Journal
ASTROPHYSICAL JOURNAL LETTERS
Volume 693, Issue 2, Pages L81-L85Publisher
IOP PUBLISHING LTD
DOI: 10.1088/0004-637X/693/2/L81
Keywords
infrared: stars; ISM: clouds; stars: formation
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Funding
- NASA [1257184]
- JPL/Caltech, JPL [960803]
- University of Rochester [31419-5714]
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Using Spitzer Infrared Spectrograph observations of G0-M4 III stars behind dark clouds, I construct 5-20 mu m empirical extinction curves for 0.3 <= A(K) < 7, which is equivalent to A(V) between approximate to 3 and 50. For A(K) < 1, the curve appears similar to the Mathis diffuse interstellar medium extinction curve, but with a greater degree of extinction. For A(K) > 1, the curve exhibits lower contrast between the silicate and absorption continuum, develops ice absorption, and lies closer to the Weingartner and Draine R-V = 5.5 Case B curve, a result which is consistent with that of Flaherty et al. and Chiar et al. Recently, work using Spitzer Infrared Array Camera data by Chapman et al. independently reaches a similar conclusion that the shape of the extinction curve changes as a function of increasing A(K). By calculating the optical depths of the 9.7 mu m silicate and 6.0, 6.8, and 15.2 mu m ice features, I determine that a process involving ice is responsible for the changing shape of the extinction curve and speculate that this process is a coagulation of ice-mantled grains rather than ice-mantled grains alone.
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