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Title: Probing the Outflowing Multiphase Gas ∼1 kpc below the Galactic Center

Journal Article · · Astrophysical Journal, Supplement Series
; ;  [1];  [2];  [3];  [4];  [5];  [6];  [7];  [8];  [9]
  1. Department of astronomy, University of Wisconsin, Madison, 475 North Charter Street, Madison, WI 53706 (United States)
  2. Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD, 21218 (United States)
  3. Space Science Institute, 4750 Walnut Street, Suite 205, Boulder, CO 80301 (United States)
  4. MIT-Kavli Center for Astrophysics and Space Research, 77 Massachusetts Avenue, Cambridge, MA 02139 (United States)
  5. Princeton University Observatory, Princeton, NJ 08544 (United States)
  6. Department of Physics, University of Notre Dame, Notre Dame, IN 46556 (United States)
  7. Institute of Astronomy, School of Physics, University of Sydney, NSW 2006 (Australia)
  8. Green Bank Observatory, P.O. Box 2, Green Bank, WV 24944 (United States)
  9. Department of Astrophysics, Radboud University, Nijmegen, PO Box 9010, 6500 GL Nijmegen (Netherlands)

Comparison of interstellar medium (ISM) absorption in the UV spectrum of LS 4825, a B1 Ib−II star d  = 21 ± 5 kpc from the Sun toward l  = 1.°67 and b  = −6.°63, with ISM absorption toward an aligned foreground star at d  < 7.0 ± 1.7 kpc, allows us to isolate and study gas associated with the Milky Way nuclear wind. Spectra from the Space Telescope Imaging Spectrograph show low-ionization absorption out to d  < 7 kpc (e.g., O i, C ii, Mg ii, Si ii, Fe ii, S ii) only between 0 and 40 km s{sup −1}, while absorption at d  > 7 kpc, ∼1 kpc below the Galactic plane, is complex and spans −290 to +94 km s{sup −1}. The intermediate and high ions Si iii, C iv, Si iv, and N v show extremely strong absorption with multiple components from −283 to 107 km s{sup −1}, implying that the ISM ∼1 kpc below the Galactic center has a substantial reservoir of plasma and more gas containing C iv and N v than in the Carina OB1 association at z  = 0 kpc. Abundances and physical conditions are presented for many absorption components. The high ion absorption traces cooling transition temperature plasma probably driven by the outflowing hot gas, while the extraordinarily large thermal pressure, p / k  ∼ 10{sup 5} cm{sup −3} K{sup −1}, in an absorption component at −114 km s{sup −1} probably arises from the ram pressure of the outflowing hot gas. The observations are consistent with a flow whose ionization structure in the high ions can be understood through a combination of nonequilibrium radiative cooling and turbulent mixing.

OSTI ID:
22661085
Journal Information:
Astrophysical Journal, Supplement Series, Vol. 232, Issue 2; Other Information: Country of input: International Atomic Energy Agency (IAEA); ISSN 0067-0049
Country of Publication:
United States
Language:
English