Dust and Diffuse Interstellar Bands in the za = 0.524 Absorption System toward AO 0235+164* **

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© 2004. The American Astronomical Society. All rights reserved. Printed in U.S.A.
, , Citation V. T. Junkkarinen et al 2004 ApJ 614 658 DOI 10.1086/423777

0004-637X/614/2/658

Abstract

We present new Hubble Space Telescope (HST) Space Telescope Imaging Spectrograph (STIS) NUV-MAMA and STIS CCD observations of the BL Lac object AO 0235+164 and the intervening damped Lyα (DLA) line at za = 0.524. The line profile gives N(H ) = × 1021 cm-2 and, combined with the H I 21 cm absorption data, leads to a spin temperature of Ts = 220 ± 60 K. Those spectra also show a strong, broad feature at the expected position of the 2175 Å graphitic dust feature at za = 0.524. Assuming a Galactic-type dust extinction curve at za = 0.524 gives a dust-to-gas ratio of 0.19 times the Galactic value, but the fit, assuming that the underlying, unreddened spectrum is a single power law, is poor in the far-UV. A dust-to-gas ratio of 0.19 times the Galactic value is similar to the LMC, but the AO 0235+164 spectrum does not fit either the LMC extinction curve or the SMC extinction curve (which has practically no 2175 Å feature). A possible interpretation includes dust similar to that in the Galaxy, but with fewer of the small particles that produce the far-UV extinction. The metallicity of the za = 0.524 absorber, estimated from the observed N(H ) and excess X-ray absorption (beyond Galactic) derived from contemporaneous and archival ASCA and ROSAT X-ray data, is Z = 0.72 ± 0.28 Z, implying in turn a dust-to-metals ratio of 0.27 times the Galactic value. If the dust mass density is the same in the za = 0.524 DLA system as in our Galaxy, only 14% (±6%) of the metals (by mass) are in dust, compared to 51%, 36%, and 46% for the Galaxy, LMC, and SMC, respectively. Such a dusty za = 0.524 AO 0235+164 absorption system is a good example of the kind of DLA system that will be missed because of selection effects, which in turn can bias the measurement of the comoving density of interstellar gas (in units of the closure density), Ωg, as a function of z.

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Footnotes

  • Based on observations with the NASA/ESA Hubble Space Telescope, obtained at the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS5-26555.

  • ** 

    Some of the data presented herein were obtained at the W. M. Keck Observatory, which is operated as a scientific partnership among the California Institute of Technology, the University of California, and the National Aeronautics and Space Administration. The Observatory was made possible by the generous financial support of the W. M. Keck Foundation.

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10.1086/423777