
Gas shells blown off stars that have run out of nuclear fuel.
The remaining central star is becoming a "white dwarf".
Light from central star ionizes the shell, causing it to glow.
Geometry is often bi-conical, rather than a simple shell.
Flow is often channeled by a circumstellar disk.
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Emission line strengths easily measured in very distant objects.
Relative strengths of lines of different chemical elements ==> ratio of
chemical abundance
s.
Classical analysis uses collisionally excited forbidden lines.
Deep spectra with high wavelength resolution now allows abundance determination also with permitted recombination lines.
The two techniques often give very discrepant results.
Up to factor 20 different.
What is going on???
Permitted lines excited by means other than recombination?
Using wrong density or temperature to determine abundances from strengths of collisionally excited lines?
Brian Sharpee's PhD thesis
Picked a PN with roughly spherical geometry.
IC 418
Expanding shell ==> faster moving gas is farther from ionizing star
Causes ionization-velocity correlation.
Used this correlation to study which permitted lines are really formed by recombinations.
Developed EMILI, a computer-aided EMIssion Line Identifier.
Publicly available at http://www.pa.msu.edu/astro/software/emili/
Comparing emission and absorption lines from same object.
Absorption lines ==> column density of gas in form of a particular ion.
Measure in UV with HST.
Find density needed to produce observed forbidden emission line surface brightness from that ion.
This should be ~same as density found for that ion from standard forbidden line analysis.
If not ==> problem with analysis of collisionally excited lines.
PNe spectra include weak collisionally excited lines from heavy r- and s-process elements.
s-process elements might be enhanced by processes in star that has formed PN. .
However, the r-process elements must be left over from the interstellar gas that originally formed the central star.
We are using very deep echelle spectra to measure abundances of r- and s-process elements.
4m Mayall Telescope at KPNO
6.5m Magellan Telescope at Las Campanas.
Bob Williams (Space Telescope Science Institute)
Brian Sharpee (Stanford Research Institute)
Ed Jenkins (Princeton University)
Mark Phillips (Las Campanas Observatory)
Peter Van Hoof (Queen's University Belfast)
Eric Pellegrini (MSU grad student)
Ken Cavagnolo (MSU grad student)
Williams, R., Jenkins, E.B., Baldwin, J.A., Zhang, Y., Sharpee, B., Pellegrini, E. & Phillips, M. 2008, ApJ (in press) Independent Emission and Absorption Abundances for Planetary Nebulae http://xxx.lanl.gov/abs/0801.2147
Sharpee, B., Zhang, Y., Williams, R., Pellegrini, E., Cavagnolo, K., Baldwin, J., Phillips, M. & Liu, X.-W. 2007, ApJ, 659, 1265, s-Process Abundances in Planetary Nebulae http://xxx.lanl.gov/abs/astro-ph/0612101
Sharpee, B., Baldwin, J.A. & Williams, R. 2004, ApJ, 615, 323 Identification and Characterization of Faint Emission Lines in the Spectrum of the Planetary Nebula IC 418 http://arxiv.org/abs/astro-ph/0407186
Sharpee, B., Williams, R., Baldwin, J.A. & van Hoof, P.A.M. 2003, ApJS, 149, 157, Introducing EMILI: Computer-aided Emission Line Identification http://arxiv.org/abs/astro-ph/0307053
Williams, R, Jenkins, E.B., Baldwin, J.A. & Sharpee, B. 2003, PASP,
115, 178 Comparative Absorption and Emission
Analyses of Nebulae: Ion Emission Densities for IC 418 http://arxiv.org/abs/astro-ph/0210551