2002ApJ...569..815T


Query : 2002ApJ...569..815T

2002ApJ...569..815T - Astrophys. J., 569, 815-835 (2002/April-3)

Systematic molecular differentiation in starless cores.

TAFALLA M., MYERS P.C., CASELLI P., WALMSLEY C.M. and COMITO C.

Abstract (from CDS):

We present evidence that low-mass starless cores, the simplest units of star formation, are systematically differentiated in their chemical composition. Some molecules, including CO and CS, almost vanish near the core centers, where the abundance decreases by at least 1 or 2 orders of magnitude with respect to the value in the outer core. At the same time, the N2H+ molecule has a constant abundance, and the fraction of NH3 increases toward the core center. Our conclusions are based on a systematic study of five mostly round starless cores (L1498, L1495, L1400K, L1517B, and L1544), which we have mapped in C18O (1-0), CS (2-1), N2H+ (1-0), NH3 (1, 1) and (2, 2), and the 1.2 mm continuum [complemented with C17O (1-0) and C34S (2-1) data for some systems]. For each core we have built a spherically symmetric model in which the density is derived from the 1.2 mm continuum, the kinetic temperature is derived from NH3, and the abundance of each molecule is derived using a Monte Carlo radiative transfer code, which simultaneously fits the shape of the central spectrum and the radial profile of integrated intensity. Regarding the cores for which we have C17O (1-0) and C34S (2-1) data, the model fits these observations automatically when the standard isotopomer ratio is assumed. As a result of this modeling, we also find that the gas kinetic temperature in each core is constant at approximately 10 K. In agreement with previous work, we find that if the dust temperature is also constant, then the density profiles are centrally flattened, and we can model them with a single analytic expression. We also find that for each core the turbulent line width seems constant in the inner 0.1 pc. The very strong abundance drop of CO and CS toward the center of each core is naturally explained by the depletion of these molecules onto dust grains at densities of (2-6)x104 cm–3. N2H+ seems unaffected by this process up to densities of several times 105 cm–3, or even 106 cm–3, while the NH3 abundance may be enhanced by its lack of depletion and by reactions triggered by the disappearance of CO from the gas phase. With the help of the Monte Carlo modeling, we show that chemical differentiation automatically explains the discrepancy between the sizes of CS and NH3 maps, a problem that has remained unexplained for more than a decade. Our models, in addition, show that a combination of radiative transfer effects can give rise to the previously observed discrepancy in the line width of these two tracers. Although this discrepancy has been traditionally interpreted as resulting from a systematic increase of the turbulent line width with radius, our models show that it can arise in conditions of constant gas turbulence.

Abstract Copyright:

Journal keyword(s): ISM: Abundances - ISM: Clouds - ISM: Molecules - Stars: Formation

Simbad objects: 18

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Number of rows : 18
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 LDN 1400K DNe 04 10 48.6 +54 53 14           ~ 32 0
2 NAME [BM89] L1498 PoC 04 10 51.4 +25 09 58           ~ 187 0
3 LDN 1498 DNe 04 11.0 +24 58           ~ 286 0
4 NAME [BM89] L1495 PoC 04 14 08.2 +28 09 31           ~ 170 0
5 V* CW Tau TT* 04 14 17.0042670144 +28 10 57.766508508 13.92 13.64 12.36 12.86   K0Ve 355 0
6 LDN 1495 DNe 04 18.1 +27 37           ~ 366 1
7 LDN 1551 DNe 04 31 30.0 +18 12 30           ~ 805 1
8 TMC-1 MoC 04 41 45.9 +25 41 27           ~ 1674 0
9 NAME [BM89] L1517B cor 04 55 18.8 +30 38 04           ~ 147 0
10 LDN 1512 MoC 05 04 09.7 +32 43 09           ~ 174 0
11 LDN 1544 DNe 05 04 16.6 +25 10 48           ~ 862 0
12 NAME [BM89] L1544 cor 05 04 22.5 +25 11 36           ~ 437 1
13 LDN 183 MoC 15 54 12.2 -02 49 42           ~ 759 1
14 LDN 1689B DNe 16 34 42.1 -24 36 11           ~ 167 0
15 LDN 977 DNe 21 39.0 +43 14           ~ 38 0
16 IC 5146 OpC 21 53 29.3 +47 14 46           ~ 466 2
17 SH 2-140 OpC 22 19 07.8 +63 17 07           ~ 658 2
18 IRAS 22176+6303 Y*O 22 19 18.23 +63 18 47.5           ~ 595 0

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