84 research outputs found
Recombination Line vs. Forbidden Line Abundances in Planetary Nebulae
Recombination lines (RLs) of C II, N II, and O II in planetary nebulae (PNs)
have been found to give abundances that are much larger in some cases than
abundances from collisionally-excited forbidden lines (CELs). The origins of
this abundance discrepancy are highly debated. We present new spectroscopic
observations of O II and C II recombination lines for six planetary nebulae.
With these data we compare the abundances derived from the optical
recombination lines with those determined from collisionally-excited lines.
Combining our new data with published results on RLs in other PNs, we examine
the discrepancy in abundances derived from RLs and CELs. We find that there is
a wide range in the measured abundance discrepancy Delta(O+2) = log O+2(RL) -
log O+2(CEL), ranging from approximately 0.1 dex up to 1.4 dex. Most RLs yield
similar abundances, with the notable exception of O II multiplet V15, known to
arise primarily from dielectronic recombination, which gives abundances
averaging 0.6 dex higher than other O II RLs. We compare Delta(O+2) against a
variety of physical properties of the PNs to look for clues as to the mechanism
responsible for the abundance discrepancy. The strongest correlations are found
with the nebula diameter and the Balmer surface brightness. An inverse
correlation of Delta(O+2) with nebular density is also seen. Similar results
are found for carbon in comparing C II RL abundances with ultraviolet
measurements of C III].Comment: 48 pages, 14 figures, accepted for publication in the Astrophysical
Journal Supplemen
Physical Structure of Small Wolf-Rayet Ring Nebulae
We have selected the seven most well-defined WR ring nebulae in the LMC (Br
2, Br 10, Br 13, Br 40a, Br 48, Br 52, and Br 100) to study their physical
nature and evolutionary stages. New CCD imaging and echelle observations have
been obtained for five of these nebulae; previous photographic imaging and
echelle observations are available for the remaining two nebulae. Using the
nebular dynamics and abundances, we find that the Br 13 nebula is a
circumstellar bubble, and that the Br 2 nebula may represent a circumstellar
bubble merging with a fossil main-sequence interstellar bubble. The nebulae
around Br 10, Br 52, and Br 100 all show influence of the ambient interstellar
medium. Their regular expansion patterns suggest that they still contain
significant amounts of circumstellar material. Their nebular abundances would
be extremely interesting, as their central stars are WC5 and WN3-4 stars whose
nebular abundances have not been derived previously. Intriguing and tantalizing
implications are obtained from comparisons of the LMC WR ring nebulae with ring
nebulae around Galactic WR stars, Galactic LBVs, LMC LBVs, and LMC BSGs;
however, these implications may be limited by small-number statistics. A SNR
candidate close to Br 2 is diagnosed by its large expansion velocity and
nonthermal radio emission. There is no indication that Br 2's ring nebula
interacts dynamically with this SNR candidate.Comment: 20 pages, Latex (aaspp4.sty), 2 figures, accepted by the Astronomical
Journal (March 99 issue
Newly Identified Star Clusters in M33. II. Radial HST/ACS Fields
We present integrated photometry and color-magnitude diagrams for 161 star
clusters in M33, of which 115 were previously uncataloged, using the Advanced
Camera For Surveys Wide Field Channel onboard the Hubble Space Telescope. The
integrated V-band magnitudes of these clusters range from Mv~-9 to as faint as
Mv~-4, extending the depth of the existing M33 cluster catalogs by ~1 mag.
Comparisons of theoretical isochrones to the color-magnitude diagrams using the
Padova models yield ages for 148 of these star clusters. The ages range from
Log (t)~7.0 to Log (t)~9.0. Our color-magnitude diagrams are not sensitive to
clusters older than ~1 Gyr. We find that the variation of the clusters'
integrated colors and absolute magnitudes with age is consistent with the
predictions of simple stellar population models. These same models suggest that
the masses of the clusters in our sample range from 5x10^3 to 5x10^4 *Msun.Comment: 28 pages, 12 figures, accepted for publication in The Astrophysical
Journa
ISO SWS Observations of H II Regions in NGC 6822 and I ZW 36: Sulfur Abundances and Temperature Fluctuations
We report ISO SWS infrared spectroscopy of the H II region Hubble V in NGC
6822 and the blue compact dwarf galaxy I Zw 36. Observations of Br alpha, [S
III] at 18.7 and 33.5 microns, and [S IV] at 10.5 microns are used to determine
ionic sulfur abundances in these H II regions. There is relatively good
agreement between our observations and predictions of S^+3 abundances based on
photoionization calculations, although there is an offset in the sense that the
models overpredict the S^+3 abundances. We emphasize a need for more
observations of this type in order to place nebular sulfur abundance
determinations on firmer ground. The S/O ratios derived using the ISO
observations in combination with optical data are consistent with values of
S/O, derived from optical measurements of other metal-poor galaxies.
We present a new formalism for the simultaneous determination of the
temperature, temperature fluctuations, and abundances in a nebula, given a mix
of optical and infrared observed line ratios. The uncertainties in our ISO
measurements and the lack of observations of [S III] lambda 9532 or lambda 9069
do not allow an accurate determination of the amplitude of temperature
fluctuations for Hubble V and I Zw 36. Finally, using synthetic data, we
illustrate the diagnostic power and limitations of our new method.Comment: 32 Pages total, including 6 encapsulated postscript figures (one with
two parts). Accepted for Publication in the 20 Dec 2002 Ap
Dust In I Zw 18 From Hubble Space Telescope Narrow Band Imaging
We present new WFPC2 narrow band imaging of the blue compact dwarf galaxy I
Zw 18, which is host to the lowest-metallicity HII regions known. Images at
H-alpha and H-beta are combined with archival broad band images to allow the
study of the ionized gas distribution and morphology. Analysis of the
H-alpha/H-beta flux ratio reveals significant enhancements in some areas of
both the ``Northwest'' and ``Southeast'' regions of the galaxy, with ratios
elevated to levels as high as 3.4. The H-alpha/H-beta ratio varies considerably
with position throughout the galaxy. Comparing this distribution with the
stellar distribution indicates that the regions of enhanced H-alpha/H-beta
ratio are not due to the effects of either collisional excitation or underlying
stellar absorption, and therefore are most likely interpreted as the presence
of dust. This dust has an estimated mass of (2-5)x10^3 solar masses, which is
consistent with the IRAS far-IR non-detection. Under the assumption that dust
traces the presence of molecular gas, these results suggest that the molecular
component of the ISM of I Zw 18, which is needed to fuel its active star
formation, is also very clumpy. Such a distribution would be consistent with
the recent FUSE non-detections of diffuse H_2.Comment: 26 pages, 3 figures. Accepted for publication in the Astrophysical
Journal, Volume 56
The Composition Gradient in M101 Revisited. II. Electron Temperatures and Implications for the Nebular Abundance Scale
(Abridged) We use high S/N spectra of 20 HII regions in the giant spiral
galaxy M101 to derive electron temperatures for the HII regions and robust
metal abundances over radii R = 0.19-1.25 Ro (6-41 kpc). We compare the
consistency of electron temperatures measured from the [O III]4363, [N II]5755,
[S III]6312, and [O II]7325 auroral lines. Temperatures from [O III], [S III],
and [N II] are correlated with relative offsets that are consistent with
expectations from nebular photoionization models. However, the temperatures
derived from the [O II]7325 line show a large scatter and are nearly
uncorrelated with temperatures derived from other ions. Our derived oxygen
abundances O/H are well fitted by an exponential distribution over six disk
scale lengths, from approximately 1.3 solar in the center to 1/15 solar in the
outermost region studied (for solar 12 + log (O/H)=8.7). We measure significant
radial gradients in N/O and He/H abundance ratios, but relatively constant S/O
and Ar/O. Our abundances are systematically lower by 0.2-0.5 dex than those
derived from the most widely used strong-line "empirical" abundance indicators.
We suspect that most of the disagreement with the strong-line abundances arises
from uncertainties in the nebular models that are used to calibrate the
"empirical" scale, and that strong-line abundances derived for HII regions and
emission-line galaxies are as much as a factor of two higher than the actual
oxygen abundances. However other explanations, such as the effects of
temperature fluctuations on the auroral line based abundances cannot be
completely ruled out. These results point to the need for direct abundance
determinations of a larger sample of extragalactic HII regions, especially for
objects more metal-rich than solar.Comment: 50 pages, 14 figures, 8 tables. Accepted by Ap
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