2002ApJ...575..337S


Query : 2002ApJ...575..337S

2002ApJ...575..337S - Astrophys. J., 575, 337-353 (2002/August-2)

Tracing the mass during low-mass star formation. III. Models of the submillimeter dust continuum emission from class 0 protostars.

SHIRLEY Y.L., EVANS II N.J. and RAWLINGS J.M.C.

Abstract (from CDS):

Seven Class 0 sources mapped with SCUBA at 850 and 450 µm are modeled using a one-dimensional radiative transfer code. The modeling takes into account heating from an internal protostar, heating from the interstellar radiation field (ISRF), realistic beam effects, and chopping to model the normalized intensity profile and spectral energy distribution. Power-law density models, n(r)∝r–p, fit all of the sources; best-fit values are mostly p=1.8±0.1, but two sources with aspherical emission contours have lower values (p∼1.1). Including all sources, <p≥1.63±0.33. Based on studies of the sensitivity of the best-fit p to variations in other input parameters, uncertainties in p for an envelope model are Δp=±0.2. If an unresolved source (e.g., a disk) contributes 70% of the flux at the peak, p is lowered in this extreme case and Δp=+0.2–0.6. The models allow a determination of the internal luminosity (<Lint≥4.0 L☉) of the central protostar as well as a characteristic dust temperature for mass determination (<Tiso≥13.8±2.4 K). We find that heating from the ISRF strongly affects the shape of the dust temperature profile and the normalized intensity profile, but it does not contribute strongly to the overall bolometric luminosity of Class 0 sources. There is little evidence for variation in the dust opacity as a function of distance from the central source. The data are well fitted by dust opacities for coagulated dust grains with ice mantles (Ossenkopf & Henning). The density profile from an inside-out collapse model (Shu) does not fit the data well, unless the infall radius is set so small as to make the density nearly a power law.

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Journal keyword(s): ISM: Dust, Extinction - ISM: Clouds - ISM: Individual: Alphanumeric: B228 - ISM: Individual: Alphanumeric: B335 - ISM: Individual: Alphanumeric: IRAS 03282+3035 - ISM: Individual: Alphanumeric: L483 - ISM: Individual: Alphanumeric: L723 - ISM: Individual: Alphanumeric: L1448C - ISM: Individual: Alphanumeric: L1527 - Stars: Formation

Simbad objects: 26

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Number of rows : 26
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 LDN 1448NW Y*O 03 25 35.66 +30 45 34.2           ~ 80 0
2 JCMTSE J032536.1+304514 Y*O 03 25 36.22 +30 45 15.7           ~ 145 0
3 LDN 1448NA smm 03 25 36.49 +30 45 22.2           ~ 193 1
4 SSTc2d J032536.4+304522 Y*O 03 25 36.49 +30 45 22.2           ~ 208 1
5 IRAS 03225+3034 IR 03 25 36.49 +30 45 22.2           ~ 165 1
6 [SDA2014] West4 Y*O 03 25 38.83 +30 44 06.2           ~ 266 1
7 IRAS F03226+3033 Y*O 03 25 38.83 +30 44 06.2           ~ 371 0
8 IRAS 03282+3035 cor 03 31 20.98 +30 45 30.1           ~ 186 0
9 NAME Perseus Cloud SFR 03 35.0 +31 13           ~ 1553 0
10 LDN 1527 DNe 04 39 53 +25 45.0           ~ 689 0
11 IRAS 04368+2557 Y*O 04 39 53.97816 +26 03 09.6804           ~ 309 0
12 NAME Taurus Complex SFR 04 41.0 +25 52           ~ 4971 0
13 RAFGL 618 pA* 04 42 53.6242032600 +36 06 53.400902220   16.32   12.59   C-rich 1027 0
14 LDN 1512 MoC 05 04 09.7 +32 43 09           ~ 184 0
15 LDN 1544 DNe 05 04 16.6 +25 10 48           ~ 965 0
16 NAME [BM89] L1544 cor 05 04 22.5 +25 11 36           ~ 437 1
17 Barnard 228 cor 15 43 00.9 -34 08 48           ~ 70 0
18 IRAS 15398-3359 Y*? 15 43 02.21016 -34 09 07.7112       18.38 21.72 ~ 215 0
19 NAME Upper Sco-Cen As* 16 15 -24.2           ~ 1497 1
20 LDN 1689B DNe 16 34 42.1 -24 36 11           ~ 181 0
21 IRAS 18148-0440 Y*O 18 17 29.94 -04 39 39.3           ~ 97 0
22 LDN 483 DNe 18 17 35 -04 39.8           ~ 359 0
23 [S2009] L723 XMM 8 * 19 17 53.1327617040 +19 12 16.426495764           ~ 39 0
24 LDN 723 DNe 19 18 12 +19 13.6           ~ 155 0
25 LDN 663 DNe 19 36 55 +07 34.4           ~ 698 0
26 IRAS 19345+0727 cor 19 37 00.7 +07 34 08           ~ 96 0

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