2014ApJ...797...99K


Query : 2014ApJ...797...99K

2014ApJ...797...99K - Astrophys. J., 797, 99 (2014/December-3)

The importance of the magnetic field from an SMA-CSO-combined sample of star-forming regions.

KOCH P.M., TANG Y.-W., HO P.T.P., ZHANG Q., GIRART J.M., CHEN H.-R.V., FRAU P., LI H.-B., LI Z.-Y., LIU H.-Y.B., PADOVANI M., QIU K., YEN H.-W., CHEN H.-H., CHING T.-C., LAI S.-P. and RAO R.

Abstract (from CDS):

Submillimeter dust polarization measurements of a sample of 50 star-forming regions, observed with the Submillimeter Array (SMA) and the Caltech Submillimeter Observatory (CSO) covering parsec-scale clouds to milliparsec-scale cores, are analyzed in order to quantify the magnetic field importance. The magnetic field misalignment δ–the local angle between magnetic field and dust emission gradient–is found to be a prime observable, revealing distinct distributions for sources where the magnetic field is preferentially aligned with or perpendicular to the source minor axis. Source-averaged misalignment angles < |δ| > fall into systematically different ranges, reflecting the different source-magnetic field configurations. Possible bimodal < |δ| > distributions are found for the separate SMA and CSO samples. Combining both samples broadens the distribution with a wide maximum peak at small < |δ| > values. Assuming the 50 sources to be representative, the prevailing source-magnetic field configuration is one that statistically prefers small magnetic field misalignments|δ|. When interpreting|δ| together with a magnetohydrodynamics force equation, as developed in the framework of the polarization-intensity gradient method, a sample-based log-linear scaling fits the magnetic field tension-to-gravity force ratio < ΣB > versus < |δ| > with < ΣB > = 0.116. exp (0.047. < |δ| > )±0.20 (mean error), providing a way to estimate the relative importance of the magnetic field, only based on measurable field misalignments|δ|. The force ratio ΣB discriminates systems that are collapsible on average ( < ΣB > < 1) from other molecular clouds where the magnetic field still provides enough resistance against gravitational collapse ( < ΣB > > 1). The sample-wide trend shows a transition around < |δ| > ~ 45°. Defining an effective gravitational force ∼1 - < ΣB > , the average magnetic-field-reduced star formation efficiency is at least a factor of two smaller than the free-fall efficiency. For about one fourth of the sources the average efficiency drops to zero. The force ratio ΣB can further be linked to the normalized mass-to-flux ratio, yielding an estimate for the latter one without the need of field strength measurements. Across the sample, a transition from magnetically supercritical to subcritcal is observed with growing misalignment < |δ| > .

Abstract Copyright:

Journal keyword(s): ISM: clouds - ISM: magnetic fields - polarization

CDS comments: Sources I18360, IRAS 05327, G34.4.0 and G34.4.1 were not identified.

Simbad objects: 48

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Number of rows : 48
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 NAME W 3 OH HII 02 27 04.1 +61 52 22           ~ 1028 2
2 W 3 MoC 02 27 04.10 +61 52 27.1           ~ 1032 3
3 GAL 240.20-65.50 MoC 02 39 34 -35 43.8           ~ 6 0
4 [JCC87] IRAS 4A Y*O 03 29 10.49 +31 13 30.8           ~ 715 1
5 [JCC87] IRAS 4 FIR 03 29 10.9 +31 13 26           ~ 478 0
6 [JCC87] IRAS 4B Y*O 03 29 12.058 +31 13 02.05           ~ 600 0
7 NAME OMC-1 MoC 05 35 14 -05 22.4           ~ 1170 2
8 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2294 1
9 OMC 3 MoC 05 35 20.0 -05 01 00           ~ 273 1
10 NGC 2024 Cl* 05 41 43 -01 50.5           ~ 1154 1
11 LBS 2-10 PoC 05 46 45.1 +00 00 24           ~ 11 0
12 GAL 192.16-03.82 HII 05 58 13.4 +16 32 00           ~ 143 1
13 NAME Mon R2 HII 06 07 47.58 -06 22 42.6           ~ 742 2
14 GGD 12 HH 06 10 50.6 -06 11 50           ~ 59 1
15 NGC 2264 12 * 06 39 16.0750498224 +09 25 57.487270728   16.76 15.46     ~ 5 0
16 NGC 2264 OpC 06 40 52.1 +09 52 37           ~ 1793 0
17 * rho Oph ** 16 25 35.11766 -23 26 49.8150 4.30 4.85 4.63 4.27 3.96 B2IV+B2V 648 0
18 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1252 1
19 NAME IRAS 16293-2422B Y*O 16 32 22.63 -24 28 31.8           ~ 283 0
20 NAME IRAS 16293-2422A Y*O 16 32 22.869 -24 28 36.11           ~ 167 0
21 NAME NGC 6334 FIR V Cl* 17 19 57 -35 57.5           ~ 95 0
22 NGC 6334A HII 17 20 19.3 -35 54 55           ~ 121 0
23 NAME NGC 6334-I Cl* 17 20 53.35 -35 47 01.5           ~ 342 0
24 NAME NGC 6334 I(N) smm 17 20 54 -35 45.0           ~ 151 1
25 GCM -0.13 -0.08 MoC 17 45 25.2 -29 05 30           ~ 122 1
26 0FGL J1746.0-2900 gam 17 45 41 -29 00.8           ~ 493 2
27 GCM -0.02 -0.07 MoC 17 45 50.4 -28 59 06           ~ 164 0
28 GCM +0.07 -0.08 MoC 17 46 06.2 -28 55 22           ~ 18 0
29 NAME the Brick MoC 17 46 09 -28 43.8           ~ 191 0
30 SNR G000.3+00.0 Rad 17 46 15 -28 38.0           ~ 39 1
31 NAME Sgr B1 MoC 17 47 02.0 -28 31 57           ~ 164 0
32 NAME Sgr B2 MoC 17 47 20.4 -28 23 07           ~ 2266 1
33 RAFGL 2046 HII 18 00 32.1 -24 04 03           ~ 362 0
34 W 33c Rad 18 13 59.0 -17 57 38           ~ 14 0
35 W 33a Y*O 18 14 39.56547 -17 52 02.2260           ~ 698 0
36 NGC 6618 OpC 18 20 47 -16 10.3           ~ 1615 0
37 IRAS 18449-0115 cor 18 47 34.27 -01 12 43.2           ~ 388 0
38 RAFGL 2271 SFR 18 53 18.54 +01 14 57.9           ~ 505 0
39 [DLW84] G35.2N HII 18 58 13.036 +01 40 36.00           ~ 116 0
40 W 49a BL? 19 10 15.7 +09 06 05           ~ 306 2
41 NAME W 51 North Rad 19 23 40.0 +14 30 51           ~ 159 0
42 W 51e2 PCG 19 23 43.906 +14 30 34.48           ~ 211 0
43 W 51e8 HII 19 23 44.2 +14 30 28           ~ 39 0
44 IRAS 20126+4104 Y*O 20 14 25.8816769656 +41 13 36.879427236           B2.5-B0.5 441 0
45 DR 21 (OH) cor 20 39 01.01 +42 22 50.2           ~ 410 0
46 DR 21 SFR 20 39 01.6 +42 19 38           O4.5 1055 0
47 NAME LDN 1157-mm Y*O 20 39 06.2 +68 02 15           ~ 189 0
48 NAME Gould Belt PoG ~ ~           ~ 874 1

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