Variation of the 9.7 µm Silicate Absorption Feature with Extinction in the Dense Interstellar Medium Megan M. Bagley with Dr. Jean E. Chiar, SETI Institute.

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Presentation transcript:

Variation of the 9.7 µm Silicate Absorption Feature with Extinction in the Dense Interstellar Medium Megan M. Bagley with Dr. Jean E. Chiar, SETI Institute Senior Honor Presentation a.k.a. Dust in Space

Dust in the Interstellar Medium Between stars, there is the interstellar medium (ISM), made up of gas and dust. Dust in the ISM blocks the light from distant bright objects. Extinction is the amount of light absorbed at a given wavelength.

Dust in the Interstellar Medium Between stars, there is the interstellar medium (ISM), made up of gas and dust. Dust in the ISM blocks the light from distant bright objects. Extinction is the amount of light absorbed at a given wavelength.

Silicates Along with hydrocarbons, silicates are one of the main components of interstellar dust. Silicates produce infrared absorption features at 9.7 and 20 μm. Some Earth silicates

Diffuse versus Dense ISM Near-infrared color excess traces the carbonaceous dust. Diffuse ISM Dense Clouds The maximum absorption at 9.7 μm gives the strength of the silicate feature. In the diffuse ISM, the dust is well-mixed, but in the dense ISM, grains may be coagulating.

The Spitzer Space Telescope Infrared observations from the ground are limited by atmospheric absorption. Spitzer’s unprecedented sensitivity allows us to observe stars behind very dense clouds. The Infrared Spectrograph (IRS) captures spectra from μm.

The Pipe Nebula

Purpose: Study the 9.7 μm silicate feature in dense cloud cores and surrounding lower-density medium in the Pipe Nebula.

Reduced Spectra: What I Started With

Fitting Stellar Photosphere Models Why fit models of starlight? – To remove the characteristics of the background source from the spectrum we study. Parameters to fit: – Spectral type – A v (visual extinction) – Extinction law (converts A V into extinction at infrared wavelengths).

Fitting Stellar Photosphere Models

Examples of Optical Depth Profiles

Absorption by Water Ice The absorption by water ice at 12 μm can affect the long- wavelength side of the silicate feature, so the water ice contribution was subtracted. CO N2N2 CO 2 O2O2 NH 3 H2OH2O CH 3 OH CO 2 Silicate core

Absorption by Water Ice The absorption by water ice at 12 μm can affect the long- wavelength side of the silicate feature, so the water ice contribution was subtracted.

Estimating τ 9.7 τ 9.7 is the maximum optical depth of the silicate feature. τ = -ln (observed flux / model continuum flux)

Optical Depth versus Extinction Diffuse ISM Pipe Nebula

Changes in the Silicate Absorption Profile

Conclusions Thus far, we see what is expected: the tight relationship between τ 9.7 and extinction that is seen in the diffuse ISM breaks down at higher values of extinction in dense clouds. We also see changes in the shape of the silicate absorption profile in dense clouds. These indicate changes in dust properties, particularly due to grain coagulation.

Future Work We will be getting observations of 1-5 µm spectra on the Very Large Telescope in Chile.

Image Credits Slide 1: Gleason, John, & Mandel, Steve. "Rho Ophiuchi and the Pipe Nebula.” Slide 2: Kuznetov, Andrey. “The Chameleon’s Dark Nebulae.” Astronomy Picture of the Day, 15 July Slide 4: Weller, R. “Olivine Photos.” Cochise College, Mattox, Steve. “Common Minerals in Volcanic Rocks.” Slide 6: NASA/JPL. “Infrared View of Spitzer.” Slide 7: Betelsky, Yuri. “The Pipe Nebula.” Slide 10: "Red Giants.” Slide 16: Slide 21: Wright, E. L. “Fractal Dust Grains.” 10 May Slide 22: "The VLT Platform at Paranal.” 21 Jan

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