A cold component and the complex velocity structure of DLA1331+170

TL;DR

This study investigates the complex velocity structure of the DLA1331+170 system, revealing multiple components, a cold neutral component at 220K, and differences between neutral and ionized gas profiles, challenging simple interpretations of the gas properties.

Contribution

It provides a detailed multi-phase analysis of the velocity structure in a high-redshift DLA, highlighting the complexity and differences across ionization stages and the limitations of current separation methods.

Findings

Identification of at least two to three velocity components with neutral carbon.

Detection of a cold component at 220K based on Doppler broadening.

Significant differences between 21cm, optical, and neutral carbon profiles.

Abstract

[ABRIDGED] We examine the velocity structure in the gas associated with \ion{H}{1} in the damped Ly$\alpha$ absorption system at redshift $z=1.7764$ towards the QSO $1331+170$ using 21cm data, optical and STIS spectra. We find at least two, and possibly three, components showing \ion{C}{1} lines. One of these has Doppler parameter $b=0.55${\kms}, corresponding to a kinetic temperature of 220K if the broadening is thermal. We re-examine the H$_2$ analysis undertaken by \citet{Cui05} using the neutral carbon velocity structure, and find a model which is, consistent with a mixture of collisional and background radiation excitation of the observed H$_2$ rotational levels. For singly ionized heavy elements we find eight components covering a velocity range of $\sim 110$ {\kms}. The \ion{H}{1} structure is expected to follow some combination of the singly ionized and neutral gas, but the 21cm absorption profile is considerably different. This may be because of the different extent and brightness distributions of the radio and optical background sources, and so the spin temperature derived by comparing the Ly$\alpha$ and 21cm line strengths has little physical meaning. The neutral and singly ionized heavy element line profiles also show significant differences, and so the dominant components in each appear to be physically distinct. Attempts to use the range of atomic masses to separate thermal and turbulent components of their Doppler widths were not generally successful. The velocity structure in all ionization stages up to $+3$, apart from the neutral heavy elements, is sufficiently complex that it is difficult to separate out the corresponding velocity components for different ionization levels and determine their column densities.