bell
- Colin T. Mant
- D Lynch
- D Marion
- DA Miller
- David N. M. Jones
- DM Oram
- EA Dertz
- F Delaglio
- FC Beasley
- G Bodenhausen
- G Winkelmann
- G Winkelmann
- GL Challis
- H Boukhalfa
- H Budzikiewicz
- H Budzikiewicz
- H Drechsel
- H Drechsel
- J Cheung
- J Kalinowski
- J Meiwes
- JJ May
- JL Cotton
- JL Markley
- Jon C. Haller
- K Muller
- KN Raymond
- L Arnow
- L Muller
- LM Russell
- LM Russell
- LM Russell
- M Ikeda
- M Munzinger
- M Rance
- Mark W. Duncan
- MJ Smith
- Randall K. Holmes
- Robert S. Hodges
- Roy Martin Roop II
- S Konetschny-Rapp
- Sheryl Zajdowicz
- SL Zajdowicz
- Steve W. Hunsucker
- T Franza
- TD Goddard
- TJ Brickman
- TZ Csaky
- U Piantini
- VJ Freeman
- WH Park
- WP Aue
- WR Harris
- Publication venue
- Public Library of Science
- Publication date
- 13/04/2012
- Field of study
During infection, Corynebacterium diphtheriae must compete with host iron-sequestering mechanisms for iron. C. diphtheriae can acquire iron by a siderophore-dependent iron-uptake pathway, by uptake and degradation of heme, or both. Previous studies showed that production of siderophore (corynebactin) by C. diphtheriae is repressed under high-iron growth conditions by the iron-activated diphtheria toxin repressor (DtxR) and that partially purified corynebactin fails to react in chemical assays for catecholate or hydroxamate compounds. In this study, we purified corynebactin from supernatants of low-iron cultures of the siderophore-overproducing, DtxR-negative mutant strain C. diphtheriae C7(β) ΔdtxR by sequential anion-exchange chromatography on AG1-X2 and Source 15Q resins, followed by reverse-phase high-performance liquid chromatography (RP-HPLC) on Zorbax C8 resin. The Chrome Azurol S (CAS) chemical assay for siderophores was used to detect and measure corynebactin during purification, and the biological activity of purified corynebactin was shown by its ability to promote growth and iron uptake in siderophore-deficient mutant strains of C. diphtheriae under iron-limiting conditions. Mass spectrometry and NMR analysis demonstrated that corynebactin has a novel structure, consisting of a central lysine residue linked through its α- and ε- amino groups by amide bonds to the terminal carboxyl groups of two different citrate residues. Corynebactin from C. diphtheriae is structurally related to staphyloferrin A from Staphylococcus aureus and rhizoferrin from Rhizopus microsporus in which d-ornithine or 1,4-diaminobutane, respectively, replaces the central lysine residue that is present in corynebactin
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- 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
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aperio Bella L
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce AT
- Arfaoui S
- Arguin JF
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astbury A
- Atkinson M
- ATLAS Collaboration The
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Backus Mayes J
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
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- Barnett RM
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- Barreiro Guimarães da Costa J
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- Beddall A
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- Bednyakov VA
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- Beemster LJ
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- Benitez Garcia JA
- Benjamin DP
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- Bensinger JR
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- Bobbink GJ
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- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) 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<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
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- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
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- Yu JM
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- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
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- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- 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 √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,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
Measurement of b hadron lifetimes in exclusive decays containing a J/psi in p-pbar collisions at sqrt(s)=1.96TeV
- Author
- Aaltonen T
- Gonzalez BA
- Amerio S
- Amidei D
- Anastassov A
- Annovi A
- Antos J
- Apollinari G
- Appel JA
- Apresyan A
- Arisawa T
- Artikov A
- Asaadi J
- Ashmanskas W
- Auerbach B
- Aurisano A
- Azfar F
- Badgett W
- Barbaro-Galtieri A
- Barnes VE
- Barnett BA
- Barria P
- Bartos P
- Bauce M
- Bauer G
- Bedeschi F
- Beecher D
- Behari S
- Bellettini G
- Bellinger J
- Benjamin D
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- Bisello D
- Bizjak I
- Bland KR
- Blocker C
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- Fang HC
- Farrington S
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- Summerscales TZ
- Sung M
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- Sutton PJ
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- Tokmakov KV
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- Vallisneri M
- van den Brand JFJ
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- van der Sluys MV
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- Yamamoto H
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- Zucker ME
- Zweizig J
- Publication venue
- Publication date
- 01/12/2010
- Field of study
We report on a measurement of b-hadron lifetimes in the fully reconstructed
decay modes B^+ -->J/Psi K+, B^0 --> J/Psi K*, B^0 --> J/Psi Ks, and Lambda_b
--> J/Psi Lambda using data corresponding to an integrated luminosity of 4.3
fb−1, collected by the CDF II detector at the Fermilab Tevatron. The
measured lifetimes are τB^+ = 1.639±0.009(stat)±0.009(syst) ps, τB^0 = 1.507±0.010(stat)±0.008(syst) ps and τLambda_b = 1.537±0.045(stat)±0.014(syst) ps. The lifetime ratios are τB^+/τB^0 = 1.088±0.009(stat)±0.004(syst) and τLambda_b/τB^0 = 1.020±0.030(stat)±0.008(syst). These are the most precise determinations
of these quantities from a single experiment.Comment: revised version. accepted for PRL publicatio
Measurement of ZZ production in leptonic final states at {\surd}s of 1.96 TeV at CDF
- Author
- Aaltonen T.
- Alvarez Gonzalez B.
- Amerio S.
- Amidei D.
- Anastassov A.
- Annovi A.
- Antos J.
- Apollinari G.
- Appel J. A.
- Aptekar RL
- Arisawa T.
- Artikov A.
- Asaadi J.
- Ashmanskas W.
- Auerbach B.
- Aurisano A.
- Azfar F.
- Badgett W.
- Bae T.
- Barbaro-Galtieri A.
- Barnes V. E.
- Barnett B. A.
- Barria P.
- Bartos P.
- Bauce M.
- Bedeschi F.
- Behari S.
- Bellettini G.
- Bellinger J.
- Benjamin D.
- Beretvas A.
- Bhatti A.
- Bisello D.
- Bizjak I.
- Bland K. R.
- Blumenfeld B.
- Bocci A.
- Bodek A.
- Bortoletto D.
- Boudreau J.
- Boveia A.
- Boynton WV
- Briggs MS
- Brigliadori L.
- Bromberg C.
- Brucken E.
- Budagov J.
- Budd H. S.
- Burkett K.
- Busetto G.
- Bussey P.
- Buzatu A.
- Calamba A.
- Calancha C.
- Camarda S.
- Campanelli M.
- Campbell M.
- Canelli F.
- Carls B.
- Carlsmith D.
- Carosi R.
- Carrillo S.
- Carron S.
- Casal B.
- Casarsa M.
- Castro A.
- Catastini P.
- Cauz D.
- Cavaliere V.
- Cavalli-Sforza M.
- Cerri A.
- Cerrito L.
- Chen Y. C.
- Chertok M.
- Chiarelli G.
- Chlachidze G.
- Chlebana F.
- Cho K.
- Chokheli D.
- Chung W. H.
- Chung Y. S.
- Ciocci M. A.
- Clark A.
- Clarke C.
- Cline TL
- Compostella G.
- Connaughton V
- Convery M. E.
- Conway J.
- Corbo M.
- Cordelli M.
- Cox C. A.
- Cox D. J.
- Crescioli F.
- Cuevas J.
- Culbertson R.
- d'Ascenzo N.
- d'Errico M.
- D'Onofrio M.
- da Costa J. Guimaraes
- Dagenhart D.
- Datta M.
- de Barbaro P.
- Dell'Orso M.
- Demortier L.
- Deninno M.
- Devoto F.
- Di Canto A.
- Di Ruzza B.
- Dittmann J. R.
- Donati S
- Dong P.
- Dorigo M.
- Dorigo T.
- Ebina K.
- Elagin A.
- Eppig A.
- Erbacher R.
- Errede S.
- Ershaidat N.
- Eusebi R.
- Farrington S.
- Feindt M.
- Fernandez J. P.
- Fernandez P. Movilla
- Field R.
- Flanagan G.
- Forrest R.
- Frank M. J.
- Franklin M.
- Frederiks DD
- Freeman J. C.
- Funakoshi Y.
- Furic I.
- Gallinaro M.
- Garcia J. E.
- Garfinkel A. F.
- Garosi P.
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- Zucchelli S.chelli S.
- Zucker ME
- Zweizig J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/12/2011
- Field of study
In this paper we present a precise measurement of the total ZZ production
cross section in pp collisions at {\surd}s= 1.96 TeV, using data collected with
the CDF II detector corresponding to an integrated luminosity of approximately
6 fb-1. The result is obtained by combining separate measurements in the
four-charged (lll'l'), and two-charged-lepton and two-neutral-lepton (llvv)
decay modes of the Z. The combined measured cross section for pp {\to} ZZ is
1.64^(+0.44)_(-0.38) pb. This is the most precise measurement of the ZZ
production cross section in 1.96 TeV pp collisions to date.Comment: submitted to Phys. Rev. Let
Measurements of normalized differential cross sections for tt̄ production in pp collisions at √(s)=7 TeV using the ATLAS detector
- Author
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- Yang Y
- Yanush S
- Yao L
- Yao W-M
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- 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
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
Measurements of normalized differential cross sections for top-quark pair production are presented as a function of the top-quark transverse momentum, and of the mass, transverse momentum, and rapidity of the t¯t system, in proton–proton collisions at a center-of-mass energy of √s=7 TeV. The data set corresponds to an integrated luminosity of 4.6 fb−1, recorded in 2011 with the ATLAS detector at the CERN Large Hadron Collider. Events are selected in the lepton+jets channel, requiring exactly one lepton and at least four jets with at least one of the jets tagged as originating from a b-quark. The measured spectra are corrected for detector efficiency and resolution effects and are compared to several Monte Carlo simulations and theory calculations. The results are in fair agreement with the predictions in a wide kinematic range. Nevertheless, data distributions are softer than predicted for higher values of the mass of the t¯t system and of the top-quark transverse momentum. The measurements can also discriminate among different sets of parton distribution functions
Antiinflammatory Therapy with Canakinumab for Atherosclerotic Disease
- Author
- A Abbate
- A Abhyankar
- A Adams
- A Agafina
- A Akyea-Djamson
- A Alan
- A Alfieri
- A Alfrey
- A Alvarisqueta
- A Amos
- A Anadiotis
- A Anneveldt
- A Antolick
- A Arthur
- A Aslam
- Abaci F
- Abdullakutty J
- Abhaichand R
- Abib E Jr
- Aboufakher R
- Abrantes J
- Abreu M
- Abulencia K
- Acampora D
- Acampora M
- Accini Mendoza Jl
- Aceto L
- Acevedo B
- Acevedo L
- Acheatel R
- Actis Mv
- Adams M
- Adjic Nc
- Affaki Gs
- Agarwal Dk
- Aggarwal Rk
- Agosta Gf
- Aguilar M
- Aguilar M
- Ahire N
- Ahmad I
- Ahmed Sh
- Ahn Y
- Aish B
- Aiub F
- Aiub J
- Ajax K
- Ajioka M
- Akai Y
- Akatova E
- Akrap B
- Al Joundi T
- Al-Khalili F
- Albisu J
- Alcalde Jm
- Alcide P
- Alfonso T
- Allen J
- Alllison Dc
- Almaliky T
- Amerena J
- Andersen K
- Andor M
- Angelova I
- Angiolillo D
- Anita S
- Anker Sd
- Antalik L
- Antonicelli R
- Aparicio Cv
- Apel T
- Apostolovic S
- Ara M
- Aragorn L
- Arango Jl
- Araujo Fonseca M
- Ardissino D
- Arenas Leon Jl
- Arevalo S
- Argiolas G
- Arif I
- Armas E
- Aron G
- Arora S
- Asafu-Adjaye N
- Ashcom T
- Ashford M
- Ashino K
- Asim Oktay Ao
- Assarsson E
- Ata B
- Ather N
- Atieh M
- Aull L
- Avalos V
- Avdonina N
- Awasthi Ak
- Axthelm C
- Ayala M
- Ayasse D
- Ayasse M
- Azizad M
- Azize Gm
- B Becker
- Baar M
- Babu R
- Backer T
- Badea C
- Baden M
- Baehl S
- Baek C
- Baeumer A
- Bagi Es
- Bai A
- Bailey K
- Bailey S
- Bair S
- Baker A
- Baker C
- Bakhai A
- Bakker H
- Baksi A
- Baldin Mg
- Bali Hk
- Ballantyne C
- Ballmajo M
- Balode A
- Balukova E
- Bang Sa
- Banker D
- Banker K
- Baquero A
- Barbarash Ol
- Barbato E
- Barbosa E
- Barnett S
- Baron S
- Barreto M
- Barroso A
- Barroso W
- Bartkowiak A
- Bartosh L
- Bartuseviciene S
- Bashir K
- Baszak J
- Bata Ir
- Bayram E
- Beall K
- Beaudry M
- Beauregard La
- Beckett L
- Belejchak P
- Belle Isle J
- Belohlavek J
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- Bender D
- Benedetti G
- Benjamin S
- Benton J
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- Berger V
- Bergeron P
- Bergholtz T
- Bergler-Klein J
- Berk M
- Berli Ma
- Bernstein M
- Berra Fc
- Berti S
- Berulfsen A
- Bevilacqua Mt
- Bhadade S
- Bilazarian S
- Bilodeau N
- Binder A
- Binns Y
- Birdane A
- Bisne V
- Bitzer V
- Blagdon M
- Blahey M
- Blankenberg S
- Blazsek Z
- Bloch S
- Blom Kb
- Bluemel J
- Blumberg C
- Blumenthal R
- Bocanera M
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- Boivin Mc
- Bolduc H
- Boley K
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- Bolsmann C
- Boman K
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- Borrayo Na
- Boström På
- Botelho R
- Botta C
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- Bourgeois S
- Bouvy C
- Bowen L
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- Bradley A
- Brady L
- Bramlet D
- Brath H
- Braun P
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- Brickman T
- Briggs S
- Briké C
- Brodmann M
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- Brouwer M
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- Buchannan C
- Budaj A
- Budassi N
- Budkova J
- Bugan V
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- Bulashova O
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- Burke W
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- Burova N
- Burris H
- Burton C
- Burton J
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- Burtt D
- Busak L
- Busic N
- Byars W
- Bøen Rh
- C Clavier-Firmin
- C Conradie
- C Contzen
- C Cotes
- C Covert
- C Cuneo
- Caballero-Valiente B
- Cabau Jr
- Calabrese A
- Campanale Eg
- Candusso R
- Cantor W
- CANTOS Trial Group. Krum H
- Capova L
- Carabajal T
- Carr K
- Carrillo J
- Caruso G
- Casala J
- Caso P
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- Castillo J
- Castillo T
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- Chambers J
- Chamblee T
- Chang K
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- Chattin W
- Chauhan D
- Chauhan H
- Chaussé I
- Chavada J
- Chaverra I
- Chaware G
- Chee L
- Chella S
- Chen Cp
- Chen J
- Chen Mh
- Chen Y
- Chen Yc
- Chen Zc
- Cheng Jj
- Cheng S
- Cheng Sm
- Cherlin R
- Cheung D
- Chhabra A
- Chintala P
- Chiodi L
- Choi Aj
- Chou S
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- Christensen L
- Christenson S
- Chung A
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- Ciglenecki N
- Cioffi A
- Cislowski D
- Cleveland T
- Clocotan M
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- Colfer H
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- Collier D
- Collins R
- Coloma G
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- Commerford P
- Conrado Y
- Cools F
- Cornel Jh
- Corona V
- Coronel J
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- Coufalova Z
- Covell W
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- Crea F
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- Crocamo A
- Cromer M
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- Csala L
- Cucher F
- Cuentas I
- Cuervo A
- Curiac D
- Cymerman K
- Cyprian R
- Czerski T
- D'Amours Dg
- D Dash
- D Dattani
- D Denham
- D Desai
- D Desalle
- D Digangi
- D Dunn
- Da Costa F
- Da Silva A
- Da Silva D Jr
- Da Silva O Jr
- Dahlen G
- Dalseg Am
- Damron M
- Danik J
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- Dave B
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- Dawood Sy
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- De Caterina R
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- De Los Milagros Had M
- De Los Rios M
- De Rosa S
- De Vos A
- De Wolf L
- Dean J
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- Dedek V
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- Defosse C
- Degennaro N
- Dehning M
- Dela Llana A
- Delfonso F
- Delforge M
- Delgadillo T
- Dellasa M
- Dellborg M
- Dellorso M
- Demidova M
- Den Hartog F
- Denecke C
- Dengler T
- Dermitzakis A
- Deslongchamps F
- Dessalvi Cc
- Destro M
- Dettmer M
- Devasia T
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- Dhanak R
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- Diago M
- Diaz M
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- Dimitrov G
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- Dobilas V
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- Dong X
- Dormidontova G
- Dorogova I
- Dos Santos A
- Dos Santos F
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- Doughty A
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- Dovgalevskiy Y
- Dovgolis S
- Dragutksy B
- Dreese M
- Drost I
- Drouin K
- Duchesne L
- Duckert A
- Duda N
- Dudarev M
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- Dwenger E
- Dzupina A
- Dékány Jn
- E Eleuteri
- E Englmann
- Earl J
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- Ebrahim I
- Eccleston D
- Echeverria L
- Eder F
- Edgerton L
- Edillo C
- Edwards J
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- Eichinger G
- Einhorn D
- Eki Y
- El Hachem M
- El Hafi S
- Ellenbroek D
- Ellis M
- Emil B
- Endo T
- Engelen W
- Erhard M
- Erickson B
- Ervin W
- Eskridge L
- Espinosa V
- Everett Bm
- F Fedele
- F Fonseca
- F Fucci
- Facello A
- Facello M
- Faghih M
- Fail P
- Falcon D
- Fang C
- Fang Cy
- Farias E
- Fattal P
- Fawson A
- Feitosa G
- Felario Junior Ga
- Felix L
- Feng Y
- Feng Z
- Ferdinand K
- Ferkl R
- Fernandez Aa
- Ferrari V
- Ferrario M
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- Ferreira Dos Santos T
- Ferreira-Jardim A
- Fien E
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- Filho P
- Fintel D
- Firek C
- Fischer Sm
- Fisher J
- Fitilev S
- Fitz-Patrick D
- Fitzpatrick L
- Flaksa I
- Flather M
- Flezar M
- Fliesser-Goerzer E
- Flores E
- Flores E
- Flores Gs
- Flores H
- Floro T
- Foerster A
- Folkeringa Rj
- Fonseca A
- Fontaine S
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- Forgosh L
- Forker A
- Forster T
- Foster M
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- Fowler V
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- Frankenstein L
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- Freitas E
- French J
- Frivold G
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- Fu G
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- Fucili A
- Fukuike C
- Fullerton D
- Fulop P
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- Furch G
- Furuseth B
- G Gacioch
- G Gosselin
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- Goudev A
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- Gravenhorst-Muenter U
- Green E
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- Greenway F
- Grieshaber V
- Griffin S
- Grigaraviciene I
- Grigorova V
- Gros C
- Grosse A
- Grover A
- Grundtvig M
- Gudipati Rvc
- Guerrero A
- Guillinta P
- Gundala Ak
- Gupta A
- Gupta A
- Gupta M
- Gupta V
- Gutmann J
- Guzman I
- Guzman P
- Gwyn M
- Gyorgyova E
- H Haldane
- H Hansen
- H Haught
- H Hill
- Haase F
- Haege R
- Haenel T
- Hage F
- Hageman T
- Hagemann D
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- Hagiwara Y
- Haidar A
- Haider K
- Hakas J
- Haldis T
- Hall C
- Hall L
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- Halliwell Tc
- Halpern S
- Hamer Bjb
- Hamud-Socoro A
- Han B
- Han S
- Hanak P
- Hanefeld M
- Hangyal T
- Hansson A
- Hanustiakova A
- Hao Y
- Hardas S
- Hardee L
- Harrell W
- Harrington A
- Harris B
- Hartleib M
- Hartwell J
- Hasan F
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- Hasegawa K
- Hattler B
- Haughton G
- Haynes E
- Haywood A
- He Y
- He Z
- Heaney L
- Hecht J
- Heeren G
- Hegedus V
- Heider J
- Heisters J
- Henley L
- Hennig D
- Henriksson A
- Hermans K
- Hernandez E
- Hernandez I
- Hernandez M
- Hernández N
- Herrman Jp
- Herzog W
- Hess E
- Hettwer Magedanz E
- Hickey L
- Hiden C
- Hielscher S
- Higuchi T
- Higuchi Y
- Hilkert R
- Hilton T
- Himpel-Boenninghoff A
- Hinderaker P
- Hioki M
- Hirayama A
- Hiroma J
- Ho Cj
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- Hogan C
- Hollanders G
- Holmes Z
- Holoubek D
- Holscher A
- Hominal M
- Homza M
- Hong T
- Hong T
- Hoogslag Pam
- Horackova K
- Horak A
- Hornig M
- Horvat P
- Hosokawa S
- Hotchkiss D
- Houra M
- Hristova K
- Hsieh Ic
- Huang A
- Huang P
- Huang Ph
- Humbert J
- Hurtig U
- Hutchens E
- Huynh T
- Hwang Jj
- Hwang Jj
- Hyun K
- Härstedt N
- Høivik Ho
- I Ilic
- I Ivanov
- Iachini K
- Iannopollo G
- Ibarra J
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- Ibañez J
- Iby M
- Ichisawa M
- Igbokidi O
- Iijima T
- Ilahi T
- Ilic S
- Ilsley M
- Imbrognio M
- Imre Bs
- Inada T
- Inagaki M
- Indolfi C
- Infusino F
- Invitti C
- Ipp E
- Isaza D
- Istratoaie O
- Istvan Kp
- Iteld B
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- Ivan P
- Iveta H
- Izmozherova N
- J Jiang
- J Johnson
- J Johnston
- J Jose
- Jacques G
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- Jaguszewska G
- Jain A
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- Jayasinghe R
- Jefferson D
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- Jensen Ed
- Jeric M
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- Jiang T
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- Jirvankar P
- Johansen Bb
- Johansen E
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- Joshi U
- Julien Ve
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- Jure D
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- K Kaigawa
- K Katahira
- K Kiroglu
- K Kordic
- K Kostov
- Kabakchieva Vm
- Kaczmarek N
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- Kala P
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- Kalina A
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- Kamensky G
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- Kapp I
- Kara Yd
- Karakai H
- Karel I
- Karpuram M
- Karsai Xz
- Kastelein Jjp
- Kataoka M
- Katona A
- Katova T
- Kaur H
- Kawahara M
- Kawai M
- Kawasaki T
- Kawka-Urbanek T
- Kazanskay E
- Ke Y
- Keba E
- Keenan S
- Kelehan S
- Kellnerova I
- Kelly R
- Kelt T
- Kendall T
- Kereiakes D
- Khan A
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- Khariouzov A
- Khirmanov V
- Khromtsova O
- Kick J
- Kiefer R
- Kietselaer B
- Kim B
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- Kim M
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- King A
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- Kitchens D
- Klamm M
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- Klemsdal To
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- Klugherz B
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- Kobalava Z
- Kodem Dr
- Koeitti P
- Koenig W
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- Koleckar P
- Kolikova V
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- Komati S
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- Zineldine A.
- Zirlik A
- Zucchetti C
- Publication venue
- 'Massachusetts Medical Society'
- Publication date
- 01/01/2017
- Field of study
Background: Experimental and clinical data suggest that reducing inflammation without affecting lipid levels may reduce the risk of cardiovascular disease. Yet, the inflammatory hypothesis of atherothrombosis has remained unproved. Methods: We conducted a randomized, double-blind trial of canakinumab, a therapeutic monoclonal antibody targeting interleukin-1β, involving 10,061 patients with previous myocardial infarction and a high-sensitivity C-reactive protein level of 2 mg or more per liter. The trial compared three doses of canakinumab (50 mg, 150 mg, and 300 mg, administered subcutaneously every 3 months) with placebo. The primary efficacy end point was nonfatal myocardial infarction, nonfatal stroke, or cardiovascular death. RESULTS: At 48 months, the median reduction from baseline in the high-sensitivity C-reactive protein level was 26 percentage points greater in the group that received the 50-mg dose of canakinumab, 37 percentage points greater in the 150-mg group, and 41 percentage points greater in the 300-mg group than in the placebo group. Canakinumab did not reduce lipid levels from baseline. At a median follow-up of 3.7 years, the incidence rate for the primary end point was 4.50 events per 100 person-years in the placebo group, 4.11 events per 100 person-years in the 50-mg group, 3.86 events per 100 person-years in the 150-mg group, and 3.90 events per 100 person-years in the 300-mg group. The hazard ratios as compared with placebo were as follows: in the 50-mg group, 0.93 (95% confidence interval [CI], 0.80 to 1.07; P = 0.30); in the 150-mg group, 0.85 (95% CI, 0.74 to 0.98; P = 0.021); and in the 300-mg group, 0.86 (95% CI, 0.75 to 0.99; P = 0.031). The 150-mg dose, but not the other doses, met the prespecified multiplicity-adjusted threshold for statistical significance for the primary end point and the secondary end point that additionally included hospitalization for unstable angina that led to urgent revascularization (hazard ratio vs. placebo, 0.83; 95% CI, 0.73 to 0.95; P = 0.005). Canakinumab was associated with a higher incidence of fatal infection than was placebo. There was no significant difference in all-cause mortality (hazard ratio for all canakinumab doses vs. placebo, 0.94; 95% CI, 0.83 to 1.06; P = 0.31). Conclusions: Antiinflammatory therapy targeting the interleukin-1β innate immunity pathway with canakinumab at a dose of 150 mg every 3 months led to a significantly lower rate of recurrent cardiovascular events than placebo, independent of lipid-level lowering. (Funded by Novartis; CANTOS ClinicalTrials.gov number, NCT01327846.
Flavor tagged time-dependent angular analysis of the B0s → J/ψϕ decay and extraction of ΔΓs and the weak phase ϕs in ATLAS
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmad A
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
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- Zaytsev A
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- Zhang D
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- Zhemchugov A
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- Zibell A
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- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zitoun R
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2014
- Field of study
A measurement of the B0s→J/ψϕ decay parameters, updated to include flavor tagging is reported using 4.9 fb−¹ of integrated luminosity collected by the ATLAS detector from √s=7 TeV pp collisions recorded in 2011 at the LHC. The values measured for the physical parameters are
ϕs=0.12±0.25(stat)±0.05(syst) rad
ΔΓs=0.053±0.021(stat)±0.010(syst) ps−¹
Γs=0.677±0.007(stat)±0.004(syst) ps−¹
|A∥(0)|2=0.220±0.008(stat)±0.009(syst)
|A0(0)|2=0.529±0.006(stat)±0.012(syst)
δ⊥=3.89±0.47(stat)±0.11(syst) rad
where the parameter ΔΓs is constrained to be positive. The S-wave contribution was measured and found to be compatible with zero. Results for ϕs and ΔΓs are also presented as 68% and 95% likelihood contours, which show agreement with the Standard Model expectations
All-sky search for gravitational-wave bursts in the second joint LIGO-Virgo run
- Author
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We present results from a search for gravitational-wave bursts in the data
collected by the LIGO and Virgo detectors between July 7, 2009 and October 20,
2010: data are analyzed when at least two of the three LIGO-Virgo detectors are
in coincident operation, with a total observation time of 207 days. The
analysis searches for transients of duration < 1 s over the frequency band
64-5000 Hz, without other assumptions on the signal waveform, polarization,
direction or occurrence time. All identified events are consistent with the
expected accidental background. We set frequentist upper limits on the rate of
gravitational-wave bursts by combining this search with the previous LIGO-Virgo
search on the data collected between November 2005 and October 2007. The upper
limit on the rate of strong gravitational-wave bursts at the Earth is 1.3
events per year at 90% confidence. We also present upper limits on source rate
density per year and Mpc^3 for sample populations of standard-candle sources.
As in the previous joint run, typical sensitivities of the search in terms of
the root-sum-squared strain amplitude for these waveforms lie in the range 5
10^-22 Hz^-1/2 to 1 10^-20 Hz^-1/2. The combination of the two joint runs
entails the most sensitive all-sky search for generic gravitational-wave bursts
and synthesizes the results achieved by the initial generation of
interferometric detectors.Comment: 15 pages, 7 figures: data for plots and archived public version at
https://dcc.ligo.org/cgi-bin/DocDB/ShowDocument?docid=70814&version=19, see
also the public announcement at
http://www.ligo.org/science/Publication-S6BurstAllSky
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