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Filamentary accretion flows in high-mass star-forming clouds

J. -E. Schneider, H. Beuther, C. Gieser, S. Jiao, M. R. A. Wells, R. Klessen, S. Feng, P. Klaassen, M. T. Beltran, R. Cesaroni, S. Leurini, J. S. Urquhart, A. Palau, R. Pudritz

TL;DR

This study investigates filamentary accretion as a mechanism for feeding dense clumps in three high-mass star-forming clouds by combining dust continuum derived surface densities with velocity differences from HCO+ and H13CO+ line data. A simple inflow model relates $\Delta v$, $\Sigma$, and the inclination $i$ to estimate mass-flow rates along filaments and onto clumps. The results reveal filamentary mass flows reaching up to $\dot{M} \sim 10^{-3} M_{\odot}\,\mathrm{yr}^{-1}$ in G75 and $\dot{M} \sim 10^{-5}$ to $10^{-4} M_{\odot}\,\mathrm{yr}^{-1}$ in IRAS21078 and NGC7538, with flows often oriented toward clumps and enhanced near overdense regions; velocity gradients associated with H II region feedback can dominate local kinematics and complicate the inflow interpretation. The work demonstrates a practical method to quantify multi-scale filamentary accretion and highlights the role of feedback in shaping gas dynamics during the early stages of high-mass star formation.

Abstract

We quantify the gas flows from a scale of up to several parsecs down to the sub-parsec scale along filamentary structures in the three high-mass star-forming regions G75.78, IRAS21078+5211 and NGC7538 with data obtained from the IRAM 30 m telescope. The analysis is carried out using the surface density derived from 1.2 mm continuum emission and velocity differences estimated from HCO$^+$ and H$^{13}$CO$^+$ molecular line data.

Filamentary accretion flows in high-mass star-forming clouds

TL;DR

This study investigates filamentary accretion as a mechanism for feeding dense clumps in three high-mass star-forming clouds by combining dust continuum derived surface densities with velocity differences from HCO+ and H13CO+ line data. A simple inflow model relates , , and the inclination to estimate mass-flow rates along filaments and onto clumps. The results reveal filamentary mass flows reaching up to in G75 and to in IRAS21078 and NGC7538, with flows often oriented toward clumps and enhanced near overdense regions; velocity gradients associated with H II region feedback can dominate local kinematics and complicate the inflow interpretation. The work demonstrates a practical method to quantify multi-scale filamentary accretion and highlights the role of feedback in shaping gas dynamics during the early stages of high-mass star formation.

Abstract

We quantify the gas flows from a scale of up to several parsecs down to the sub-parsec scale along filamentary structures in the three high-mass star-forming regions G75.78, IRAS21078+5211 and NGC7538 with data obtained from the IRAM 30 m telescope. The analysis is carried out using the surface density derived from 1.2 mm continuum emission and velocity differences estimated from HCO and HCO molecular line data.

Paper Structure

This paper contains 11 sections, 2 equations, 46 figures, 5 tables.

Figures (46)

  • Figure 1: Top row: NIKA2 1.2 mm dust continuum maps (see beuther2024) of the star-forming regions showing the clump and filament designations. The red and magenta markers indicate the data points used for the flow rate estimation in Section \ref{['sec:fila-flows']}. Triangular magenta markers indicate a separate section along a structure. Black contours outline the 1.2 mm continuum, ranging from 3$\sigma$ to 39$\sigma$ in steps of 3$\sigma$ (the RMS-values are presented in Table \ref{['tab:dust_hii_rms']}). The red contours in the upper panels mark the peak-positions of the continuum emission from 20% to 100% in steps of 20%. Designations used in the following refer to clumps and filament-structures, filaments are marked by an "F" in the designation; "CF" in G75 stands for "central filament", "CC" in IRAS21078 refers to "central clump" while the clumps in NGC7538 are the known objects IRS9, IRS1 and S (e.g. Beuther). G75 S1 is the object G75.78+0.34. We present the clump-designations together with their coordinates in Table \ref{['tab:clumps']}. Bottom row: The same dust-maps with red contour lines outlining the H$II$1.2ex-regions at 1.4 GHz (21 cm) (CondonVLA_1998); the contours range from 10% to 100% of the peak emission in steps of 10% (see Table \ref{['tab:dust_hii_rms']} for reference). The positions of the two main exciting sources of the H$II$1.2ex-region in NGC7538, NGC7538 IRS5 and NGC7538 IRS6, are marked in the lower right panel (Puga).
  • Figure 2: First moment (intensity-weighted peak-velocity) maps for the HCO$^+$ ($1-0$)-line. The beam size is 27″ (lower left corner). The sources are labeled in each panel. The scale bar indicates the length of 1 parsec in each panel. Contour lines show the 1.2 mm dust continuum ranging from 3$\sigma$ to 39$\sigma$ in 3$\sigma$-steps.
  • Figure 3: As for Fig. \ref{['fig:1stmoment_hco+']} but for H$^{13}$CO$^+$ ($1-0$)-transition.
  • Figure 4: Dust temperature maps of G75 (left panel) and NGC7538 (right panel). Both maps were created using Herschel-data (Molinari2010) and free-free corrected dust continuum emission from the NIKA2 dataset. In the bottom left corner the 27″ beam of the final data product is shown. Black contours outline the free-free corrected 1.2 mm continuum emission at 27″ resolution in logarithmic scale from 5$\sigma$ to peak value.
  • Figure 5: Spectra towards G75, showing molecular emission of HCO$^+$ ($1-0$) (red) and H$^{13}$CO$^+$ ($1-0$) (black). The left panel shows the emission at the clump position S1 in G75. The right panel shows the spectra for a position along the CF filament in G75 (see upper left panel of Fig. \ref{['fig:dusttags']}).
  • ...and 41 more figures