1 / 16

The circumstellar environment of evolved stars as seen by VLTI / MIDI

The circumstellar environment of evolved stars as seen by VLTI / MIDI. Keiichi Ohnaka Max-Planck-Institut für Radioastronomie, Infrared Interferometry Group kohnaka@mpifr-bonn.mpg.de. Carbon star, IRC+10216. AGB, AFGL2290. Asymptotic Giant Branch (AGB). Post-AGB Red Rectangle.

emi-mann
Download Presentation

The circumstellar environment of evolved stars as seen by VLTI / MIDI

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. The circumstellar environment of evolved stars as seen by VLTI / MIDI Keiichi Ohnaka Max-Planck-Institut für Radioastronomie, Infrared Interferometry Group kohnaka@mpifr-bonn.mpg.de

  2. Carbon star, IRC+10216 AGB, AFGL2290 Asymptotic Giant Branch (AGB) Post-AGB Red Rectangle Teff ~ 3000K L ~ 104 L8 Mass loss ~10-8—10-5 M8/yr Mass loss mechanism The structure of the outer atmosphere: Molecule & dust formation Morphology from AGB to Planetary Nebulae PN, Cat’s Eye Nebula

  3. AMBER MIDI What can interferometry do to study AGB stars? Mira variables: Large variability amplitude ~ 9 mag (in V) Expanding dust shell Outer atmosphere Molecular layers Dust formation Mid-infrared Near-infrared

  4. Infrared long-baseline interferometry Spatial resolution = l/Bp N band Bp= 200m  10mas What’s observed: Visibility, not an image! Bp Visibility = Amplitude of the (complex) Fourier transform of the object’s intensity = Fringe contrast B MIDI AMBER Point source  V = 1 Extended source  V < 1 Larger size  lower V It “contains” information on the angular size and shape Is it useful? Yes, especially with spectral resolution!

  5. MIDI: first fringe in December 2002 Open to the community since April 2004 N band: 8 – 13 mm (dust features, molecular bands) Spectral resolution: 30 / 230 Sensitivity @ 10mm: 1 Jy / 10 Jy VLTI Interferometric Laboratory

  6. MIDI observation of the Mira variable RR Sco 2003 June, Science Demonstration Time Unit Telescopes 1 & 3 (8m) Projected baseline = 74—100m Angular resolution @ 10mm = ~20mas RR Sco (Phase = 0.6 in 2003 June) P = 284 days, d = 320 pc (Hipparcos) Dust emission not strong  Good for studying the molecular layers UT3 UT1 102m

  7. MIDI observation of RR Sco: spectrally dispersed fringes 7.5 mm 13.3 mm

  8. Observed N-band visibility of RR Sco • Visibility increases from 8 to 10 mm, constant l > 10 mm • UD diameter constant between 8 and 10 mm (~18 mas), UD diameter increases l > 10 mm (~25 mas @ 13 mm) • N-band UD diameter (MIDI) twice as large as that in the K band • (VINCI, 3 weeks later) Why?

  9. Observed N-band visibility of RR Sco

  10. K band (2—2.4mm) No dust emission N band (8—13mm) Basic idea Optically thick emission from H2O (pure rotation) + SiO (fundamental) gas + Dust emission Expanding dust shell H2O + SiO gas  Angular size larger Modeling H2O + SiO layer (constant temperature, column densities, radius) Optically thin dust shell (silicate+corundum) (Inner radius, optical depth) H2O + CO bands Not optically thick  Angular size smaller  Ohnaka et al. 2005, A&A, 429, 1067

  11. T = 1400 K N(H2O) = 3 x 1021cm-2 N(SiO) = 1 x 1020cm-2 R = 2.3 Rstar Dust emission (silicate 20% + corundum 80%) Tin ~ 700 K, Rin = 7--8 Rstar H2O+SiO emission t= 0.2 – 0.3 (V band), 0.025 (10mm) • Comparison with pulsation models is ongoing

  12. MIDI observation of the silicate carbon star Hen 38 Silicate carbon star : carbon-rich photosphere, oxygen-rich circumstellar dust Usually… carbon star, carbon-rich circumstellar dust (amorphous carbon, SiC) M giants (O-rich), oxygen-rich circumstellar dust (silicate, Al2O3: corundum) How can silicate (O-bearing dust) exist around a carbon star?

  13. AGB star + main sequence star AGB, primary star: oxygen-rich, mass loss  Circumbinary disk is formed Oxygen-rich dust (silicate) reservoir Mass loss Primary star becomes a carbon star. Oxygen-rich dust is stored in the disk  Silicate carbon star High-resolution observation in the silicate emission feature is the most direct approach VLTI/MIDI

  14. Compact silicate disk + extended corundum disk Silicate Compact disk Corundum (Al2O3) • Only present in the outer region • Increase of the angular size l > 10 mm

  15. Silicate + corundum disk model Corundum dominant Silicate torus (ring) dominant 15 – 35 Rstar, t(10mm) = 1.5 > 35 Rstar, t(10mm) = 0.4

  16. Concluding remarks First “spectro-interferometric” observation of RR Sco  Wavelength dependence of the angular size Angular size constant between 8 and 10 mm, increases longward of 10 mm, More than twice as large as in the K-band Observed N-band visibilities and spectra can be explained by optically thick emission from H2O + SiO gas & dust emission  Consistent with ISO and previous results Potential to probe the circumstellar environment (molecule and dust) with spatial and spectral information disentangled  Totally new picture of the circumstellar environment Upcoming: more Miras (oxygen-rich, carbon-rich, S-type), Circumstellar dust disks around (post-)AGB stars, Symbiotic stars (Mira + hot companion), etc…

More Related