2024MNRAS.529.1715B


Query : 2024MNRAS.529.1715B

2024MNRAS.529.1715B - Mon. Not. R. Astron. Soc., 529, 1715-1722 (2024/April-1)

Magnetic field alignment in low-mass molecular clouds: the role of turbulence and density of the clouds.

BARMAN B. and DAS H.S.

Abstract (from CDS):

In this work, we report the role of turbulence (measured by the $^{12}\mathrm{ CO}$ linewidth, $\Delta V$) on the offset between the orientation of local magnetic field in the low-density regions of dark clouds ($\theta ^{\mathrm{ env}}_\mathrm{ B}$) and the position angle of the Galactic Plane (GP; $\theta _{\mathrm{ GP}}$) in 15 low-mass isolated molecular clouds. We find a dependency of $\Delta V$ on offset, ($\theta _{\mathrm{ off}} =|\theta ^{\mathrm{ env}}_\mathrm{ B}-\theta _{\mathrm{ GP}}|$), represented by a second-order polynomial equation, $\theta _{\mathrm{ off}}=(3.328 \pm 1.187) {\Delta V}^2 - (0.991 \pm 5.541) {\Delta V} + (4.767 \pm 5.309)$. In regions where the majority of low turbulence is observed, characterized by $\Delta V \ \lt\ 3.1 \ \mathrm{ km\,s}^{-1}$, the envelope magnetic fields closely align with the orientation of the GP ($\theta _{\mathrm{ off}}\ \lt\ 20^\circ$). Conversely, in areas exhibiting high turbulence with $\Delta V \ \gt\ 3.1 \ \mathrm{ km\,s}^{-1}$ (for clouds CB130 and CB188), the envelope magnetic field tends to misalign with the GP ($\theta _{\mathrm{ off}}\ \gt\ 50^\circ$). This suggests that turbulence could be one of the important factors influencing the alignment of the local magnetic field with the GP. We have also explored the potential link between gas density of clouds ($\rho$) and turbulence ($\Delta V$) for the first time, utilizing data from 10 isolated clouds. This analysis suggests a possible correlation, with the observed trend quantified as, $\Delta V \propto \rho ^{-0.19}$.

Abstract Copyright: © 2024 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): polarization - turbulence - ISM: magnetic fields - galaxies: magnetic fields

Simbad objects: 34

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Number of rows : 34
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 LBN 119.83-06.05 MoC 00 28 43.5075 +56 41 56.868           ~ 72 0
2 [DB2002b] G121.03-9.97 MoC 00 39 03 +52 51.5           ~ 23 0
3 LDN 1389 MoC 04 04 38 +56 56.2           ~ 99 0
4 LDN 1498 DNe 04 11.0 +24 58           ~ 306 0
5 LDN 1495 DNe 04 18.1 +27 37           ~ 408 1
6 LDN 1506 DNe 04 20.0 +25 17           ~ 81 0
7 LDN 1415 DNe 04 42.0 +54 26           ~ 15 0
8 [DB2002b] G155.76+5.91 MoC 04 58 30 +52 15.7           ~ 45 0
9 LDN 1437 DNe 04 59 04.1 +52 03 24           ~ 24 0
10 LDN 1439 DNe 05 00 09 +52 04.9           ~ 103 0
11 LDN 1512 MoC 05 04 09.7 +32 43 09           ~ 184 0
12 NAME Ori B MoC 05 41 43.0 -01 54 44           ~ 1498 0
13 [CB88] 34 MoC 05 47 02.3 +21 00 10           ~ 64 0
14 [DB2002b] G192.63-3.05 MoC 06 02 00 +16 31.0           ~ 29 0
15 LDN 1570 DNe 06 07 28.4 +19 28 04           ~ 46 0
16 [DB2002b] G227.77-8.20 MoC 06 48 43 -16 53.4           ~ 20 0
17 LBN 1042 HII 07 04 17 -16 24.5           ~ 11 0
18 [CB88] 54 MoC 07 04 21.2170 -16 23 15.000           ~ 53 0
19 NGC 2345 OpC 07 08 21.4 -13 11 44   8.58 7.7     ~ 92 0
20 [DB2002b] G237.93-6.46 MoC 07 14 36 -25 08.9           ~ 11 0
21 [DB2002b] G236.96-5.04 MoC 07 18 13 -23 38.8           ~ 16 0
22 LDN 1670 MoC 08 04 36.9 -31 30 44           ~ 17 0
23 [CB88] 62 MoC 13 34 46 +79 53.4           ~ 8 0
24 LDN 1755 DNe 16 43.5 -21 58           ~ 37 0
25 LDN 146 MoC 16 57 17.5 -16 09 18           ~ 89 1
26 [DB2002b] G351.19+5.20 MoC 17 02 20 -33 16.6           ~ 12 0
27 LDN 507 MoC 18 16 15 -02 32.8           ~ 32 0
28 LDN 594 DNe 19 00.6 -01 46           ~ 6 0
29 [CB88] 188 cor 19 20 15.6 +11 36 15           ~ 37 0
30 LDN 663 DNe 19 36 55 +07 34.4           ~ 698 0
31 LDN 1177 DNe 21 17 38.62 +68 17 34.0           ~ 95 1
32 LDN 1225 DNe 23 11 58 +61 39.0           ~ 15 0
33 LDN 1262 MoC 23 25 47 +74 17.6           ~ 136 0
34 LDN 1253 DNe 23 56 32 +58 31.7           ~ 56 0

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