Free-Free Spectral Energy Distributions of Hierarchically Clumped HII Regions
Astrophys.J. 610 (2004) 351-360 In an effort to understand unusual power-law spectral slopes observed in some hypercompact HII regions, we consider the radio continuum energy distribution from an ensemble of spherical clumps. An analytic expression for the free-free emission from a single spherical...
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Format | Journal Article |
Language | English |
Published |
30.03.2004
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Online Access | Get full text |
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Summary: | Astrophys.J. 610 (2004) 351-360 In an effort to understand unusual power-law spectral slopes observed in some
hypercompact HII regions, we consider the radio continuum energy distribution
from an ensemble of spherical clumps. An analytic expression for the free-free
emission from a single spherical clump is derived. The radio continuum slope
(with F_\nu \nu^\alpha) is governed by the population of clump optical depths
N(tau), such that (a) at frequencies where all clumps are thick, a continuum
slope of +2 is found, (b) at frequencies where all clumps are optically thin, a
flattened slope of -0.11 is found, and (c) at intermediate frequencies, a
power-law segment of significant bandwidth with slopes between these two
limiting values can result. For the ensemble distribution, we adopt a power-law
distribution N(tau) tau^{-\gamma}, and find that significant power-law segments
in the SED with slopes from +2 to -0.11 result only for a relatively restricted
range of $\gamma$ values of 1 to 2. Further, a greater range of clump optical
depths for this distribution leads to a wider bandwidth over which the
intermediate power-law segment exists. The model is applied to the source
W49N-B2 with an observed slope of \alphab +0.9, but that may be turning over to
become optically thin around 2 mm. An adequate fit is found in which most
clumps are optically thin and there is little shadowing of rearward clumps by
foreground clumps (i.e., the geometrical covering factor C<<1). The primary
insight gained from our study is that in the Rayleigh-Jeans limit for the
Planck function that applies for the radio band, it is the distribution in
optical depth of the clump population that is solely responsible for setting
the continuum shape, with variations in the size and temperature of clumps
serving to modulate the level of free-free emission. |
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DOI: | 10.48550/arxiv.astro-ph/0403689 |