1,326 research outputs found
EST Analysis of Ostreococcus lucimarinus, the Most Compact Eukaryotic Genome, Shows an Excess of Introns in Highly Expressed Genes
- Author
- AB Carvalho
- AE Vinogradov
- AF Pendle
- Ahmed Moustafa
- AO Urrutia
- B Palenik
- BA Williams
- C Courties
- CI Castillo-Davis
- DA Petrov
- DA Petrov
- DA Petrov
- DA Petrov
- DA Petrov
- DC Presgraves
- Debashish Bhattacharya
- DF Kapraun
- DG Scofield
- E Derelle
- E Eisenberg
- ET Munoz
- GP Henderson
- H Le Hir
- J Steinkötter
- JM Comeron
- JM Comeron
- JM Comeron
- JM Comeron
- Josep M. Comeron
- JP Blumenstiel
- L Duret
- M Ares Jr
- M Lynch
- M Spingola
- ME Fahey
- MJ Chretiennot-Dinet
- PJ Keeling
- R Ophir
- Robert DeSalle
- S Robbens
- TR Gregory
- TR Gregory
- TR Gregory
- William Lanier
- XY Ren
- YW Fong
- Z Zhou
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2008
- Field of study
Background: The genome of the pico-eukaryotic (bacterial-sized) prasinophyte green alga Ostreococcus lucimarinus has one of the highest gene densities known in eukaryotes, yet it contains many introns. Phylogenetic studies suggest this unusually compact genome (13.2 Mb) is an evolutionarily derived state among prasinophytes. The presence of introns in the highly reduced O. lucimarinus genome appears to be in opposition to simple explanations of genome evolution based on unidirectional tendencies, either neutral or selective. Therefore, patterns of intron retention in this species can potentially provide insights into the forces governing intron evolution. Methodology/Principal Findings: Here we studied intron features and levels of expression in O. lucimarinus using expressed sequence tags (ESTs) to annotate the current genome assembly. ESTs were assembled into unigene clusters that were mapped back to the O. lucimarinus Build 2.0 assembly using BLAST and the level of gene expression was inferred from the number of ESTs in each cluster. We find a positive correlation between expression levels and both intron number (R = +0.0893, p =,0.0005) and intron density (number of introns/kb of CDS; R = +0.0753, p =,0.005). Conclusions/Significance: In a species with a genome that has been recently subjected to a great reduction of non-coding DNA, these results imply the existence of selective/functional roles for introns that are principally detectable in highly expressed genes. In these cases, introns are likely maintained by balancing the selective forces favoring their maintenanc
Mode-locking via dissipative Faraday instability
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Emergence of coherent structures and patterns at the nonlinear stage of modulation instability of a uniform state is an inherent feature of many biological, physical and engineering systems. There are several well-studied classical modulation instabilities, such as Benjamin-Feir, Turing and Faraday instability, which play a critical role in the self-organization of energy and matter in non-equilibrium physical, chemical and biological systems. Here we experimentally demonstrate the dissipative Faraday instability induced by spatially periodic zig-zag modulation of a dissipative parameter of the system - spectrally dependent losses - achieving generation of temporal patterns and high-harmonic mode-locking in a fibre laser. We demonstrate features of this instability that distinguish it from both the Benjamin-Feir and the purely dispersive Faraday instability. Our results open the possibilities for new designs of mode-locked lasers and can be extended to other fields of physics and engineering
Hair Cell Bundles: Flexoelectric Motors of the Inner Ear
- Author
- A Flock
- A Wright
- AF Huxley
- AG Petrov
- AG Petrov
- AG Petrov
- AJ Hudspeth
- AJ Hudspeth
- AJ Hudspeth
- AJ Hudspeth
- AJ Ricci
- B Anvari
- C Geisler
- C Harasztosi
- CM Hackney
- CM Hackney
- DE Zetes
- DM Freeman
- E Glassinger
- E Murugasu
- E Verpy
- F Rattay
- H Tiersten
- HJ Kennedy
- HW Lin
- J Cotton
- J Happel
- JA Halter
- JH Nam
- JH Nam
- JH ten Kate
- JJ Guinan
- JR Cotton
- JR Holt
- Kathryn D. Breneman
- KD Breneman
- KD Breneman
- L Meirovitch
- LG Tilney
- LS Frishkopf
- M Muller
- M Vater
- MC Liberman
- ME Benser
- MJ Mulroy
- P Dallos
- P Fuchs
- P Martin
- R Stepanyan
- RD Rabbitt
- Richard D. Rabbitt
- RM Hochmuth
- RM Hochmuth
- RM Raphael
- T Holton
- T Weiss
- TF Weiss
- TJ Garfinkle
- Vladimir Brezina
- VM Eguíluz
- William E. Brownell
- YC Fung
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
Microvilli (stereocilia) projecting from the apex of hair cells in the inner ear are actively motile structures that feed energy into the vibration of the inner ear and enhance sensitivity to sound. The biophysical mechanism underlying the hair bundle motor is unknown. In this study, we examined a membrane flexoelectric origin for active movements in stereocilia and conclude that it is likely to be an important contributor to mechanical power output by hair bundles. We formulated a realistic biophysical model of stereocilia incorporating stereocilia dimensions, the known flexoelectric coefficient of lipid membranes, mechanical compliance, and fluid drag. Electrical power enters the stereocilia through displacement sensitive ion channels and, due to the small diameter of stereocilia, is converted to useful mechanical power output by flexoelectricity. This motor augments molecular motors associated with the mechanosensitive apparatus itself that have been described previously. The model reveals stereocilia to be highly efficient and fast flexoelectric motors that capture the energy in the extracellular electro-chemical potential of the inner ear to generate mechanical power output. The power analysis provides an explanation for the correlation between stereocilia height and the tonotopic organization of hearing organs. Further, results suggest that flexoelectricity may be essential to the exquisite sensitivity and frequency selectivity of non-mammalian hearing organs at high auditory frequencies, and may contribute to the “cochlear amplifier” in mammals
The Evolution of Compact Binary Star Systems
- Author
- A Ahmad
- A Blaauw
- A Bragaglia
- A Burrows
- A Burrows
- A Burrows
- A Büning
- A Cooray
- A Corongiu
- A Duquennoy
- A Gianninas
- A Heger
- A Kashi
- A Kusenko
- A Massevitch
- A Menon
- A Nebot Gómez-Morán
- A Noriega-Crespo
- A Noutsos
- A Palacios
- A Skumanich
- A Stroeer
- A Stroeer
- A Tornambé
- A Ulla
- A Wongwathanarat
- AA Zdziarski
- AC Fabian
- AE Rosenbush
- AG Kuranov
- AG Kuranov
- AG Lyne
- AG Lyne
- AG Lyne
- AG Massevich
- AG Massevitch
- AG Riess
- AH Prestwich
- AI Bogomazov
- AI Karakas
- AJ Farmer
- AJ Faulkner
- AJ Faulkner
- AJ Loveridge
- AJ Ruiter
- AJ Ruiter
- AJ Ruiter
- AJT Poelarends
- AL Kraus
- AL Piro
- AL Piro
- AL Piro
- AM Cherepashchuk
- AM Cherepashchuk
- AM Cherepashchuk
- AR King
- AR King
- AS Endal
- AS Oliveira
- AV Fedorova
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AW Hotan
- B Külebi
- B Külebi
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paxton
- B Paxton
- B Voss
- B Wang
- B Warner
- B Warner
- B Willems
- B Willems
- B Willems
- B Willems
- B-Q For
- BC Barish
- BD Mason
- BD Mason
- BD Metzger
- BE Schaefer
- BJ Shappee
- BJ Shappee
- BMS Hansen
- BP Flannery
- BS Sathyaprakash
- BT Gänsicke
- BT Hayden
- BW Ritchie
- C Badenes
- C Cutler
- C Foellmi
- C Georgy
- C Georgy
- C Georgy
- C Holcomb
- C Karl
- C Kim
- C Knigge
- C Knigge
- C Motch
- C Palenzuela
- C Raskin
- C Raskin
- C Ritossa
- C Weidner
- C-A Faucher-Giguère
- C-A Faucher-Giguère
- CA Whyte
- CD Bailyn
- CD Bailyn
- CJ Deloye
- CJ Philp
- CL Fryer
- CL Fryer
- CL Fryer
- CL Fryer
- CL Fryer
- CL Rodriguez
- CO Heinke
- CR Evans
- D Bhattacharya
- D Branch
- D Foss
- D Gerosa
- D Grossman
- D Hils
- D Hils
- D Ibeling
- D Kasen
- D Koester
- D Koester
- D Kushnir
- D Lai
- D Lai
- D Levitan
- D Lommen
- D Maoz
- D Prialnik
- D Prialnik
- D Prialnik
- D Raghavan
- D Schiminovich
- D Vanbeveren
- DA Dale
- DA Howell
- DJ Champion
- DJ Nice
- DJ Nice
- DL Kaplan
- DM Townsley
- DM Townsley
- DR Lorimer
- DW Schuerman
- E Bear
- E Berger
- E Cappellaro
- E Cappellaro
- E Donder De
- E Donder De
- E Donder De
- E Ergma
- E Ergma
- E García-Berro
- E Kuulkers
- E Livne
- E Livne
- E Nakar
- E Pfahl
- E Pfahl
- E Pfahl
- E Pylyser
- E Schatzman
- E Schatzman
- E-M Pauli
- EE Salpeter
- EF Keane
- EI Popova
- EI Popova
- EJ Lentz
- EL Robinson
- EL Robinson
- EM Green
- EM Sion
- EM Sion
- EM Sion
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- ES Phinney
- F Acernese
- F Camilo
- F D’Antona
- F Espinosa Lara
- F Foucart
- F Herwig
- F Herwig
- F Koliopanos
- F Ozel
- F Ozel
- F Patat
- F Ricci
- F Verbunt
- F Verbunt
- F Yuan
- FB Bianco
- FR Boffi
- FR Stephenson
- FS Kitaura
- FX Timmes
- FX Timmes
- G Duchêne
- G Giampieri
- G Hobbs
- G Lü
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Pandey
- G Ramsay
- G Ramsay
- G Stasińska
- G Tovmassian
- GE Brown
- GE Brown
- GE Soberman
- GH Tovmassian
- GHA Roelofs
- GHA Roelofs
- GJ Savonije
- GL Israel
- GP Kuiper
- GS Bisnovatyi-Kogan
- GS Bisnovatyi-Kogan
- GS Bisnovatyi-Kogan
- GS Bisnovatyi-Kogan
- H Belkus
- H Bondi
- H Ge
- H Ge
- H Ritter
- H Saio
- H Saio
- H Sana
- H Sana
- H Susa
- H-T Janka
- H-T Janka
- HA Abt
- HA Bethe
- HA Kobulnicky
- HB Perets
- HC Harris
- HC Spruit
- HC Spruit
- HHB Lau
- HS Zapolsky
- I Brott
- I Dominguez
- I Domínguez
- I Domínguez
- I Hachisu
- I Hachisu
- I Hachisu
- I Hachisu
- I Hachisu
- I Hachisu
- I Iben Jr
- I Iben Jr
- I Iben Jr
- I Iben Jr
- I Iben Jr
- I Iben Jr
- I Iben Jr
- I Iben Jr
- I Iben Jr
- I Iben Jr
- I Iben Jr
- I Idan
- I Kotko
- I Kowalska
- I Mandel
- IF Mirabel
- IF Mirabel
- IH Stairs
- IH Stairs
- IR Seitenzahl
- IS Shklovskii
- J Abadie
- J Abadie
- J Boersma
- J Casares
- J Crowder
- J Faulkner
- J Faulkner
- J Fuller
- J Fuller
- J Girven
- J Guillochon
- J Isern
- J Isern
- J Liebert
- J Nordhaus
- J Papaloizou
- J Schwab
- J Smak
- J Whelan
- J-C Passy
- J-C Passy
- J-E Solheim
- J-E Solheim
- J-E Solheim
- J-P Lasota
- J-U Ness
- JA Edlund
- JA Freitas Pacheco de
- JA Frieman
- JA Orosz
- JA Orosz
- JA Orosz
- JA Orosz
- JB Lamb
- JC Lombardi Jr
- JCA Miller-Jones
- JDM Dewi
- JDM Dewi
- JE Faller
- JE Gunn
- JE McClintock
- JE McClintock
- JE Pringle
- JG Mengel
- JH Shiode
- JH Taylor
- JJ Drake
- JJ Hermes
- JJM Zand in’t
- JM Lattimer
- JM Lattimer
- JM Silverman
- JM Silverman
- JM Silverman
- JM Weisberg
- JM Weisberg
- JP Cox
- JP Greve De
- JPA Clark
- JPA Clark
- JR Hurley
- JR Hurley
- JR Maund
- JS Bloom
- JSW Claeys
- JW Truran
- JW Truran
- K Belczynski
- K Belczynski
- K Belczynski
- K Belczynski
- K Belczynski
- K Belczynski
- K Hotokezaka
- K Lepo
- K Moore
- K Nomoto
- K Nomoto
- K Nomoto
- K Nomoto
- K Riles
- K Siellez
- K Somiya
- K Takahashi
- K Yagi
- K-C Pan
- KA Postnov
- KA Postnov
- KA Postnov
- KJ Shen
- KJ Shen
- KJ Shen
- KJ Shen
- KJ Shen
- KJ Shen
- KK Ghosh
- KM Blundell
- KS Thorne
- KS Thorne
- L Bildsten
- L Bildsten
- L Bildsten
- L Chomiuk
- L Chomiuk
- L Dessart
- L Guillemot
- L Kreidberg
- L Mahy
- L Mestel
- L Mestel
- L Piersanti
- L Piersanti
- L Piersanti
- L Piersanti
- L Siess
- L Siess
- L Siess
- L Trepl
- L-X Li
- LA Nelson
- LD Landau
- LD Landau
- LG Althaus
- LM Close
- LM Haaften van
- LM Haaften van
- LM Haaften van
- LP Grishchuk
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LR Yungelson
- LZ Kelley
- M Bailes
- M Burgay
- M Burgay
- M Dan
- M Dan
- M Dan
- M Dominik
- M Dominik
- M Fink
- M Fukugita
- M Gilfanov
- M Gilfanov
- M Hamuy
- M Henze
- M Hicken
- M Ilkov
- M Kato
- M Kato
- M Kato
- M Kato
- M Kilic
- M Kilic
- M Kilic
- M Kool de
- M Kromer
- M Kromer
- M Livio
- M Livio
- M Nauenberg
- M Plavec
- M Politano
- M Reggiani
- M Rieutord
- M Rigault
- M Rigault
- M Tavani
- M Tsugawa
- M Val-Borro de
- M Yamanaka
- M Zorotovic
- M Zorotovic
- MA Ruderman
- MBN Kouwenhoven
- MBN Kouwenhoven
- MBN Kouwenhoven
- MCP Bours
- MCP Bours
- MCR D’Souza
- ME Alexander
- ME Beer
- ME Prokhorov
- MM Kasliwal
- MM Kasliwal
- MM Phillips
- MM Shara
- MM Shara
- MP Muno
- MR Bate
- MR Drout
- MS Hjellming
- MT Botticella
- MTB Nielsen
- MTB Nielsen
- MV Barkov
- MV Sluys van der
- N Andersson
- N Brandt
- N Chamel
- N Epelstain
- N Gehrels
- N Ivanova
- N Ivanova
- N Ivanova
- N Ivanova
- N Ivanova
- N Ivanova
- N Ivanova
- N Langer
- N Langer
- N Panagia
- N Smith
- N Soker
- N Soker
- N Tominaga
- N Vranesevic
- N Wex
- N Yusof
- NI Shakura
- NJ Cornish
- NM Ashok
- NM Gosnell
- NN Chugai
- NN Chugai
- NN Chugai
- NR Tanvir
- NV Raguzova
- O Birnholtz
- O Graur
- O Graur
- O Marco De
- O Marco De
- O Schnurr
- O Yaron
- OF Dorofeev
- OR Pols
- P Amaro-Seoane
- P Amaro-Seoane
- P André
- P Astier
- P Bagot
- P Eggleton
- P Esposito
- P Gil-Pons
- P Hoeflich
- P Höflich
- P Kahabka
- P Kahabka
- P Lorén-Aguilar
- P Madau
- P Munar-Adrover
- P Podsiadlowski
- P Podsiadlowski
- P Podsiadlowski
- P Podsiadlowski
- P Rodríguez-Gil
- P Ruiz-Lapuente
- P Szypryt
- PA Crowther
- PA Crowther
- PA Crowther
- PA Denissenkov
- PA Woudt
- PA Woudt
- PC Peters
- PD Kiel
- PD Kiel
- PD Sackett
- PE Nugent
- PFL Maxted
- PG Jonker
- PG Pérez-González
- PJ Carter
- PJ Carter
- PJ Carter
- PJ Carter
- PL Bender
- PM Motl
- PM Ricker
- PM Ricker
- PP Eggleton
- R Canal
- R Canal
- R Canal
- R Chini
- R Fender
- R Giacconi
- R Mochkovitch
- R Moll
- R Morrison
- R Napiwotzki
- R Napiwotzki
- R Napiwotzki
- R Narayan
- R Narayan
- R O’Shaughnessy
- R Pakmor
- R Scalzo
- R Scalzo
- R Stefano Di
- R Stefano Di
- R Stefano Di
- R Takahashi
- R Tylenda
- R Voss
- R Waldman
- R Wesson
- RA Chevalier
- RA Chevalier
- RA Chevalier
- RA Chevalier
- RA Hulse
- RA Remillard
- RA Saffer
- RA Saffer
- RA Wade
- RC Kennicutt
- RD Ferdman
- RE Falcon
- RE Taam
- RE Taam
- RE Williams
- RF Webbink
- RF Webbink
- RF Webbink
- RF Webbink
- RF Webbink
- RF Webbink
- RF Webbink
- RH Durisen
- RJ Dewey
- RJ Foley
- RJ Parker
- RK Kopparapu
- RL Barone-Nugent
- RLM Corradi
- RN Manchester
- RP Kraft
- RS Benson
- RW Romani
- RW Romani
- RW Sayer
- S Babak
- S Cassisi
- S Ekström
- S Fabrika
- S Geier
- S Geier
- S Geier
- S Geier
- S Geier
- S Geier
- S Geier
- S Horiuchi
- S Ji
- S Johnston
- S Jones
- S Jones
- S Justham
- S Miyaji
- S Mohamed
- S Neo
- S Nissanke
- S Nissanke
- S Oslowski
- S Perlmutter
- S Rappaport
- S Rappaport
- S Rappaport
- S Refsdal
- S Repetto
- S Rosswog
- S Shah
- S Shah
- S Starrfield
- S Starrfield
- S Starrfield
- S Starrfield
- S Taubenberger
- S Toonen
- S Toonen
- S Vennes
- S Vereshchagin
- S Yu
- S Yu
- S-B Qian
- S-C Yoon
- S-C Yoon
- S-C Yoon
- S-C Yoon
- SA Colgate
- SA Sim
- SB Anderson
- SB Popov
- SC Vila
- SE Thorsett
- SE Timpano
- SE Woosley
- SE Woosley
- SE Woosley
- SF Portegies Zwart
- SF Portegies Zwart
- SF Portegies Zwart
- SH Lubow
- SL Larson
- SL Shapiro
- SN Shore
- SP Littlefair
- SS Kumar
- T Abel
- T Bulik
- T Dermine
- T Fragos
- T Kupfer
- T Linden
- T Linden
- T Nugis
- T Pan
- T Shahbaz
- T Wettig
- T-W Wong
- TA Prince
- TB Littenberg
- TE Woods
- TE Woods
- TE Woods
- TF Cartwright
- TJ Maccarone
- TM Tauris
- TM Tauris
- TM Tauris
- TR Marsh
- TR Marsh
- TR Marsh
- TR Marsh
- TR Marsh
- TR Marsh
- U Heber
- V Gokhale
- V Kalogera
- V Kalogera
- V Kalogera
- V Kalogera
- V Kalogera
- V Kalogera
- VA Brumberg
- VG Kornilov
- VG Kornilov
- VM Kaspi
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VM Lipunov
- VN Mironovskii
- VS Petrov
- VV Davydov
- W Benz
- W Fong
- W Li
- W Li
- W-R Hamann
- WE Kerzendorf
- WE Kerzendorf
- WK Rose
- WM Farr
- WM Sparks
- WM Wolf
- WR Brown
- WR Brown
- X Meng
- X Wang
- X Zhang
- X-J Xu
- X-J Xu
- Y Osaki
- YA Fadeyev
- YA Fadeyev
- YB Zel’dovich
- YV Baryshev
- Z Barkat
- Z Han
- Z Han
- Z Han
- Z Han
- Z Han
- Z Kopal
- Z Li
- Z-W Liu
- ZW Liu
- ÉÉ Flanagan
- Publication venue
- 'Living Reviews'
- Publication date
- 03/01/2007
- Field of study
We review the formation and evolution of compact binary stars consisting of
white dwarfs (WDs), neutron stars (NSs), and black holes (BHs). Binary NSs and
BHs are thought to be the primary astrophysical sources of gravitational waves
(GWs) within the frequency band of ground-based detectors, while compact
binaries of WDs are important sources of GWs at lower frequencies to be covered
by space interferometers (LISA). Major uncertainties in the current
understanding of properties of NSs and BHs most relevant to the GW studies are
discussed, including the treatment of the natal kicks which compact stellar
remnants acquire during the core collapse of massive stars and the common
envelope phase of binary evolution. We discuss the coalescence rates of binary
NSs and BHs and prospects for their detections, the formation and evolution of
binary WDs and their observational manifestations. Special attention is given
to AM CVn-stars -- compact binaries in which the Roche lobe is filled by
another WD or a low-mass partially degenerate helium-star, as these stars are
thought to be the best LISA verification binary GW sources.Comment: 105 pages, 18 figure
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- 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
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alexander J
- Aliev T
- Allfrey P
- 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
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Asaadi J
- Asghar MI
- Askew A
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
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- Yilmaz Y
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- Ziebarth EB
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- Zorbilmez C
- Zotto P
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- Zumerle G
- Zuranski A
- 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
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
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- Adam W
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- Adiguzel A
- Adler V
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- Agram JL
- Aguilar-Benitez M
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- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
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- Albayrak EA
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- Amsler C
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- Anastassov A
- Anderson J
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- Andreev Y
- Andrews W
- Anghel IM
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- Antunes JR
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- Apollinari G
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- Worm SD
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- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- 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
- Zang SL
- 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
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- Zoeller MH
- Zotto P
- Zou W
- 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
Effective Rheology of Bubbles Moving in a Capillary Tube
- Author
- Abelev B
- Adam J
- Adamova D
- Adare AM
- Aggarwal MM
- Agocs AG
- Agostinelli A
- Ahammed Z
- Ahmad N
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- Alaniz EC
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- Alessandro B
- Alici A
- Alkin A
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- Andrei C
- Andronic A
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- Augustinus A
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- Balbastre GC
- Baldisseri A
- Baldit A
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- Baumann C
- Bearden IG
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- Belmont-Moreno E
- Bencedi G
- Beole S
- Berceanu I
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bergmann C
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- Bhasin A
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- Borissov A
- Bornec YL
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- Bossu F
- Botje M
- Bottger S
- Boyer B
- Braidot E
- Braun-Munzinger P
- Bregant M
- Breitner T
- Browning TA
- Broz M
- Brun R
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- Bruno GE
- Budnikov D
- Buesching H
- Bufalino S
- Bugaiev K
- Busch O
- Bustamante RTJ
- Buthelezi Z
- Caffarri D
- Cahuantzi MR
- Cai X
- Caines H
- Camerini P
- Carena F
- Carena W
- Carminati F
- Caro AD
- Castellanos JC
- Castro XS
- Casula EAR
- Cataldo GD
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- Chang B
- Chapeland S
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- Chawla I
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- Chinellato DD
- Chochula P
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- Christakoglou P
- Christensen CH
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- Chujo T
- Chung SU
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Coccetti F
- Colamaria F
- Colella D
- Collaboration ALICE
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- Crescio E
- Crochet P
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- Cuveland JD
- Dainese A
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- Danu A
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- Dominguez I
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- Engel H
- Erasmo GD
- Erdal HA
- Espagnon B
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- Fehlker D
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- Feofilov G
- Ferreiro EG
- Ferretti A
- Ferretti R
- Ferroli RB
- Figiel J
- Figueredo MAS
- Filchagin S
- Filho EPDO
- Filho NC
- Finogeev D
- Fionda FM
- Fiore EM
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- Foertsch S
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- Fragiacomo E
- Fragkiadakis M
- Frankenfeld U
- Fuchs U
- Furget C
- Gaardhoje JJ
- Gagliardi M
- Gago A
- Gallio M
- Gangadharan DR
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- Garcia GM
- Garcia-Solis E
- Garishvili I
- Gerhard J
- Germain M
- Geuna C
- Gheata A
- Gheata M
- Ghidini B
- Ghosh P
- Gianotti P
- Giglio CD
- Girard MF
- Girard MR
- Giubellino P
- Gladysz-Dziadus E
- Glassel P
- Godoy DAMD
- Gomez R
- Gonzalez-Trueba LH
- Gonzalez-Zamora P
- Gorbunov S
- Goswami A
- Gotovac S
- Grabski V
- Graczykowski LK
- Grajcarek R
- Grelli A
- Grigoras A
- Grigoras C
- Grigoriev V
- Grigoryan A
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- Grinyov B
- Grion N
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- Grossiord JY
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- Gruttola DD
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- Guevara PLD
- Guilbaud M
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- Gunji T
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- Gupta R
- Gutbrod H
- Gutierrez CG
- Haaland O
- Hadjidakis C
- Haiduc M
- Haller BV
- Hamagaki H
- Hamar G
- Han BH
- Hanratty LD
- Hansen A
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- Harris JW
- Hartig M
- Hasegan D
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- Hayrapetyan A
- Heckel ST
- Heide M
- Helstrup H
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- Hille PT
- Hippolyte B
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- Huber S
- Humanic TJ
- Hwang DS
- Ichou R
- Ilkaev R
- Ilkiv I
- Inaba M
- Incani E
- Innocenti GM
- Innocenti PG
- Ippolitov M
- Irfan M
- Ivan C
- Ivanov A
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- Ivanytskyi O
- Jacholkowski A
- Jacobs PM
- Jancurova L
- Jang HJ
- Jangal S
- Janik MA
- Janik R
- Jayarathna PHSY
- Jena S
- Jirden L
- Jones PG
- Jung H
- Jusko A
- Kaidalov AB
- Kakoyan V
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- Kalliokoski T
- Kalweit A
- Kanaki K
- Kang JH
- Kaplin V
- Karampatsos LX
- Karavichev O
- Karavicheva T
- Karpechev E
- Kazantsev A
- Kebschull U
- Keidel R
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- Khanzadeev A
- Kharlov Y
- Kileng B
- Kim B
- Kim DJ
- Kim DW
- Kim JH
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- Kirsch S
- Kisel I
- Kiselev S
- Kisiel A
- Klay JL
- Klein J
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- Zampolli C
- Zaporozhets S
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- Zavada P
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- Zbroszczyk H
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- Zetina LM
- Zgura IS
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- Zimmermann A
- Zinovjev G
- Zoccarato Y
- Zynovyev M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 16/03/2012
- Field of study
We calculate the average volumetric flux versus pressure drop of bubbles
moving in a single capillary tube with varying diameter, finding a square-root
relation from mapping the flow equations onto that of a driven overdamped
pendulum. The calculation is based on a derivation of the equation of motion of
a bubble train from considering the capillary forces and the entropy production
associated with the viscous flow. We also calculate the configurational
probability of the positions of the bubbles.Comment: 4 pages, 1 figur
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Smirnov I
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- Yilmaz Y
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
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- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
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- Zeinali 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
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
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- Acosta MV
- Adair A
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- CMS Collaboration
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- Cumalat JP
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- Xiao H
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- 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
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- Zhukov V
- Zhukova V
- Ziebarth EB
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- 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
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- 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
- 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
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