THE INTERSTELLAR MEDIUM

(3) The Spectrum of Cooling Galactic Fountain Gas

In the two decades which have passed since Shapiro and Field (1976, ApJ, 205, 762) first proposed the Galactic Fountain model for the galactic halo of interstellar gas and Shapiro and Moore (1976, ApJ, 207, 460) calculated the time-dependent, nonequilibrium ionization and radiative cooling of a hot, optically thin cosmic gas, including the emergent radiation spectrum, the observational support for the Galactic Fountain model has grown considerably. One of the longstanding puzzles which made the Fountain explanation of halo gas difficult, however, was only resolved in the last several years, by a renewed attack on the theory of the Galactic Fountain by Shapiro and his Ph.D. student Benjamin, which addressed the fact that UV absorption line strengths of highly ionized species C IV, Si IV, and N V due to halo gas were inconsistent with both the collisionally-ionized gas calculations of Shapiro and Moore and others and with the alternative picture of a halo of photoionized gas. In an attempt to reconcile the model with these and other observations of the galactic halo of the Milky Way and other galaxies, radiative transfer was included for the first time, in new calculations of the nonequilibrium thermal and ionization history of gas cooling radiatively from T~10^6K to T~10^4K in a 1D, planar, steady flow model of the galactic fountain ( Shapiro and Benjamin 1993; Benjamin & Shapiro 2000, submitted; Benjamin Ph.D. thesis). These results showed that such a flow is capable of matching the UV absorption and emission lines observed from highly ionized species in our Galactic halo, provided that "self-ionization" by "self-illumination" - the photoionization feedback of radiation emitted by the flow on the flow itself - is included, and that gas stops compressing isobarically at some point as it cools. A transverse magnetic field in the cooling flow would naturally produce this required non-isobaric cooling. To demonstrate this explicitly, an MHD radiative shock code was also written which incorporated all of the nonequilibrium ionization rate equations, cooling, and radiative transfer described above, and the results confirmed that a radiative shock of a few hundred kilometers per second in gas with microgauss strength magnetic field would reproduce the results of the cooling flow calculations described above, as required to explain the halo observations (Benjamin & Shapiro 2000, submitted; Benjamin Ph.D. thesis). This is but one plausible example of how the necessary non-isobaricity of the Fountain flow might be achieved. The same basic Fountain model was then applied to explain the absorption lines due to metals in Lyman Limit System quasar absorption line gas at high redshift as due to cooling gas in galactic halos and a successful match to observed line strengths was obtained, including the prediction that the same gas should show other highly ionized species like O VI, which has since been detected ( Shapiro and Benjamin 1993; Benjamin & Shapiro 2000, submitted; Benjamin Ph.D. thesis).

Previous page Next page Return to table of contents