2025MNRAS.536.1736P


Query : 2025MNRAS.536.1736P

2025MNRAS.536.1736P - Mon. Not. R. Astron. Soc., 536, 1736-1751 (2025/January-2)

The JCMT BISTRO Survey: the magnetized evolution of star-forming cores in the Ophiuchus molecular cloud interpreted using histograms of relative orientation.

PERRY J.P., PATTLE K., JOHNSTONE D., KWON W., BOURKE T.L., CHUNG E.J., COUDE S., DOI Y., FANCIULLO L., HWANG J., KHAN Z.A., KWON J., LAI S.-P., LE GOUELLEC V.J.M., LEE C.W., OHASHI N., SADAVOY S., SAVINI G., SHARMA E. and TAMURA M.

Abstract (from CDS):

The relationship between B-field orientation and density structure in molecular clouds is often assessed using the histogram of relative orientations (HRO). We perform a plane-of-the-sky geometrical analysis of projected B-fields, by interpreting HROs in dense, spheroidal, pre-stellar, and protostellar cores. We use James Clerk Maxwell Telescope POL-2 850 $\mu$m polarization maps and Herschel column density maps to study dense cores in the Ophiuchus molecular cloud complex. We construct two-dimensional core models, assuming Plummer column density profiles and modelling both linear and hourglass B-fields. We find that high-aspect ratio ellipsoidal cores produce strong HRO signals, as measured using the shape parameter $\xi$. Cores with linear fields oriented $<\!\! 45 ^{\circ }$ from their minor axis produce constant HROs with $-1 \lt \xi \lt 0$, indicating that fields are preferentially parallel to column density gradients. Fields parallel to the core minor axis produce the most negative value of $\xi$. For low-aspect ratio cores, $\xi \approx 0$ for linear fields. Hourglass fields produce a minimum in $\xi$ at intermediate densities in all cases, converging to the minor-axis-parallel linear field value at high and low column densities. We create HROs for six dense cores in Ophiuchus. $\rho$ Oph A and IRAS 16293 have high aspect ratios and preferentially negative HROs, consistent with moderately strong field behaviour. $\rho$ Oph C, L1689A, and L1689B have low aspect ratios, and $\xi \approx 0$. $\rho$ Oph B is too complex to be modelled using a simple spheroidal field geometry. We see no signature of hourglass fields, agreeing with previous findings that dense cores generally exhibit linear fields on these size scales.

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

Journal keyword(s): techniques: polarimetric - stars: formation - ISM: clouds - ISM: magnetic fields - ISM: structure

Simbad objects: 15

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Number of rows : 15
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 HD 147889 Or* 16 25 24.3163637976 -24 27 56.569805208 8.56 8.73 7.90     B2V 512 1
2 NAME rho Oph A Cloud MoC 16 26 26.4 -24 22 33           ~ 312 1
3 NAME VLA 1623-243 Y*O 16 26 26.42 -24 24 30.0           ~ 429 0
4 HGBS J162627.6-242359 cor 16 26 27.60 -24 23 55.0           ~ 75 0
5 GSS 35 TT* 16 26 34.1761719864 -24 23 28.283473860     16.53 14.75 12.51 B3 254 1
6 NAME rho Oph C Cloud MoC 16 26 53.1 -24 32 31           ~ 80 0
7 NAME rho Oph B Cloud MoC 16 27 11 -24 28.5           ~ 88 1
8 Elia 2-33 Y*O 16 27 30.18024 -24 27 43.3656           M2 125 1
9 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3969 1
10 JCMTSE J163138.6-244950 smm 16 31 39.2 -24 49 48           ~ 14 0
11 LDN 1689A DNe 16 32 12.5 -25 02 53           ~ 26 0
12 LDN 1689 DNe 16 32 22.5 -24 28 29           ~ 153 0
13 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1357 1
14 NAME IRAS 16293E cor 16 32 29.060 -24 29 10.27           ~ 69 1
15 LDN 1689B DNe 16 34 42.1 -24 36 11           ~ 181 0

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