LMC HII Region Luminosities versus
Observed Ionizing Stars

M. S. Oey and R. C. Kennicutt, Jr., PASA, 15 (1), 141
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Methods

The Large Magellanic Cloud (LMC) offers a broad range of HII regions of varying luminosities and morphologies, and for over a dozen of these, a complete, classified census is available for the hottest, most massive stars (e.g., Massey etal. 1995; Oey 1996). Likewise, a catalog of uniform nebular photometry is available for the Htex2html_wrap_inline135 luminosities of the HII\ regions (Kennicutt & Hodge 1986). With the aid of stellar atmosphere models, it is possible to estimate the Lyman continuum (Lyc) photon emission rate for the individual stars, and obtain a predicted total nebular Htex2html_wrap_inline135\ luminosity, to compare directly with the observed values.

Table 1 shows the results of this comparison for 12 objects. Column 1 identifies the nebula by its designation in the Davies, Elliott & Meaburn (1976; DEM) Htex2html_wrap_inline135 catalog, and column 2 identifies the corresponding OB association from the Lucke & Hodge (1970; LH) catalog. In the third column, we list the number of O stars (tex2html_wrap_inline161) identified spectroscopically from the reference shown in the last column. We have considered the ionizing contributions of only O stars, but we identify those associations containing WR stars with an asterisk on tex2html_wrap_inline161. Column 4 shows the ratio of the observed Htex2html_wrap_inline135\ luminosity (tex2html_wrap_inline167) to that predicted (tex2html_wrap_inline169) from the observed O stars, using the stellar Lyc emission rates of Schaerer & deKoter (1997). tex2html_wrap_inline169 is adjusted for the observed extinction, derived from the reddenings found in the stellar observations. Further details regarding the measurement of tex2html_wrap_inline167 and computation of tex2html_wrap_inline169 may be found in Oey & Kennicutt (1997). In column 5, we classify the nebular morphology as diffuse HII region (D), superbubble (S), or composite (C).

 

DEM LH tex2html_wrap_inline161 tex2html_wrap_inline181 Morph Reference
10B 2 0.81 D J. Wm. Parker, unpublished
31 6 0.40 S Oey (1996)
34 9, 10 44tex2html_wrap_inline183 0.66 C Parker etal. (1991)
106 38 0.61 S Oey (1996)
152, 156tex2html_wrap_inline185 47, 48 35tex2html_wrap_inline183 0.66 C Oey & Massey (1995)
192 51, 54 25tex2html_wrap_inline183 0.83 S Oey & Smedley (1997)
199 58 22tex2html_wrap_inline183 1.22 C Garmany etal. (1994)
226 73 0.93 S Oey (1996)
243 83 11  0.54 D Oey (1996)
293 110 1.09 D Conti etal. (1986)
301 114 0.20 S Oey (1996)
323, 326 117, 118 20  1.13 D Massey etal. (1989)
Table 1: Ratio of Observed and Predicted HII Region Luminosities
tex2html_wrap_inline183WR star excluded; DEM 199 contains 3 WR stars.

tex2html_wrap_inline185Not including DEM 152A.

The median tex2html_wrap_inline181 is 0.74, suggesting that many HII regions are significantly density-bounded. However, there are many sources of substantial uncertainty, which are discussed in detail by Oey & Kennicutt (1997). These include uncounted O and WR stars; the effect of B stars, whose ionizing fluxes are poorly known; accounting for LMC metallicity; observational errors in extinction; and error in the LMC distance. However, the modeled ionizing fluxes of O stars are by far the dominant source of uncertainty, contributing about tex2html_wrap_inline201% to the overall median tex2html_wrap_inline181. We therefore estimate that tex2html_wrap_inline205, or equivalently, that a median fraction of ionizing radiation that escapes the local nebulae is in the range 0 - 51%.


Next Section: Results
Title/Abstract Page: LMC HII Region Luminosities
Previous Section: Introduction
Contents Page: Volume 15, Number 1

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