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Incidence of HI 21-cm absorption in strong FeII systems at 0.5<z<1.50.5<z<1.5

Abstract

We present the results from our search for HI 21-cm absorption in a sample of 16 strong FeII systems (WrW_{\rm r}(MgII λ2796\lambda2796) 1.0\ge1.0 \AA\ and WrW_{\rm r}(FeII λ2600\lambda2600) or WFeIIW_{\rm FeII} 1\ge1 \AA) at 0.5<z<1.50.5<z<1.5 using the Giant Metrewave Radio Telescope and the Green Bank Telescope. We report six new HI 21-cm absorption detections from our sample, which have increased the known number of detections in strong MgII systems at this redshift range by 50\sim50%. Combining our measurements with those in the literature, we find that the detection rate of HI 21-cm absorption increases with WFeIIW_{\rm FeII}, being four times higher in systems with WFeIIW_{\rm FeII} 1\ge1 \AA\ compared to systems with WFeIIW_{\rm FeII} <1<1 \AA. The NN(HI) associated with the HI 21-cm absorbers would be 2×1020\ge 2 \times 10^{20} cm2^{-2}, assuming a spin temperature of 500\sim500 K (based on HI 21-cm absorption measurements of damped Lyman-α\alpha systems at this redshift range) and unit covering factor. We find that HI 21-cm absorption arises on an average in systems with stronger metal absorption. We also find that quasars with HI 21-cm absorption detected towards them have systematically higher E(BV)E(B-V) values than those which do not. Further, by comparing the velocity widths of HI 21-cm absorption lines detected in absorption- and galaxy-selected samples, we find that they show an increasing trend (significant at 3.8σ3.8\sigma) with redshift at z<3.5z<3.5, which could imply that the absorption originates from more massive galaxy haloes at high-zz. Increasing the number of HI 21-cm absorption detections at these redshifts is important to confirm various trends noted here with higher statistical significance.Comment: 17 pages, 10 figures, 8 tables, accepted for publication in MNRA

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