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We have used the Westerbork Synthesis Radio Telescope to detect HI 21cm absorption at $z sim 0.7645$ in the gravitational lens system towards PMN J0134-0931. The 21cm profile has two broad components, with peak optical depths of $0.047 pm 0.007$ and $0.039 pm 0.007$, at heliocentric redshifts $0.76470 pm 0.00006$ and $0.76348 pm 0.00006$, respectively. The redshift of the stronger component matches that of CaII H and K absorption detected earlier. The absorption has a total velocity width of $sim 500$ km/s (between nulls) and an equivalent width of $7.1 pm 0.08$ km/s. This would imply a total HI column density of $2.6 pm 0.3 times 10^{21}$ per cm$^2$, for a spin temperature of 200 K and a covering factor of unity. The high estimated HI column density is consistent with the presence of large amounts of dust at the lens redshift; the intervening dust could be responsible for the extremely red colour of the background quasar.
We report the GMRT detection of HI 21cm absorption from the $z sim 3.39$ damped Lyman-$alpha$ absorber (DLA) towards PKS 0201+113, the highest redshift at which 21cm absorption has been detected in a DLA. The absorption is spread over $sim 115$ km s$
We present an HI 21cm absorption study of a sample of 26 radio-loud active galactic nuclei (AGN) at $0.25 < z < 0.4$ carried out with the Karl G. Jansky Very Large Array. Our aim was to study the rate of incidence of HI in various classes of radio AG
We report the serendipitous discovery of a quadruply-lensed source behind the z=0.095 edge-on disk galaxy 2MASXJ13170000-1405187, based on public imaging survey data from Pan-STARRS PS1 and the VISTA Hemisphere Survey. Follow-up imaging from Magellan
We address the issue of anomalous image flux ratios seen in the double-image gravitational lens JVAS B0218+357. From the multi-frequency observations presented in a recent study (Mittal et al. 2006) and several previous observations made by other aut
We present the results from our search for HI 21-cm absorption in a sample of 16 strong FeII systems ($W_{rm r}$(MgII $lambda2796$) $ge1.0$ AA and $W_{rm r}$(FeII $lambda2600$) or $W_{rm FeII}$ $ge1$ AA) at $0.5<z<1.5$ using the Giant Metrewave Radio