Note to users. If you're seeing this message, it means that your browser cannot find this page's style/presentation instructions -- or possibly that you are using a browser that does not support current Web standards. Find out more about why this message is appearing, and what you can do to make your experience of our site the best it can be.

Site Tools

  • AAAS
  • Subscribe
  • Feedback

Site Search

Search Advanced

Science 10 August 2001:
Vol. 293. no. 5532, pp. 1112 - 1116
DOI: 10.1126/science.1062693

Reports

Resolving the Structure of Ionized Helium in the Intergalactic Medium with the Far Ultraviolet Spectroscopic Explorer

G. A. Kriss,12* J. M. Shull,3 W. Oegerle,4 W. Zheng,2 A. F. Davidsen,2dagger A. Songaila,5 J. Tumlinson,3 L. L. Cowie,5 J.-M. Deharveng,6 S. D. Friedman,2 M. L. Giroux,3 R. F. Green,7 J. B. Hutchings,8 E. B. Jenkins,9 J. W. Kruk,2 H. W. Moos,2 D. C. Morton,8 K. R. Sembach,2 T. M. Tripp9

The neutral hydrogen (H I) and ionized helium (He II) absorption in the spectra of quasars are unique probes of structure in the early universe. We present Far-Ultraviolet Spectroscopic Explorer observations of the line of sight to the quasar HE2347-4342 in the 1000 to 1187 angstrom band at a resolving power of 15,000. We resolve the He II Lyman alpha  (Lyalpha ) absorption as a discrete forest of absorption lines in the redshift range 2.3 to 2.7. About 50 percent of these features have H I counterparts with column densities NH I > 1012.3 per square centimeter that account for most of the observed opacity in He II Lyalpha . The He II to H I column density ratio ranges from 1 to >1000, with an average of ~80. Ratios of <100 are consistent with photoionization of the absorbing gas by a hard ionizing spectrum resulting from the integrated light of quasars, but ratios of >100 in many locations indicate additional contributions from starburst galaxies or heavily filtered quasar radiation. The presence of He II Lyalpha absorbers with no H I counterparts indicates that structure is present even in low-density regions, consistent with theoretical predictions of structure formation through gravitational instability.

1 Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218, USA.
2 Center for Astrophysical Sciences, Department of Physics and Astronomy, Johns Hopkins University, Baltimore, MD 21218, USA.
3 CASA and JILA, Department of Astrophysical and Planetary Sciences, University of Colorado, Campus Box 389, Boulder, CO 80309, USA.
4 Laboratory for Astronomy and Solar Physics, Code 681, NASA/Goddard Space Flight Center, Greenbelt, MD 20771, USA.
5 Institute for Astronomy, University of Hawaii, 2680 Woodlawn Road, Honolulu, HI 96822, USA.
6 Laboratorie d'Astronomie Spatiale, BP 8, 13376 Marseille Cedex 12, France.
7 Kitt Peak National Observatory, National Optical Astronomy Observatories, Post Office Box 26732, 950 North Cherry Avenue, Tucson, AZ 85726, USA.
8 Herzberg Institute of Astrophysics, National Research Council of Canada, Victoria, BC V8X 4M6, Canada.
9 Princeton University Observatory, Princeton, NJ 08544, USA.
*   To whom correspondence should be addressed. E-mail: gak{at}stsci.edu

dagger    Deceased.


Read the Full Text






ADVERTISEMENT
Click Me!

ADVERTISEMENT

To Advertise     Find Products


Science. ISSN 0036-8075 (print), 1095-9203 (online)