534 research outputs found
Pre-Exposure to 50 Hz Magnetic Fields Modifies Menadione-Induced Genotoxic Effects in Human SH-SY5Y Neuroblastoma Cells
- Author
- A Cossarizza
- A Fischer-Nielsen
- A Markkanen
- A Rothfuss
- Anne Höytö
- Anu Liimatainen
- B Brocklehurst
- B Halliwell
- C Andreoli
- DJ McConkey
- G Iarmarcovai
- GD Garson
- J Juutilainen
- J Juutilainen
- J Luukkonen
- JG Robison
- JM Akudugu
- Jonne Naarala
- Jukka Juutilainen
- Jukka Luukkonen
- K Chow
- M Terradas
- ME Frazier
- Michael Volkert
- O Cantoni
- PA Jeggo
- RR Tice
- S Orrenius
- SM Bryce
- T Kumlin
- Publication venue
- Public Library of Science
- Publication date
- 23/03/2011
- Field of study
BACKGROUND: Extremely low frequency (ELF) magnetic fields (MF) are generated by power lines and various electric appliances. They have been classified as possibly carcinogenic by the International Agency for Research on Cancer, but a mechanistic explanation for carcinogenic effects is lacking. A previous study in our laboratory showed that pre-exposure to ELF MF altered cancer-relevant cellular responses (cell cycle arrest, apoptosis) to menadione-induced DNA damage, but it did not include endpoints measuring actual genetic damage. In the present study, we examined whether pre-exposure to ELF MF affects chemically induced DNA damage level, DNA repair rate, or micronucleus frequency in human SH-SY5Y neuroblastoma cells. METHODOLOGY/PRINCIPAL FINDINGS: Exposure to 50 Hz MF was conducted at 100 µT for 24 hours, followed by chemical exposure for 3 hours. The chemicals used for inducing DNA damage and subsequent micronucleus formation were menadione and methyl methanesulphonate (MMS). Pre-treatment with MF enhanced menadione-induced DNA damage, DNA repair rate, and micronucleus formation in human SH-SY5Y neuroblastoma cells. Although the results with MMS indicated similar effects, the differences were not statistically significant. No effects were observed after MF exposure alone. CONCLUSIONS: The results confirm our previous findings showing that pre-exposure to MFs as low as 100 µT alters cellular responses to menadione, and show that increased genotoxicity results from such interaction. The present findings also indicate that complementary data at several chronological points may be critical for understanding the MF effects on DNA damage, repair, and post-repair integrity of the genome
Colony Collapse Disorder: A Descriptive Study
- Author
- A Petrie
- A Stoner
- AC Martel
- AM Collins
- AP Møller
- AR Palmer
- AR Palmer
- AR Palmer
- B Leung
- B Scharlaken
- Bach Kim Nguyen
- BK Nguyen
- BP Oldroyd
- C Claudianos
- C Contzen
- C Saegerman
- CA Mullin
- Chris Mullin
- Claude Saegerman
- D vanEngelsdorp
- D vanEngelsdorp
- D vanEngelsdorp
- David R. Tarpy
- DC Somerville
- Delfinado-Baker
- Dennis vanEngelsdorp
- DI Nielsen
- Diana Cox-Foster
- DL Cox-Foster
- DL Farrar
- E Zander
- Eric Haubruge
- F Hendrickx
- FAM Tuyttens
- G DeGrandi-Hoffman
- G Palacios
- GD Friedman
- GE Cantwell
- GE Robinson
- GM Clarke
- GV Amdam
- H Shimanuki
- HR Mattila
- HR Mattila
- HR Mattila
- I Keller
- IL Dryden
- J Kralj
- J Vandesompele
- Jay D. Evans
- JD Ellis
- JD Evans
- Jeffery S. Pettis
- Jim Frazier
- JS Pettis
- JS Pettis
- JS Pettis
- Justin Brown
- KC Hymans
- KE Clarke
- L Bailey
- L Margolis
- L vanValen
- M Frazier
- M Higes
- M Higes
- Maryann Frazier
- N Desneux
- N Milani
- P Franck
- PA Parsons
- PG Gregory
- PL Bowen-Walker
- R Martín-Hernández
- R Underwood
- RA Goodman
- RC Aikin
- RC Dicker
- RF Leary
- RM Johnson
- Robyn Underwood
- RR Sagili
- RR Sagili
- SJ Lehotay
- SJ Martin
- SS Schneider
- T Rinderer
- TA Markow
- TD Koepsell
- V Trotta
- XL Yang
- Y Chen
- Y Chen
- Yanping Chen
- YP Chen
- YP Chen
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
BACKGROUND: Over the last two winters, there have been large-scale, unexplained losses of managed honey bee (Apis mellifera L.) colonies in the United States. In the absence of a known cause, this syndrome was named Colony Collapse Disorder (CCD) because the main trait was a rapid loss of adult worker bees. We initiated a descriptive epizootiological study in order to better characterize CCD and compare risk factor exposure between populations afflicted by and not afflicted by CCD. METHODS AND PRINCIPAL FINDINGS: Of 61 quantified variables (including adult bee physiology, pathogen loads, and pesticide levels), no single measure emerged as a most-likely cause of CCD. Bees in CCD colonies had higher pathogen loads and were co-infected with a greater number of pathogens than control populations, suggesting either an increased exposure to pathogens or a reduced resistance of bees toward pathogens. Levels of the synthetic acaricide coumaphos (used by beekeepers to control the parasitic mite Varroa destructor) were higher in control colonies than CCD-affected colonies. CONCLUSIONS/SIGNIFICANCE: This is the first comprehensive survey of CCD-affected bee populations that suggests CCD involves an interaction between pathogens and other stress factors. We present evidence that this condition is contagious or the result of exposure to a common risk factor. Potentially important areas for future hypothesis-driven research, including the possible legacy effect of mite parasitism and the role of honey bee resistance to pesticides, are highlighted
Asteroseismology and Interferometry
- Author
- A Baglin
- A Chelli
- A Claret
- A Domiciano de Souza
- A Domiciano de Souza
- A Domiciano de Souza
- A Domiciano de Souza
- A Grigahcène
- A Kanaan
- A Mazumdar
- A Mazumdar
- A Miglio
- A Miglio
- A Miglio
- A Moya
- A Munteanu
- A Mérand
- A Quirrenbach
- A Quirrenbach
- A Quirrenbach
- A Quirrenbach
- A Quirrenbach
- A Schwarzenberg-Czerny
- A Stankov
- A Thoul
- A Thoul
- A. Baglin
- A. Domiciano de Souza
- A. Miglio
- A. Miglio
- A. Quirrenbach
- AA Michelson
- AA Pamyatnykh
- AA Pamyatnykh
- AB Kaye
- AF Boden
- AF Boden
- AF Boden
- AF Boden
- AF Boden
- AF Boden
- AF Boden
- AG Kosovichev
- AJ Brickhill
- AJ Brickhill
- AN Ellis
- AN Tikhonov
- AR Hajian
- AS Eddington
- BF Lane
- BF Lane
- BG Castanheira
- BJ Brewer
- C Aerts
- C Aerts
- C Aerts
- C Aerts
- C Aerts
- C Aerts
- C Aerts
- C Aerts
- C Aime
- C Catala
- C Koen
- C Koen
- C Schrijvers
- C Waelkens
- C. Aerts
- C. Catala
- CA Hummel
- CA Hummel
- CA Hummel
- CA Hummel
- CA Hummel
- CA Hummel
- CJ Hansen
- CL Wolff
- CN Sabbey
- CS Jeffery
- CS Jeffery
- CS Rosenthal
- D Dravins
- D Dravins
- D Herbison-Evans
- D Heynderickx
- D Hoffleit
- D Kilkenny
- D Mozurkewich
- D Mozurkewich
- D Mékarnia
- D Pourbaix
- D Pourbaix
- D Reese
- D Reese
- D Stello
- D Ségransan
- D. Pourbaix
- D. W. Kurtz
- DB Guenther
- DB Guenther
- DB Guenther
- DE Blackwell
- DE Winget
- DE Winget
- DF Gray
- DH Berger
- DL Buzasi
- DM Peterson
- DM Peterson
- DO Gough
- DO Gough
- DO Gough
- DO Gough
- DO Gough
- DO Gough
- DO Gough
- DO Gough
- DO Gough
- DO Gough
- DO Gough
- DR Gies
- DR Xiong
- DR Xiong
- DR Xiong
- DS Leckrone
- DW Kurtz
- DW Kurtz
- DW Kurtz
- E Böhm-Vitense
- E Di Folco
- E Michel
- E Poretti
- E RodrÃguez
- EA Olivier
- EJ Kennelly
- EN Frazier
- F Bouchy
- F Carrier
- F Carrier
- F Carrier
- F Lignières
- F Malbet
- F Pérez Hernández
- F Schmitz
- F Soufi
- F Svensson
- F Thévenin
- F Thévenin
- F Thévenin
- F. Carrier
- F. Grundahl
- F. P. Pijpers
- F. Thévenin
- FJ Robinson
- FL Deubner
- FP Pijpers
- FP Pijpers
- FP Pijpers
- G Backus
- G Backus
- G Basri
- G Fontaine
- G Gonczi
- G Grec
- G Handler
- G Handler
- G Handler
- G Handler
- G Handler
- G Houdek
- G Houdek
- G Houdek
- G Houdek
- G Perrin
- G Perrin
- G Perrin
- G Perrin
- G Torres
- G van Belle
- G Walker
- G. Perrin
- GAH Walker
- GAH Walker
- GK Batchelor
- GT van Belle
- GT van Belle
- H Bruntt
- H Kjeldsen
- H Kjeldsen
- H Kjeldsen
- H Kjeldsen
- H Lamb
- H Otà Floranes
- H Robe
- H Saio
- H Saio
- H Saio
- H Saio
- H Saio
- H Shapley
- H von Zeipel
- HA McAlister
- HA McAlister
- HA McAlister
- HM Antia
- HM Dyck
- HS Leavitt
- IW Roxburgh
- IW Roxburgh
- IW Roxburgh
- IW Roxburgh
- IW Roxburgh
- IW Roxburgh
- IW Roxburgh
- IW Roxburgh
- J Andersen
- J Ballot
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Christensen-Dalsgaard
- J Daszyńska-Daszkiewicz
- J Daszyńska-Daszkiewicz
- J Daszyńska-Daszkiewicz
- J Davis
- J Davis
- J De Ridder
- J De Ridder
- J Fernandes
- J Hao
- J Lochard
- J Provost
- J Schou
- J Tomkin
- J Tomkin
- J van Neuman
- J. Christensen-Dalsgaard
- JA Benson
- JA Eisner
- JA Guzik
- JA Guzik
- JB Rice
- JC Suárez
- JD Monnier
- JD Monnier
- JD Scargle
- JE Baldwin
- JE Baldwin
- JH Telting
- JH Telting
- JH Telting
- JM Beckers
- JM Mariotti
- JM Matthews
- JN Bahcall
- JP Aufdenberg
- JP Aufdenberg
- JP Aufdenberg
- JP Cox
- JP Cox
- JP Cox
- JP Zahn
- JR Brookes
- JR North
- JR North
- JR North
- JT Armstrong
- JT Armstrong
- JT Armstrong
- JT Armstrong
- JT Armstrong
- JW Goodman
- K Ohnaka
- K Uytterhoeven
- K Uytterhoeven
- K Uytterhoeven
- K Uytterhoeven
- K Zwintz
- K. Rousselet-Perraut
- KB MacGregor
- KG Libbrecht
- L Bigot
- L Bigot
- L Bigot
- L Gizon
- L Gizon
- L Lefèvre
- L Paternò
- L. Bigot
- LA Balona
- LA Balona
- LA Balona
- LA Balona
- LA Balona
- LA Balona
- LG Henyey
- M Aizenman
- M Asplund
- M Asplund
- M Asplund
- M Ausseloos
- M Ausseloos
- M Breger
- M Breger
- M Breger
- M Breger
- M Briquet
- M Gabriel
- M Gabriel
- M Gabriel
- M Gabriel
- M Gehmeyr
- M Gehmeyr
- M Konacki
- M Marengo
- M Marti´c
- M Ollivier
- M Rieutord
- M Shao
- M Takata
- M Tassoul
- M Tassoul
- M Viskum
- M Wittkowski
- M Wittkowski
- M Wittkowski
- M Wittkowski
- M Yildiz
- M Zhao
- M. J. P. F. G. Monteiro
- M. J. Thompson
- M. S. Cunha
- MA Dupret
- MA Dupret
- MA Dupret
- MA Dupret
- MA Dupret
- MA Smith
- MA Smith
- MAC Perryman
- MC Rabello-Soares
- MH Montgomery
- MH Montgomery
- MH Montgomery
- MJ Goupil
- MJ Lighthill
- MJ Seaton
- MJ Thompson
- MJ Thompson
- MJPFG Monteiro
- MJPFG Monteiro
- MJPFG Monteiro
- MJPFG Monteiro
- MM Colavita
- MP Di Mauro
- MP Di Mauro
- MS Cunha
- MS Cunha
- MS Cunha
- MS Cunha
- MS Cunha
- MS Cunha
- MS Cunha
- MU Feuchtinger
- MW Muterspaugh
- MW Muterspaugh
- N Baker
- N Baker
- N Ohishi
- N Zwahlen
- NH Baker
- NH Baker
- NJ Balmforth
- NJ Balmforth
- O Kochukhov
- O Kochukhov
- O Lardière
- O. L. Creevey
- OL Creevey
- P Bloomfield
- P Bordé
- P Brassard
- P De Cat
- P De Cat
- P De Cat
- P De Cat
- P De Cat
- P Eggenberger
- P Goldreich
- P Goldreich
- P Kervella
- P Kervella
- P Kervella
- P Kervella
- P Kervella
- P Ledoux
- P Smeyers
- P. Eggenberger
- P. J. V. Garcia
- P. Kervella
- P. Mathias
- PA Bradley
- PA Bradley
- PA Stamford
- PB Warner
- PD Bennett
- PD Edmonds
- PE Tremblay
- PH Hauschildt
- PH Scherrer
- PR Bevington
- R Hanbury Brown
- R Hanbury Brown
- R Kuhfuß
- R Samadi
- R Samadi
- R Samadi
- R Samadi
- R Scuflaire
- R Smolec
- R Stein
- R Trampedach
- R van Boekel
- R van Boekel
- R Vio
- RA GarcÃa
- RB Leighton
- RD Watson
- RF Christy
- RF Stein
- RF Stein
- RF Stein
- RF Stein
- RF Stein
- RF Stellingwerf
- RF Stellingwerf
- RG Petrov
- RHD Townsend
- RK Ulrich
- RK Ulrich
- RK Ulrich
- RL Gilliland
- RL Kurucz
- RM Nowakowski
- RP Butler
- RR Shobbrook
- S Basu
- S Basu
- S Basu
- S Chandrasekhar
- S Frandsen
- S Frandsen
- S Hekker
- S Jackson
- S Jankov
- S Kraus
- S Leccia
- S Ragland
- S Théado
- S Théado
- S Vauclair
- S. Basu
- S. Söderhjelm
- SA Zhevakin
- SA Zhevakin
- SK Randall
- SK Randall
- SO Kepler
- ST Fletcher
- SV Berdyugina
- SV Berdyugina
- T Appourchaux
- T Chlebowski
- T. C. Teixeira
- T. M. Brown
- TA Ryabchikova
- TA ten Brummelaar
- TC Teixeira
- TH Rivinius
- TL Jr Duvall
- TL Jr Duvall
- TM Brown
- TM Brown
- TR Bedding
- TR Bedding
- TR Bedding
- TR Bedding
- TS Metcalfe
- TS Metcalfe
- TS Metcalfe
- V Antoci
- VM Canuto
- VM Canuto
- VM Canuto
- W Dziembowski
- W Unno
- W Unno
- W Zima
- W Zima
- WA Dziembowski
- WA Dziembowski
- WA Dziembowski
- WA Dziembowski
- WC Danchi
- WD Pesnell
- WG Bagnuolo
- WG Jr Bagnuolo
- WJ Chaplin
- WJ Chaplin
- WJ Chaplin
- WJ Chaplin
- WJ Chaplin
- WJ Tango
- XP Pan
- XP Pan
- Y Osaki
- Y Wu
- Å Nordlund
- Å Nordlund
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2007
- Field of study
Asteroseismology provides us with a unique opportunity to improve our
understanding of stellar structure and evolution. Recent developments,
including the first systematic studies of solar-like pulsators, have boosted
the impact of this field of research within Astrophysics and have led to a
significant increase in the size of the research community. In the present
paper we start by reviewing the basic observational and theoretical properties
of classical and solar-like pulsators and present results from some of the most
recent and outstanding studies of these stars. We centre our review on those
classes of pulsators for which interferometric studies are expected to provide
a significant input. We discuss current limitations to asteroseismic studies,
including difficulties in mode identification and in the accurate determination
of global parameters of pulsating stars, and, after a brief review of those
aspects of interferometry that are most relevant in this context, anticipate
how interferometric observations may contribute to overcome these limitations.
Moreover, we present results of recent pilot studies of pulsating stars
involving both asteroseismic and interferometric constraints and look into the
future, summarizing ongoing efforts concerning the development of future
instruments and satellite missions which are expected to have an impact in this
field of research.Comment: Version as published in The Astronomy and Astrophysics Review, Volume
14, Issue 3-4, pp. 217-36
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Beernaert K
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
- Bell KW
- Bellan P
- Bellan R
- Bellato M
- Bellinger JN
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bialkowska H
- Bian JG
- Bianchi G
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boimska B
- Boldizsar L
- Bolla G
- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
- Bondu O
- Bontenackels M
- Boos E
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bortoletto D
- Bose S
- Bose T
- Bostock F
- Botta C
- Boudoul G
- Boulahouache C
- Boumediene D
- Bourilkov D
- Boutemeur M
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breto G
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Broccolo G
- Brochero Cifuentes JA
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
- Brown RM
- Brownson E
- Brun H
- Bruno G
- Bryer AG
- Buchmann MA
- Buchmuller O
- Bunkowski K
- Bunn J
- Buontempo S
- Burgmeier A
- Burkett K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butt J
- Butz E
- Bylsma B
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Callner J
- Calvert B
- Calvo E
- Campagnari C
- Campbell A
- Camporesi T
- Capiluppi P
- Caponeri B
- Cappello G
- Cardaci M
- Carlin R
- Carlsmith D
- Carrillo Moreno S
- Carroll R
- Cartiglia N
- Carvalho W
- Casal B
- Casimiro Linares E
- Castaldi R
- Castello R
- Castilla-Valdez H
- Castro A
- Castro E
- Caudron J
- Caulfield M
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Ceballos GG
- Cepeda M
- Cerati GB
- Cerci DS
- Cerci S
- Cerizza G
- Cerminara G
- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan M
- Chang P
- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen KH
- Chen M
- Chen Y
- Chen Z
- Cherepanov V
- Chertok M
- Chetluru V
- Cheung HWK
- Chhibra SS
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Cho Y
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chou JP
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Acosta MV
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- Christiansen T
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- Clerbaux B
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- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Conetti S
- Contardo D
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- Conway J
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- Cooper SI
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- Cornelis T
- Correa Martins Junior M
- Cortezon EP
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- Costantini S
- Coughlan JA
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- Cuevas J
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- Czellar S
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- Da Costa EM
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
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- Zatserklyaniy A
- Zeinali M
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- Zeuner WD
- Zeyrek M
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- Zoeller MH
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Civinini C
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- CMS Collaboration
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- Cripps N
- Cuevas J
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- Cumalat JP
- Cuplov V
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- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Da Silva WLP
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
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- Das S
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- Daubie E
- David A
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- de Barbaro P
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- de Cassagnac RG
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- Eugster J
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
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- Aguilar-Benitez M
- Aguilo E
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- Ahmad WH
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- Vishnevskiy D
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- Vizan Garcia JM
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- Wyslouch B
- Xiao H
- Xie S
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- Yang F
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- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam N
- Adam W
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- Wyslouch B
- Xiao H
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- Yang F
- Yang M
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
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- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
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- Zhukov V
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- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta MV
- Adair A
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram J-L
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Minimally invasive, patient specific, beat-by-beat estimation of left ventricular time varying elastance.
- Author
- A Vieillard-Baron
- Antoine Pironet
- BW Smith
- C Starfinger
- Chris Pretty
- D Burkhoff
- D Burkhoff
- D Chung
- D Mozaffarian
- D Mozaffarian
- D Stevenson
- D Stevenson
- DC Angus
- E Bouvier
- E Brinke Ten
- F Jardin
- G Hasenfuss
- G Swamy
- H Fujiwara
- H Senzaki
- H Suga
- H Suga
- HB Nguyen
- J Baan
- J Tuchschmidt
- J-A Broscheit
- J-L Vincent
- J. Geoffrey Chase
- JA Revie
- JA Revie
- JE Hall
- JE Porterfield
- Joel Balmer
- K Chatterjee
- K Sagawa
- K Sunagawa
- L Zhong
- LA Pineda
- M Kastrup
- ME Weaver
- RM Lang
- RR Tuttle
- S Harvey
- S Kamoi
- Shaun Davidson
- Shun Kamoi
- SK Frazier
- T Shishido
- Thomas Desaive
- W Grossman
- Publication venue
- BioMed Central
- Publication date
- 01/01/2017
- Field of study
peer reviewedBACKGROUND: The aim of this paper was to establish a minimally invasive method for deriving the left ventricular time varying elastance (TVE) curve beat-by-beat, the monitoring of which's inter-beat evolution could add significant new data and insight to improve diagnosis and treatment. The method developed uses the clinically available inputs of aortic pressure, heart rate and baseline end-systolic volume (via echocardiography) to determine the outputs of left ventricular pressure, volume and dead space volume, and thus the TVE curve. This approach avoids directly assuming the shape of the TVE curve, allowing more effective capture of intra- and inter-patient variability. RESULTS: The resulting TVE curve was experimentally validated against the TVE curve as derived from experimentally measured left ventricular pressure and volume in animal models, a data set encompassing 46,318 heartbeats across 5 Pietrain pigs. This simulated TVE curve was able to effectively approximate the measured TVE curve, with an overall median absolute error of 11.4% and overall median signed error of -2.5%. CONCLUSIONS: The use of clinically available inputs means there is potential for real-time implementation of the method at the patient bedside. Thus the method could be used to provide additional, patient specific information on intra- and inter-beat variation in heart function
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