The Very Large Telescope Interferometer
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Transcript of The Very Large Telescope Interferometer
The Very LargeTelescope Interferometer
Neon School, Garching29 August, 2008
Andrea RichichiEuropean Southern Observatory
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0.2
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~ /D
~ /B
D
B
/2
/2
Michelson Stellar Interferometer
Stellar source with angular size α0
Add fringe patterns (i.e. intensities) between ± α0/2
Resulting fringe pattern shows reduced contrast.Reduced contrast depends on B – and on α0 .
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movies courtesy of A. Glindemann
Optical vs Radio Interferometry
In common: Visibilities, Closure Phases, Angular Resolution (λ/B)
Radio: more baselines, phases, “true” imaging
VLTI Scheme
The wavefronts must be “clean”, i.e. adaptive optics needed for large telescopes.
The optical path difference must be continuously compensated by the delay lines.
Atmospheric turbulence causes rapid fringe motion which must be “frozen” by a so-called fringe tracker.
The “Paranal Express”
• correct sidereal path difference
• six delay lines• combine all UT
baselines• combine almost all
AT baselines• laser metrology
The VLTI TodayThe VLTI Today
+ FINITO, IRIS, Differential Delay Lines, ARAL, vibration correction, ...
How to obtain and use VLTI data
Public Archive (VINCI~20000 OBs, SDT, MIDI, AMBER): register as an Archive user
VINCI: pipeline
MIDI: MIA/EWS software (IDL)
AMBER: Ammyorick, Reflex
Write your own proposal
Interferometric Science Highlights
AGNs (dust tori)
Hot stars; massive stars; star formation
Evolved stars; dust in giants; AGBs
Stellar pulsation
Binary stars
MS stars and fundamental parameters
Search for exoplanets (direct detection)
Solar system (asteroids)
Black holes and relativity
• Angular diameter (interferometry)
• Radial velocity data (spectroscopy)
Cepheid Stars
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0.0 0.2 0.4 0.6 0.8 1.0
Phase
Taille
rela
tive (
Dsol)
1.50
1.55
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1.65
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1.75
0 0.2 0.4 0.6 0.8 1Phase
DU (mas)
Perpendicularly to the plane of the sky In the plane of the sky
Distance
Re
lativ
e s
ize
(S
ola
r u
nits
)
An
gu
lar
dia
me
ter(
ma
s)
From P. Kervella (2005)
Cep
• Prototype Classical Cepheid• Interferometry is no longer the
limitation to the IBW method• Individual V2 lead to / <
0.5% • Potentially*, the distance is
determined at the 2% level
* How well do we trust LD & p-factor models ???
Mourard et al. 1997Pulsation not detected
Lane et al. 2000First detection
Cep FLUOR/CHARA
Evolution of the IBW method at a glance:
B=313m
From A. Mérand (2005)
l Car
2.4
2.6
2.8
3.0
3.2
3.4
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4
Pulsation Phase
LD (
mas
)SUSI Observations
VLTI Observations
From J. Davis (2005)
Potential distance uncert. 11/545pc
The VLTI TomorrowThe VLTI Tomorrow
MATISSE VSI GRAVITY
3-20µm, 4 beams 1-2.5µm, 4-6 beams 2.2µm, 4x2 beams
Phase A studies concluded (Sep’07) for 2nd Generation Instruments
PRIMADual-feed facilityStart of integration in Paranal in 2008First scientific use in 2009 TBC
PRIMADual-feed facilityStart of integration in Paranal in 2008First scientific use in 2009 TBC
ConclusionsConclusions
•VLTI is well-developed, open, user-friendly facilityVLTI is well-developed, open, user-friendly facility
•Flexible baseline system gives wide Flexible baseline system gives wide uvuv coverage coverage
•Most powerful combination of long baselines and Most powerful combination of long baselines and large telescopeslarge telescopes
•Standard system of observation, data quality and data Standard system of observation, data quality and data analysisanalysis
•Diverse scientific issues at 0.001” resolutionDiverse scientific issues at 0.001” resolution
•Lively futureLively future