109 research outputs found
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An Overview of the Use of Neural Networks for Data Mining Tasks
- Author
- Publication venue
- 'Wiley'
- Publication date
- 01/01/2012
- Field of study
In the recent years the area of data mining has experienced a considerable demand for technologies that extract knowledge from large and complex data sources. There is a substantial commercial interest as well as research investigations in the area that aim to develop new and improved approaches for extracting information, relationships, and patterns from datasets. Artificial Neural Networks (NN) are popular biologically inspired intelligent methodologies, whose classification, prediction and pattern recognition capabilities have been utilised successfully in many areas, including science, engineering, medicine, business, banking, telecommunication, and many other fields. This paper highlights from a data mining perspective the implementation of NN, using supervised and unsupervised learning, for pattern recognition, classification, prediction and cluster analysis, and focuses the discussion on their usage in bioinformatics and financial data analysis tasks
Evolutionary and pulsational properties of white dwarf stars
- Author
- A Baglin
- A Beauchamp
- A Bischoff-Kim
- A Bischoff-Kim
- A Bischoff-Kim
- A Díaz–Pinto
- A Gautschy
- A Gautschy
- A Gautschy
- A Gautschy
- A Gianninas
- A Gianninas
- A Kawka
- A Nitta
- A Nitta
- A Udalski
- AA Abrikosov
- AC Becker
- AD Grauer
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AH Córsico
- AJ Brickhill
- Alejandro H. Córsico
- AN Cox
- AS Mukadam
- AS Mukadam
- AU Landolt
- B Goldman
- B Pfeiffer
- B Voss
- B Warner
- BG Castanheira
- BG Castanheira
- BG Castanheira
- BG Castanheira
- BM Lasker
- BM Lasker
- BMS Hansen
- BMS Hansen
- BMS Hansen
- BMS Hansen
- BMS Hansen
- BN Barlow
- BT Gänsicke
- C Alcock
- C Alcock
- C Alcock
- C Ritossa
- C Ritossa
- CJ Deloye
- CJ Hansen
- CL Pekeris
- D Branch
- D Kilkenny
- D Koester
- D Koester
- D Koester
- D Koester
- D Koester
- D Koester
- D Saumon
- D Saumon
- D Schönberner
- DA Kirshnitz
- DE Winget
- DE Winget
- DE Winget
- DE Winget
- DE Winget
- DE Winget
- DE Winget
- DE Winget
- DE Winget
- DE Winget
- DE Winget
- DG York
- DJ Eisenstein
- DJ Stevenson
- DQ Lamb
- E García-Berro
- E García-Berro
- E García-Berro
- E García-Berro
- E García-Berro
- E García–Berro
- E García–Berro
- E Sauvenier-Goffin
- EC Stoner
- EE Salpeter
- EL Robinson
- EL Robinson
- EL Robinson
- EM Green
- Enrique García-Berro
- F D’Antona
- F D’Antona
- F Herwig
- F Mullally
- G Chanmugam
- G Fontaine
- G Fontaine
- G Fontaine
- G Fontaine
- G Fontaine
- G Shaviv
- G Vauclair
- G Vauclair
- G Vauclair
- GG Raffelt
- H Saio
- H Saio
- H Saio
- HB Richer
- HB Richer
- HC Harris
- HE Bond
- HE Bond
- HE Bond
- HM Horn van
- HN Russell
- I Domínguez
- I Iben Jr
- I Iben Jr
- I Iben Jr
- I Renedo
- J Camacho
- J Faulkner
- J Guerrero
- J Isern
- J Isern
- J Isern
- J Isern
- J Isern
- J Isern
- J Isern
- J Liebert
- J Madej
- J Yoo
- J-E Solheim
- J-N Fu
- JC Clemens
- JC Clemens
- JES Costa
- JES Costa
- JM González Pérez
- Jordi Isern
- JP Cox
- JP Ostriker
- JT McGraw
- JT McGraw
- JT McGraw
- K Unglaub
- K Werner
- K Werner
- K Werner
- K Werner
- L Koesterke
- L Mestel
- L Segretain
- L Siess
- L Stanghellini
- Leandro G. Althaus
- LG Althaus
- LG Althaus
- LG Althaus
- LG Althaus
- LG Althaus
- LG Althaus
- LG Althaus
- LG Althaus
- LG Althaus
- LG Althaus
- LG Althaus
- LG Althaus
- LR Bedin
- M Aizenman
- M Hernanz
- M Kilic
- M Salaris
- M Salaris
- M Schmidt
- M Tassoul
- M Tassoul
- MD Reed
- MH Kerkwijk van
- MH Kerkwijk van
- MH Montgomery
- MH Montgomery
- MH Montgomery
- MH Montgomery
- MJ Sarna
- MM Miller Bertolami
- MM Miller Bertolami
- MM Miller Bertolami
- MS O’Brien
- MS O’Brien
- MY Fujimoto
- N Dolez
- N Itoh
- O Straniero
- OG Benvenuto
- OG Benvenuto
- P Bergeron
- P Bergeron
- P Bergeron
- P Bergeron
- P Brassard
- P Brassard
- P Brassard
- P Brassard
- P Brassard
- P Dufour
- P Dufour
- P Dufour
- P Dufour
- P Dufour
- P Goldreich
- P Lorén-Aguilar
- P Tisserand
- P-O Quirion
- P-O Quirion
- PA Bradley
- PA Bradley
- PA Bradley
- PA Bradley
- PA Bradley
- PA Bradley
- PA Bradley
- PA Bradley
- PA Bradley
- PG Prada Moroni
- PJ Ledoux
- PJ Ledoux
- PW Jones
- R Ciardullo
- R Ibata
- R Kippenhahn
- R Kotak
- R Kotak
- R Kotak
- R Kotak
- R Kotak
- R Mochkovitch
- R Silvotti
- R Silvotti
- RA Méndez
- RA Méndez
- RD Rohrmann
- RD Rohrmann
- RE Nather
- RH Fowler
- RVR Harper
- S Catalán
- S Chandrasekhar
- S Chandrasekhar
- S Charpinet
- S DeGennaro
- S Dreizler
- S Dreizler
- S Dreizler
- S Starrfield
- S Starrfield
- S Torres
- S Torres
- S Torres
- S Torres
- SD Hügelmeyer
- SD Kawaler
- SD Kawaler
- SD Kawaler
- SD Kawaler
- SD Kawaler
- SD Kawaler
- SD Kawaler
- SE Thompson
- SJ Kleinman
- SL Casewell
- SO Kepler
- SO Kepler
- SO Kepler
- SO Kepler
- T Driebe
- T Hippel Von
- T Hippel Von
- T Lasserre
- T Nagel
- T Rauch
- TG Cowling
- TG Cowling
- TM Brown
- TR Marsh
- TS Metcalfe
- TS Metcalfe
- TS Metcalfe
- TS Metcalfe
- V Weidemann
- W Anderson
- W Dziembowski
- W Dziembowski
- W Unno
- WM Luyten
- WS Adams
- WS Adams
- Y Muraki
- Zs Bognár
- ZW Xu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 15/07/2010
- Field of study
Abridged. White dwarf stars are the final evolutionary stage of the vast
majority of stars, including our Sun. The study of white dwarfs has potential
applications to different fields of astrophysics. In particular, they can be
used as independent reliable cosmic clocks, and can also provide valuable
information about the fundamental parameters of a wide variety of stellar
populations, like our Galaxy and open and globular clusters. In addition, the
high densities and temperatures characterizing white dwarfs allow to use these
stars as cosmic laboratories for studying physical processes under extreme
conditions that cannot be achieved in terrestrial laboratories. They can be
used to constrain fundamental properties of elementary particles such as axions
and neutrinos, and to study problems related to the variation of fundamental
constants.
In this work, we review the essentials of the physics of white dwarf stars.
Special emphasis is placed on the physical processes that lead to the formation
of white dwarfs as well as on the different energy sources and processes
responsible for chemical abundance changes that occur along their evolution.
Moreover, in the course of their lives, white dwarfs cross different
pulsational instability strips. The existence of these instability strips
provides astronomers with an unique opportunity to peer into their internal
structure that would otherwise remain hidden from observers. We will show that
this allows to measure with unprecedented precision the stellar masses and to
infer their envelope thicknesses, to probe the core chemical stratification,
and to detect rotation rates and magnetic fields. Consequently, in this work,
we also review the pulsational properties of white dwarfs and the most recent
applications of white dwarf asteroseismology.Comment: 85 pages, 28 figures. To be published in The Astronomy and
Astrophysics Revie
Genome of the Avirulent Human-Infective Trypanosome—Trypanosoma rangeli
- Author
- A Buschiazzo
- AC Frasch
- AC Ivens
- AL Price
- Alexandra Gerber
- Ana Tereza Ribeiro de Vasconcelos
- Arnaldo Zaha
- B Li
- B Roure
- Björn Andersson
- C Biemont
- C Folgueira
- CA Buscaglia
- CA Buscaglia
- Carlos Talavera-Lopez
- CB Lira
- CB Toaldo
- CE Butler
- Claudia Elizabeth Thompson
- CP Pena
- CS Peacock
- D Bahia
- D Bahia
- D Cosentino-Gomes
- D Ekanayake
- D Horn
- D Miranda-Saavedra
- D Salmon
- DA Largaespada
- DA Urrea
- DA Urrea
- Daniella Castanheira Bartholomeu
- DC Bartholomeu
- DG Passos-Silva
- Diana Bahia
- DM Martin
- Débora Denardin Lückemeyer
- E Ghedin
- EC Grisard
- EC Grisard
- Edmundo Carlos Grisard
- EJ Tobie
- EL Raven
- Elgion Loreto
- Elisa Beatriz Prestes
- F Corpet
- F Guhl
- F Guhl
- F Maia Da Silva
- F Maia da Silva
- F Maia da Silva
- F Sievers
- FB Nogueira
- Fábio Mitsuo Lima
- G Benson
- G Wagner
- GA Vallejo
- GA Vallejo
- GA Vallejo
- Gabriela Rodrigues-Luiz
- Glauber Wagner
- Gustavo Adolfo Vallejo
- H Castro
- H Diez
- H Diez
- H Diez
- H Ngo
- H Shi
- H Shi
- HA Schmidt
- HG van Luenen
- HS Kim
- I Kamileri
- I Romero
- J Baum
- J Fonager
- J Henriksson
- J Jurka
- JD Damasceno
- JE Vasquez
- Jessica C. Kissinger
- JF Turrens
- JH Lee
- JL Affranchino
- JL Parsons
- José Franco da Silveira Filho
- JV Bannister
- K Ersfeld
- K Strimmer
- KA Norris
- Karina Mariante Monteiro
- Kevin Morris Tyler
- KL Patrick
- L Piacenza
- L Piacenza
- LF Lye
- LG Almeida
- LJ Cliffe
- LM Freitas
- Luiz Gonzaga Paula de Almeida
- M Berriman
- M Cabrine-Santos
- M Cabrine-Santos
- M Schramp
- M Steindel
- MA Chiurillo
- MA de Sousa
- Mauro Freitas Ortiz
- MB Rogers
- MC Elias
- MC Motta
- MD Pineyro
- MF Amaya
- MH de Moraes
- MH Saier Jr
- MI Cano
- Miguel Angel Chiurillo
- Milene Höehr de Moraes
- MJ Fraser Jr
- MJ Schofield
- MM Kangussu-Marcolino
- MP Wymann
- MR Briones
- MR Garcia Silva
- MT Tammi
- Mário Steindel
- N Anez-Rojas
- N Añez
- N Inoue
- N Saitou
- NM El-Sayed
- NM El-Sayed
- O Franzen
- O Franzen
- Oberdan de Lima Cunha
- P Luciano
- Patrícia Hermes Stoco
- R Bosotti
- R Marone
- RD Page
- RL Barnes
- Rondon Mendonça-Neto
- Rosane Silva
- RR Moraes Barros
- RT Souza
- S Cestari Idos
- S Kumar
- S Martinez-Calvillo
- S Muller
- S Schenkman
- Santuza Maria Ribeiro Teixeira
- SF Altschul
- Silvane Maria Fonseca Murta
- SJ Westenberger
- SL dos Santos
- SM Teixeira
- SR Wilkinson
- SR Wilkinson
- SR Wilkinson
- SS Dc-Rubin
- Sérgio Schenkman
- T Downing
- TA Minning
- TA Pitcovsky
- Thais Cristine Marques Sincero
- Tiago Antonio de Oliveira Mendes
- Turán Peter Urmenyi
- Viviane Grazielle Silva
- Wanderson Duarte DaRocha
- WD DaRocha
- X Huang
- ZC Caballero
- Álvaro José Romanha
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/09/2014
- Field of study
Background: Trypanosoma rangeli is a hemoflagellate protozoan parasite infecting humans and other wild and domestic mammals across Central and South America. It does not cause human disease, but it can be mistaken for the etiologic agent of Chagas disease, Trypanosoma cruzi. We have sequenced the T. rangeli genome to provide new tools for elucidating the distinct and intriguing biology of this species and the key pathways related to interaction with its arthropod and mammalian hosts. Methodology/Principal Findings: The T. rangeli haploid genome is ,24 Mb in length, and is the smallest and least repetitive trypanosomatid genome sequenced thus far. This parasite genome has shorter subtelomeric sequences compared to those of T. cruzi and T. brucei; displays intraspecific karyotype variability and lacks minichromosomes. Of the predicted 7,613 protein coding sequences, functional annotations could be determined for 2,415, while 5,043 are hypothetical proteins, some with evidence of protein expression. 7,101 genes (93%) are shared with other trypanosomatids that infect humans. An ortholog of the dcl2 gene involved in the T. brucei RNAi pathway was found in T. rangeli, but the RNAi machinery is non-functional since the other genes in this pathway are pseudogenized. T. rangeli is highly susceptible to oxidative stress, a phenotype that may be explained by a smaller number of anti-oxidant defense enzymes and heatshock proteins. Conclusions/Significance: Phylogenetic comparison of nuclear and mitochondrial genes indicates that T. rangeli and T. cruzi are equidistant from T. brucei. In addition to revealing new aspects of trypanosome co-evolution within the vertebrate and invertebrate hosts, comparative genomic analysis with pathogenic trypanosomatids provides valuable new information that can be further explored with the aim of developing better diagnostic tools and/or therapeutic targets
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
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
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- Akesson TPA
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- Akimov AV
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- Aktas A
- Alam MA
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- Aleksandrov IN
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- Alexa C
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- Alexandre G
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- Allwood-Spiers SE
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- Zhemchugov A
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Measurement of the cross-section for b-jets produced in association with a Z boson at root s=7 TeV with the ATLAS detector ATLAS Collaboration
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
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- Adye T
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- Aguilar-Saavedra JA
- Aharrouche M
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- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
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- Alexandre G
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- Aliev M
- Alimonti G
- Alison J
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- Allport PP
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- Zhemchugov A
- Zheng S
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- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2011
- Field of study
A measurement is presented of the inclusive cross-section for b-jet production in association with a Z boson in pp collisions at a centre-of-mass energy of root s = 7 TeV. The analysis uses the data sample collected by the ATLAS experiment in 2010, corresponding to an integrated luminosity of approximately 36 pb(-1). The event selection requires a Z boson decaying into high P-T electrons or muons, and at least one b-jet, identified by its displaced vertex, with transverse momentum p(T) > 25 GeV and rapidity vertical bar y vertical bar < 2.1. After subtraction of background processes, the yield is extracted from the vertex mass distribution of the candidate b-jets. The ratio of this cross-section to the inclusive Z cross-section (the average number of b-jets per Z event) is also measured. Both results are found to be in good agreement with perturbative QCD predictions at next-to-leading order
Determination of the ratio of b-quark fragmentation fractions fs/fd in pp collisions at √s = 7 TeV with the ATLAS Detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
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- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
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- Allbrooke BMM
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- Amadio BT
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- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yuen SPY
- Yurkewicz A
- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
With an integrated luminosity of 2.47 fb−1 recorded by the ATLAS experiment at the LHC, the exclusive decays B 0s→J/ψϕ and B0d→J/ψK*0 of B mesons produced in pp collisions at √s=7 TeV are used to determine the ratio of fragmentation fractions fs/fd. From the observed B0s→J/ψϕ and B0d→J/ψK*0 yields, the quantity (fs/fd)[B(B0s→J/ψϕ)/B(B 0d→J/ψK*0)] is measured to be 0.199±0.004(stat)±0.008(syst). Using a recent theory prediction for [B(B0s→J/ψϕ)/B(B0d→J/ψK*0)] yields (fs/fd)=0.240±0.004(stat)±0.010(syst)±0.017(th). This result is based on a new approach that provides a significant improvement of the world average
Identification of boosted, hadronically decaying W bosons and comparisons with ATLAS data taken at √s = 8 TeV
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- X. Chen
- X. Hu
- X. Ju
- X. Lei
- X. Li
- X. Lou
- X. Ruan
- X. Sun
- X. Wang
- X. Wu
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- X. Zhuang
- Y Cui
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- Y. Amaral Coutinho
- Y. Arai
- Y. B. Pan
- Y. Bai
- Y. Benhammou
- Y. C. Yap
- Y. Chen
- Y. Cheng
- Y. Coadou
- Y. Davygora
- Y. Enari
- Y. F. Ryabov
- Y. Fang
- Y. Gao
- Y. Guo
- Y. Hasegawa
- Y. Heng
- Y. Hernández Jiménez
- Y. Horii
- Y. Huang
- Y. Ikegami
- Y. Ilchenko
- Y. J. Schnellbach
- Y. Jiang
- Y. K. Kim
- Y. Kataoka
- Y. Komori
- Y. Kulchitsky
- Y. Li
- Y. Liu
- Y. Makida
- Y. Minami
- Y. Ming
- Y. Nagai
- Y. Nagasaka
- Y. Nakahama
- Y. Ninomiya
- Y. Okumura
- Y. Oren
- Y. Qin
- Y. Rozen
- Y. S. Gao
- Y. Sakurai
- Y. Sasaki
- Y. Silver
- Y. Smirnov
- Y. Sugaya
- Y. Takubo
- Y. Tayalati
- Y. Unno
- Y. Wu
- Y. Yamaguchi
- Y. Yamazaki
- Y. Yang
- Y. Yasu
- Y. Zhao
- Y. Zhu
- Yu. A. Tikhonov
- Z. Barnovska
- Z. D. Greenwood
- Z. Dolezal
- Z. Gecse
- Z. H. Citron
- Z. Hajduk
- Z. Hubacek
- Z. Idrissi
- Z. J. Grout
- Z. Kohout
- Z. Liang
- Z. M. Karpova
- Z. Marshall
- Z. Rurikova
- Z. Vykydal
- Z. Yan
- Z. Zhang
- Z. Zhao
- Z. Zinonos
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
This paper reports a detailed study of techniques for identifying boosted, hadronically decaying W bosons using 20.3 fb −¹ of proton–proton collision data collected by the ATLAS detector at the LHC at a centre-of-mass energy √s = 8 TeV. A range of techniques for optimising the signal jet mass resolution are combined with various jet substructure variables. The results of these studies in Monte Carlo simulations show that a simple pairwise combination of groomed jet mass and one substructure variable can provide a 50 % efficiency for identifying W bosons with transverse momenta larger than 200 GeV while maintaining multijet background efficiencies of 2–4 % for jets with the same transverse momentum. These signal and background efficiencies are confirmed in data for a selection of tagging techniques
Search for the standard model Higgs boson in the diphoton decay channel with 4.9fb -1 of pp collision data at √s=7TeV with atlas
- Author
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- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdesselam A
- Abdinov O
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- Åkesson TPA
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- Publication venue
- Publication date
- 01/01/2012
- Field of study
A search for the standard model Higgs boson is performed in the diphoton decay channel. The data used correspond to an integrated luminosity of 4.9 fb-1 collected with the ATLAS detector at the Large Hadron Collider in proton-proton collisions at a center-of-mass energy of √s=7 TeV. In the diphoton mass range 110–150 GeV, the largest excess with respect to the background-only hypothesis is observed at 126.5 GeV, with a local significance of 2.8 standard deviations. Taking the look-elsewhere effect into account in the range 110–150 GeV, this significance becomes 1.5 standard deviations. The standard model Higgs boson is excluded at 95% confidence level in the mass ranges of 113–115 GeV and 134.5–136 GeV
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