Ultraviolet spectral variability and the Lyα forest in the lensed quasar Q0957+561

被引:6
|
作者
Dolan, JF
Michalitsianos, AG
Nguyen, QT
Hill, RJ
机构
[1] NASA, Goddard Space Flight Ctr, Astron & Solar Phys Lab, Greenbelt, MD 20771 USA
[2] San Diego State Univ, Dept Astron, San Diego, CA 92182 USA
来源
ASTROPHYSICAL JOURNAL | 2000年 / 539卷 / 01期
关键词
gravitational lensing; quasars : absorption lines; quasars : emission lines; quasars : individual (Q0957+561); ultraviolet : galaxies;
D O I
10.1086/309206
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Far-ultraviolet spectra of the gravitational lens components Q0957+561A, B were obtained with the Hubble Space Telescope Faint Object Spectrograph (FOS) at five equally spaced epochs, one every 2 weeks. We confirm the flux variability of the quasar's Ly alpha and O VI lambda 1037 emission lines in IUE spectra reported in earlier work of Dolan et al. The fluxes in these lines vary on a timescale of weeks in the observer's rest frame, independently of each other and of the surrounding continuum. The individual spectra of each image were co-added to investigate the properties of the Ly alpha forest along the two lines of sight to the quasar. Absorption lines having equivalent width W-lambda greater than or equal to 0.3 Angstrom in the observer's frame not previously identified by Michalitsianos et al. as interstellar lines, metal lines, or higher order Lyman lines were taken to be Ly alpha forest lines. The existence of each line in this consistently selected set was then verified by its presence in two archival FOS spectra with similar to 1.5 times higher signal to noise than our co-added spectra. Ly alpha forest lines with W-lambda greater than or equal to 0.3 A appear at 41 distinct wavelengths in the spectra of the two images. One absorption line in the spectrum of image A has no counterpart in the spectrum of image B, and one line in image B has no counterpart in image A. Based on the separation of the lines of sight over the redshift range searched for Ly alpha forest lines, the density of the absorbing clouds in the direction of Q0957 + 561 must change significantly over a distance R = 160(-70)(+120) h(50)(-1) kpc in the simplified model where the absorbers are treated as spherical clouds and the characteristic dimension, R, is the radius. (We adopt H-0 = 50 h(50) km s(-1) Mpc(-1), q(0) = 1/2, and Lambda = 0 throughout this paper.) The 95% confidence interval on R extends from 50 to 950 h(50)(-1) kpc. We show in the Appendix that the fraction of Lya forest lines that appear in only one spectrum can be expressed as a rapidly converging power series in 1/r, where r the ratio of the radius of the cloud to the separation of the two lines of sight at the redshift of the cloud. This power series can be rewritten to give r in terms of the fraction of Ly alpha forest wavelengths that appear in the spectrum of only one image. A simple linear approximation to the solution that everywhere agrees with the power series solution to better than 0.8% for r greater than or equal to 2 is derived in the Appendix.
引用
收藏
页码:111 / 123
页数:13
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