G. Garay et al., VLA OBSERVATIONS OF CARBON RADIO RECOMBINATION LINES TOWARD THE H-II REGION COMPLEX S88B, The Astrophysical journal, 501(2), 1998, pp. 699-709
We present high angular resolution VLA observations of the C92 alpha,
C110 alpha, and C166 alpha radio recombination lines of carbon from th
e region of massive star formation known as S88B. The observations rev
eal that the carbon emission arises from two distinct components that
are intimately associated with the compact (S88B2) and cometary (S88B1
) regions of ionized gas within the complex. The brighter carbon compo
nent has an angular size of similar to 6''.6, an average line-center v
elocity of 21.0 +/- 0.5 km s(-1), and an average line width of 5.1 +/-
1.0 km s(-1); it is associated with the compact H II region. The seco
nd component has an angular size of similar to 16 degrees and is found
projected toward the head of the cometary-like H II region. The avera
ge center velocity and width of the carbon line emission are 21.1 +/-
0.7 km s(-1) and 5.1 +/- 1.7 km s(-1), respectively. The spatial locat
ion and velocity of both carbon regions suggest that the emission aris
es in layers of photodissociated gas at the interface between the mole
cular cloud and the regions of ionized gas that are undergoing a champ
agne phase. From a model analysis of the dependence of the recombinati
on line intensity with principal quantum number, we conclude that the
carbon emission originates in warm photodissociated regions. The elect
ron temperatures and electron densities of the photodissociated gas ra
nge between 400 and 600 K and between 40 and 80 cm(-3), respectively.
Further, we find that stimulated amplification of the background H II
region continuum radiation contributes significantly to the carbon emi
ssion in both components. We also detected emission in sulfur radio re
combination lines from both components. We find that the ratios of sul
fur to carbon line intensities are considerable larger than the [S/C]
cosmic abundance ratio and that they vary with principal quantum numbe
r, with values in the range between 0.3 and 0.6. We attribute the larg
e values of the intensity ratios to depletion of carbon in the gas pha
se by a factor of similar to 5 and the variations with principal quant
um number to stimulated emission effects in a region of low electron d
ensity (n(e) similar to 3 cm(-3)) and low temperature (T-e similar to
50 K) that surrounds the C+ region.