2009A&A...506..661L

We aim to understand the nature of the absorbing neutral gas in the galaxies hosting high-redshift long-duration gamma-ray bursts (GRBs) and to determine their physical conditions.A detailed analysis of high-quality VLT/UVES spectra of the optical afterglow of GRB050730 and other Swift-era bursts is presented.We report the detection of a significant number of previously unidentified allowed transition lines of Fe⁺, involving the fine structure of the ground term (⁶D_7/2, ⁶D_5/2, ⁶D_3/2, ⁶D_1/2) and that of other excited levels (⁴F_9/2, ⁴F_7/2, ⁴F_5/2, ⁴F_3/2, ⁴D_7/2, ⁴D_5/2), from the z_ abs_=3.969, logN(H⁰)=22.10, damped Lyman-α (DLA) system located in the host galaxy of GRB050730. No molecular hydrogen (H₂) is detected down to a molecular fraction of logf←8.0. We derive accurate metal abundances for Fe⁺, S⁺, N⁰, Ni⁺, and, for the first time in this system, Si⁺ and Ar⁰. The absorption lines are best-fit as a single narrow velocity component at z_abs=3.96857. The time-dependent evolution of the observed Fe⁺ energy-level populations is modelled by assuming the excitation mechanism is fluorescence following excitation by ultraviolet photons emitted by the afterglow of GRB050730. This UV pumping model successfully reproduces the observations, yielding a total Fe⁺ column density of logN=15.49±0.03, a burst/cloud distance (defined to the near-side of the cloud) of d=440±30pc, and a linear cloud size of l=520⁺²⁴⁰_–190pc. This application of our photo-excitation code demonstrates that burst/DLA distances can be determined without strong constraints on absorption-line variability provided enough energy levels are detected. From the cloud size, we infer a particle density of n_H≃5-15cm^–3.We discuss these results in the context of no detections of H₂ and CI lines (with log N(C⁰)/N(S⁺)←3) in a sample of seven z>1.8 GRB host galaxies observed with VLT/UVES. We show that the lack of H₂ can be explained by the low metallicities, [X/H]←1, low depletion factors, and, at most, moderate particle densities of the systems. This points to a picture where GRB-DLAs typically exhibiting very high H⁰ column densities are diffuse metal-poor atomic clouds with high kinetic temperatures, T_kin>1000K, and large physical extents, l>100pc. The properties of GRB-DLAs observed at high spectral resolution towards bright GRB afterglows differ markedly from the high metal and dust contents of GRB-DLAs observed at lower resolution. This difference likely results from the effect of a bias, against systems of high metallicity and/or close to the GRB, due to dust obscuration in the magnitude-limited GRB afterglow samples observed with high-resolution spectrographs.