SearcharxivSearch

arXiv · astro-ph/9608092

The Gaseous Environments of Radio Galaxies in the Early Universe: Kinematics of the Lyman $α$ Emission

Abstract

We present intermediate resolution ($\sim3$ Å) spectra of the Ly$α$ emission from 15 high redshift radio galaxies ($z>2$). Together with previously published spectra we analyze data for a sample of 18 objects. In 11 of the 18 radio galaxies we find deep troughs in the Ly$α$ emission profile, which we interpret as H\,{\sc i} absorption with column densities in the range $10^{18}$--$10^{19.5}$ cm$^{-2}$. Since in most cases the Ly$α$ emission is absorbed over its entire spatial extent (up to 50 kpc), the absorbers must have a covering fraction close to unity. Under plausible assumptions for the temperature and density of the absorbing gas this implies that the absorbing material must consist of $\sim 10^{12}$ clouds of typical size $\sim 0.03$ pc with a total mass of $\sim 10^8$ M$_{\odot}$. Our observations show that strong H\,{\sc i} absorption occurs in $>60$\% of the high redshift radio galaxies, while from the statistics of quasar absorption lines there is only a 2\% probability of such a strong H\,{\sc i} absorption line falling by chance in the small redshift interval of the Ly$α$ emission line. These absorbers are therefore most likely to be physically associated with the galaxy hosting the radio source or its direct environment. There are strong correlations between the properties of the Ly$α$ emission of the galaxies and the size of the associated radio source: (i) Of the smaller ($<50$ kpc) radio galaxies 9 out of 10 have strong associated H\,{\sc i} absorption, whereas only 2 of the 8 larger ($>50$ kpc) radio galaxies show such strong absorption. (ii) Larger radio sources tend to have larger Ly$α$ emission regions and (iii) a smaller Ly$α$ velocity

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

R. van Ojik, H. J. A. Röttgering, G. K. Miley, R. W. Hunstead. 1996-08-14. The Gaseous Environments of Radio Galaxies in the Early Universe: Kinematics of the Lyman $α$ Emission. https://arxiv.org/abs/astro-ph/9608092

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Cosmic Variance and Its Effect on the Luminosity Function Determination in Deep High z Surveys

We study cosmic variance in deep high redshift surveys and its influence on the determination of the luminosity function for high redshift galaxies. For several survey geometries relevant for HST and JWST instruments, we characterize the distribution of the galaxy number counts. This is obtained by means of analytic estimates via the two point correlation function in extended Press-Schechter theory as well as by using synthetic catalogs extracted from N-body cosmological simulations of structure formation. We adopt a simple luminosity - dark halo mass relation to investigate the environment effects on the fitting of the luminosity function. We show that in addition to variations of the normalization of the luminosity function, a steepening of its slope is also expected in underdense fields, similarly to what is observed within voids in the local universe. Therefore, to avoid introducing artificial biases, caution must be taken when attempting to correct for field underdensity, such as in the case of HST UDF i-dropout sample, which exhibits a deficit of bright counts with respect to the average counts in GOODS. A public version of the cosmic variance calculator based on the two point correlation function integration is made available on the web.

astro-ph

Receiver control for the Submillimeter Array

Efficient operation of a submillimeter interferometer requires remote (preferably automated) control of mechanically tuned local oscillators, phase-lock loops, mixers, optics, calibration vanes and cryostats. The present control system for these aspects of the Submillimeter Array (SMA) will be described. Distributed processing forms the underlying architecture and the software is split between hardware platforms in a leader/follower arrangement. In each antenna cabin, a serial network of up to ten independent 80C196 microcontroller boards attaches to the real-time PowerPC computer (running LynxOS). A multi-threaded, gcc-compiled leader program on the PowerPC accepts top-level requests via remote procedure calls (RPC), subsequently dispatches tuning commands to the relevant follower microcontrollers, and regularly reports the system status to optical-fiber-based reflective memory for common access by the telescope monitor and error reporting system. All serial communication occurs asynchronously via encoded, variable-length packets. The microcontrollers respond to the requested commands and queries by accessing non-volatile, rewriteable lookup-tables (when appropriate) and executing embedded software that operates additional electronic devices (DACs, ADCs, etc.). Since various receiver hardware components require linear or rotary motion, each microcontroller also implements a position servo via a one-millisecond interrupt service routine which drives a DC-motor/encoder combination that remains standard across each subsystem.

astro-ph

Classical analysis of the rotational dynamic of spiral galaxies: Quo Vadis Dark Matter?

In this paper we study a stellar dynamic model for the stars' rotational-dynamics, with a distribution of its own mass, rotating around its center with a higher density, like spiral galaxies happen, by means of a classical calculus of the rotation velocities of a particle around its rotational axis, inside a smoothed distribution of matter. The stars are supposed to be particles and their distribution in the galaxy is modelled as a matter distribution inversely proportional to its distance from its center. Two kinds of matter distribution are supposed: one with constant density, and other with radial distribution. Two types of galaxy symmetry are also considered: spherical and oblate ellipsoidal. Using only classical mechanics arguments it is shown that the calculated velocity distribution inside the galaxy is similar to that obtained from astronomical observations, without the necessity of suppose the existence of dark matter or other phenomena.

astro-ph