2009ApJ...699.1209F


Query : 2009ApJ...699.1209F

2009ApJ...699.1209F - Astrophys. J., 699, 1209-1222 (2009/July-2)

An analysis of the shapes of interstellar extinction curves. VI. The Near-IR extinction law.

FITZPATRICK E.L. and MASSA D.

Abstract (from CDS):

We combine new observations from the Hubble Space Telescope's Advanced Camera of Survey with existing data to investigate the wavelength dependence of near-IR (NIR) extinction. Previous studies suggest a power law form for NIR extinction, with a "universal" value of the exponent, although some recent observations indicate that significant sight line-to-sight line variability may exist. We show that a power-law model for the NIR extinction provides an excellent fit to most extinction curves, but that the value of the power, β, varies significantly from sight line to sight line. Therefore, it seems that a "universal NIR extinction law" is not possible. Instead, we find that as β decreases, R(V) ≡ A(V)/E(B - V) tends to increase, suggesting that NIR extinction curves which have been considered "peculiar" may, in fact, be typical for different R(V) values. We show that the power-law parameters can depend on the wavelength interval used to derive them, with the β increasing as longer wavelengths are included. This result implies that extrapolating power-law fits to determine R(V) is unreliable. To avoid this problem, we adopt a different functional form for NIR extinction. This new form mimics a power law whose exponent increases with wavelength, has only two free parameters, can fit all of our curves over a longer wavelength baseline and to higher precision, and produces R(V) values which are consistent with independent estimates and commonly used methods for estimating R(V). Furthermore, unlike the power-law model, it gives R(V)s that are independent of the wavelength interval used to derive them. It also suggests that the relation R(V) = -1.36 x E(K-V)/E(B-V) -0.79 can estimate R(V) to ±0.12. Finally, we use model extinction curves to show that our extinction curves are in accord with theoretical expectations, and demonstrate how large samples of observational quantities can provide useful constraints on the grain properties.

Abstract Copyright: ∼

Journal keyword(s): dust, extinction

Simbad objects: 21

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Number of rows : 21
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 BD+56 517 * 02 18 55.7271815616 +57 09 06.625290312 10.26 10.77 10.4410   9.6640 B1.5III 43 0
2 BD+45 973 * 04 43 01.9718619648 +45 37 49.449710388 8.75 9.04 8.63     B3V 26 0
3 BD+44 1080 * 05 02 21.7143311904 +44 16 10.460320212 10.18 9.91 9.29     B5V 31 1
4 BD+52 913 WD* 05 05 30.6180977592 +52 49 51.919301604 10.25 11.44 11.69 11.93 12.108 DA.8 1153 0
5 Brun 885 * 05 35 49.7894957016 -05 40 27.806024892 12.123 12.024 11.477   9.913 F6IV 38 0
6 GD 71 WD* 05 52 27.6198591816 +15 53 13.228887444 11.675 12.783 13.032 13.169 13.337 DA1.5 407 0
7 HD 46106 Y*O 06 31 38.3968383096 +05 01 36.396422796 7.33 8.08 7.93 7.76 7.66 O9.7III(n) 167 0
8 * 15 Mon Be* 06 40 58.65963 +09 53 44.7229 3.360 4.45 4.68   4.88 O7V+B1.5/2V 823 0
9 HD 292167 * 06 44 53.8144895352 +00 37 12.593465724 9.1 9.82 9.63 9.21   A3Ia 52 0
10 HD 68633 ** 08 10 53.1452339928 -51 11 26.083231800   8.19 7.96     B5V 31 0
11 HD 70614 * 08 21 10.2967682064 -42 24 42.401942136   9.66 9.29     B3III 20 0
12 Cl Trumpler 14 27 SB* 10 43 43.8836722848 -59 33 46.270987560 10.979 11.539 11.219 11.13 10.62 B1.5V 41 0
13 Cl Trumpler 14 6 Y*? 10 43 57.5626033368 -59 33 38.648795904 10.616 11.329 11.121   10.663 B1V 40 0
14 GD 153 WD* 12 57 02.3224909560 +22 01 52.634778240 11.883 13.060 13.349 13.488 13.669 DA1.2 380 0
15 * rho Oph ** 16 25 35.11766 -23 26 49.8150 4.30 4.85 4.63 4.27 3.96 B2IV+B2V 670 0
16 NAME Her 36SE Y*O 18 03 40.3201232304 -24 22 42.857540472 10.26 11.022 10.372 10.267   O8V+ 210 0
17 * 9 Sgr Y*O 18 03 52.4450051016 -24 21 38.632254012 5.08 5.97 5.97 5.72 5.70 O4V((f))z 563 0
18 NGC 6530 OpC 18 04 31 -24 21.5           ~ 443 0
19 HD 229196 Pu* 20 23 10.7840350992 +40 52 29.847533160 9.29 9.32 8.59     O6II(f) 123 0
20 HD 204827 SB* 21 28 57.7592315784 +58 44 23.238427956 8.63 8.74 7.94 7.25 6.76 O9.5IV 372 0
21 BD+61 2365 Y*O 22 54 18.0388647744 +62 39 55.135306224 9.27 9.59 9.2     B5 37 0

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