2025RAA....25h5018J


Query : 2025RAA....25h5018J

2025RAA....25h5018J - Research in Astron. and astroph., 25, part no 8, 5018 (2025/August-0)

Properties of the Cores and Filaments in the Ophiuchus Molecular Cloud and its L1688 Hub-filament System.

JIA B.-S., ZHANG G.-Y., MEN'SHCHIKOV A., DIB S., LI J.-Z., WANG K., LI D., LI X.-M., REN Z.-Y., ZHANG C., PERVAIZ N. and XIAO L.

Abstract (from CDS):

Analyzing filaments and cores in molecular clouds is key to understanding galactic star formation and its environmental dependence. This paper studies the properties and distribution of dense cores and filaments in the Ophiuchus molecular cloud, with a focus on the L1688 hub-filament system (HFS) and its star formation potential. We extracted sources and filaments from Herschel images and a 13$\mathop{.}\limits^{^{\prime\prime} }$5 resolution surface density map using the getsf method, identified dense cores among the extracted sources, evaluated core mass segregation, and constructed the core mass function (CMF). We derived properties of the filaments from their radial surface density profiles, constructed the filament linear density function (FLDF), and assessed the mass distribution in the L1688 HFS to estimate the core and filament formation efficiencies (CFEs, FFEs). We identified 64 protostellar, 132 prestellar, and 686 unbound cores. The CMF of the prestellar cores has a power-law exponent of -0.86, and the FLDF of the densest filaments has a similar slope of -0.97, whereas the CMF of the unbound cores is found to be -1.36. Mass segregation is prominent among the most massive cores, with only slight differences between the bound and unbound cores. The low-mass unbound cores affect the overall spatial distribution. Among the 769 well-resolved filaments, we find a median half-maximum width of 0.12 pc and a median slope of -1.4 for the filament radial profiles. Mass distribution in the L1688 hub is dominated by the filaments, and outside the hub, it is dominated by the molecular cloud background. There exists a strong correlation between FFE and CFE, which reach their respective maxima of 71% and 5% within the hub and decrease to 21% and 0.9% outside it. The results suggest that the gravitational potential in the L1688 HFS influences core clustering in its high-density regions and that the filament-dominated core formation is a key mechanism in star formation within the system.

Abstract Copyright: © 2025. National Astronomical Observatories, CAS and IOP Publishing Ltd. All rights, including for text and data mining, AI training, and similar technologies, are reserved.

Journal keyword(s): stars: formation - ISM: molecules - infrared: ISM

Status at CDS : Large table(s) will be appraised for possible ingestion in VizieR.

Simbad objects: 17

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Number of rows : 17
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 NAME California Molecular Cloud MoC 04 10.0 +39 00           ~ 188 1
2 Barnard 211 DNe 04 17 35 +27 43.1           ~ 141 0
3 Barnard 213 DNe 04 20 51 +27 16.3           ~ 249 0
4 Barnard 218 DNe 04 28.1 +26 16           ~ 43 0
5 NAME Taurus Complex SFR 04 41.0 +25 52           ~ 4971 0
6 NAME Ori B MoC 05 41 43.0 -01 54 44           ~ 1498 0
7 NAME Mon R2 HII 06 07 47.58 -06 22 42.6           ~ 789 2
8 NAME Upper Sco-Cen As* 16 15 -24.2           ~ 1497 1
9 HD 147889 Or* 16 25 24.3163637976 -24 27 56.569805208 8.56 8.73 7.90     B2V 512 1
10 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3969 1
11 LDN 1709 DNe 16 31 34.8 -24 02 55           ~ 84 0
12 LDN 1689 DNe 16 32 22.5 -24 28 29           ~ 153 0
13 LDN 1712 DNe 16 38.0 -24 26           ~ 43 0
14 NAME Serpens Cloud SFR 18 29 49 +01 14.8           ~ 1195 1
15 NAME Aql Region reg 18 31.1 -02 10           ~ 456 0
16 W 43 SFR 18 47 32 -01 56.5           ~ 604 0
17 NAME Cygnus X North MoC 20 37.0 +41 56           ~ 33 0

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