2002ApJ...572..238C


Query : 2002ApJ...572..238C

2002ApJ...572..238C - Astrophys. J., 572, 238-263 (2002/June-2)

Dense cores in dark clouds. XIV. N2H+ (1-0) maps of dense cloud cores.

CASELLI P., BENSON P.J., MYERS P.C. and TAFALLA M.

Abstract (from CDS):

We present results of an extensive mapping survey of N2H+ (1-0) in about 60 low-mass cloud cores already mapped in the NH3 (1, 1) inversion transition line. The survey has been carried out at the FCRAO antenna with an angular resolution of 54", about 1.5 times finer than the previous ammonia observations made at the Haystack telescope. The comparison between N2H+ and NH3 maps shows strong similarities in the size and morphology of the two molecular species, indicating that they are tracing the same material, especially in starless cores. Cores with stars typically have map sizes about a factor of 2 smaller for N2H+ than for NH3, indicating the presence of denser and more centrally concentrated gas compared to starless cores. The mean aspect ratio is ∼2. Significant correlations are found between NH3 and N2H+ column densities and excitation temperatures in starless cores, but not in cores with stars, suggesting a different chemical evolution of the two species. Starless cores are less massive (Mvir≃3 M) than cores with stars (Mvir≃9 M). Velocity gradients range between 0.5 and 6 km.s–1.pc–1, similar to what has been found with NH3 data, and the ratio β of rotational kinetic energy to gravitational energy has magnitudes between ∼10–4 and 0.07, indicating that rotation is not energetically dominant in the support of the cores. ``Local'' velocity gradients show significant variation in both magnitude and direction, suggesting the presence of complex motions not interpretable as simple solid-body rotation. Integrated intensity profiles of starless cores present a ``central flattening'' and are consistent with a spherically symmetric density law n∝r–α, where α=1.2 for r<rbreak and α=2 for r>rbreak, with rbreak∼0.03 pc. Cores with stars are better modeled with single density power laws with α≥2, in agreement with observations of submillimeter continuum emission. Line widths change across the core, but we did not find a general trend: there are cores with significant positive as well as negative linear correlations between Δv and the impact parameter b. The deviation in line width correlates with the mean line width, suggesting that the line of sight contains ∼10 coherence lengths. The corresponding value of the coherence length, ∼0.01 pc, is similar to the expected cutoff wavelength for MHD waves. This similarity may account for the increased ``coherence'' of line widths on small scales. Despite finer angular resolution, the majority of N2H+ and NH3 maps show a similar ``simple'' structure, with single peaks and no elongation.

Abstract Copyright:

Journal keyword(s): ISM: Clouds - ISM: Molecules - ISM: Structure - Molecular Data - Radio Lines: ISM

Nomenclature: Table 1: [LMG94] Per 4A (Nos 4A, 4B, 4C) added.

Simbad objects: 68

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Number of rows : 68
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 [LMG94] Per 4C PoC 03 29 15.7 +31 28 21           ~ 2 0
2 [LMG94] Per 4 PoC 03 29 18.0 +31 27 31           ~ 10 0
3 SCOPE G158.19-20.25 cor 03 29 23.3 +31 36 08           ~ 10 0
4 SSTc2d J032923.5+313330 Y*O 03 29 23.47 +31 33 29.5           ~ 39 1
5 IRAS 03267+3128 cor 03 29 51.82 +31 39 06.0           ~ 55 0
6 [LMG94] Per 6 PoC 03 30 14.9 +30 22 48           ~ 13 0
7 [LMG94] Per 7 PoC 03 32 45.1 +30 59 56           ~ 10 0
8 [LMG94] Per 9 PoC 03 33 16.5 +31 20 18           ~ 6 0
9 NAME [BM89] B5 DNe 03 47 38.3 +32 52 43           ~ 223 0
10 LDN 1471 DNe 03 48.0 +32 54           ~ 329 0
11 LDN 1389 MoC 04 04 38 +56 56.2           ~ 92 0
12 LDN 1489 DNe 04 04 47.5 +26 19 42           ~ 228 0
13 LDN 1400K DNe 04 10 48.6 +54 53 14           ~ 32 0
14 NAME [BM89] L1498 PoC 04 10 51.4 +25 09 58           ~ 187 0
15 LDN 1498 DNe 04 11.0 +24 58           ~ 286 0
16 NAME [BM89] L1495 PoC 04 14 08.2 +28 09 31           ~ 170 0
17 LDN 1495 DNe 04 18.1 +27 37           ~ 366 1
18 LDN 1400G DNe 04 25 10.5 +54 19 11           ~ 22 0
19 Barnard 217 DNe 04 27 46.5 +26 17 52           ~ 89 0
20 LDN 1524 DNe 04 27 57.7 +24 39 18           ~ 83 0
21 JCMTSF J043155.5+243254 PoC 04 31 55.9 +24 32 49           ~ 42 0
22 NAME Kutner's Cloud MoC 04 32 44.6 +24 23 13           ~ 273 0
23 NAME [BM89] TMC-2 PoC 04 32 44.7 +24 25 13           ~ 186 0
24 LDN 1536 DNe 04 33 24.6 +22 43 29           ~ 111 0
25 LDN 1527 DNe 04 39 53 +25 45.0           ~ 635 0
26 TMC-1 NH3 PoC 04 41 18.5 +25 48 14           ~ 19 0
27 TMC-1 C2 PoC 04 41 29.8 +26 01 43           ~ 1 0
28 Barnard 220 DNe 04 41 38.8 +26 00 42           ~ 137 0
29 LDN 1534 DNe 04 41 46 +25 41.4           ~ 45 0
30 NAME [BM89] L1517B cor 04 55 18.8 +30 38 04           ~ 147 0
31 LDN 1512 MoC 05 04 09.7 +32 43 09           ~ 175 0
32 LDN 1544 DNe 05 04 16.6 +25 10 48           ~ 863 0
33 NAME [BM89] L1544 cor 05 04 22.5 +25 11 36           ~ 437 1
34 NAME [BM89] L1582A DNe 05 31 18.4 +12 30 31           ~ 33 0
35 Barnard 35 DNe 05 45.5 +09 03           ~ 59 0
36 LDN 134A DNe 15 53 36.4 -04 35 26           ~ 49 0
37 LDN 183 MoC 15 54 12.2 -02 49 42           ~ 759 1
38 LDN 1681B DNe 16 27 35.7 -24 43 26           ~ 27 0
39 NAME Ophiuchus D MoC 16 28 29.2 -24 18 25           ~ 117 0
40 LDN 43 DNe 16 34 29.3 -15 47 11           ~ 142 1
41 LDN 260 DNe 16 46 58.2 -09 36 20           ~ 43 0
42 LDN 158 DNe 16 47 50 -14 05.3           ~ 33 0
43 LDN 234E DNe 16 48 04.5 -10 56 58           ~ 26 0
44 LDN 234A DNe 16 48 06.9 -10 51 48           ~ 23 0
45 LDN 63 DNe 16 50 15.5 -18 06 06           ~ 76 0
46 LDN 57 DNe 17 22 38.2 -23 49 34           ~ 314 1
47 LDN 483 DNe 18 17 35 -04 39.8           ~ 315 0
48 LDN 531 DNe 19 06 10.0 -06 53 45           ~ 66 0
49 LDN 778 DNe 19 26 32.5 +23 58 42           ~ 51 1
50 LDN 663 DNe 19 36 55 +07 34.4           ~ 646 0
51 LDN 1152 DNe 20 35 50.2 +67 54 22           ~ 73 0
52 LDN 1155C DNe 20 43 18.1 +67 50 36           ~ 30 0
53 NAME [BM89] L1082C DNe 20 51 27.4 +60 19 00           ~ 33 0
54 LDN 1082A DNe 20 53 29.6 +60 14 40           ~ 42 1
55 IRAS 20582+7724 Y*O 20 57 12.9250225656 +77 35 43.656301932           ~ 117 0
56 LDN 1228 DNe 20 57 13 +77 35.8           ~ 128 0
57 RNO 129 Y*O 20 59 14.08512 +78 23 04.0020       15.30   G:e 47 1
58 LDN 1174 DNe 21 00 22.4 +68 12 53           ~ 65 0
59 LDN 1172A DNe 21 02 27.7 +67 54 08           ~ 24 0
60 LDN 970 DNe 21 12 13.1 +47 23 23           ~ 67 0
61 LDN 1031C DNe 21 46 17.7 +47 18 54           ~ 7 0
62 LDN 1031B DNe 21 47 25.7 +47 32 09           ~ 22 0
63 LDN 1221 DNe 22 28 02.9 +69 01 13           ~ 50 0
64 LDN 1251A DNe 22 30 31.8 +75 14 17           ~ 75 2
65 LDN 1251C DNe 22 35 40.0 +75 18 06           ~ 22 1
66 LDN 1251E DNe 22 39 18.3 +75 14 31           ~ 18 0
67 LDN 1262 MoC 23 25 47 +74 17.6           ~ 134 0
68 TMC-1 CS PoC ~ ~           ~ 1 0

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