The baryonic processes in galaxy evolution include gas infall onto galaxies to form neutral atomic hydrogen (HI), the conversion of HI to the molecular state (H$_2$), and, finally, the conversion of H$_2$ to stars. Understanding galaxy evolution thus requires understanding the evolution of both the stars, and the neutral atomic and molecular gas, the primary fuel for star-formation, in galaxies. For the stars, the cosmic star-formation rate density is known to peak in the redshift range $z \approx 1-3$, and to decline by an order of magnitude over the next $\approx 10$ billion years; the causes of this decline are not known. For the gas, the weakness of the hyperfine HI 21cm transition, the main tracer of the HI content of galaxies, has mea...
We use a pressure-based model for splitting cold hydrogen into its atomic (HI) and molecular (H2) co...
We investigate the far-infrared properties of galaxies selected via deep, narrow-band imaging of the...
The observed evolution of the gas fraction and its associated depletion time in main sequence (MS) g...
We use the Giant Metrewave Radio Telescope (GMRT) Cold-HI AT $z\approx1$ (CAT$z1$) survey, a 510 hr ...
We use observations from the Giant Metrewave Radio Telescope (GMRT) to measure the atomic hydrogen g...
© 2021. The American Astronomical Society. All rights reserved. This is the accepted manuscript vers...
The first epoch of galaxy formation is governed by the infall of neutral, pristine gas. These neutra...
We present new empirical constraints on the evolution of ${\rho }_{{{\rm{H}}}_{2}}$, the cosmologica...
We measure the neutral atomic hydrogen (H i) gas content of field galaxies at intermediate redshifts...
In this paper, we present an attempt to estimate the redshift evolution of the molecular to neutral ...
We study the evolution of the cold gas content of galaxies by splitting the interstellar medium into...
One of the major science goals of the Square Kilometre Array (SKA) is to understand the role played ...
We use observations made with the Giant Metrewave Radio Telescope (GMRT) to probe the neutral hydrog...
In the past decade, molecular gas observations have begun probing the high redshift universe in a sy...
We present IRAM Plateau de Bure interferometric detections of CO (J = 1 -> 0) emission from a 24 mu ...
We use a pressure-based model for splitting cold hydrogen into its atomic (HI) and molecular (H2) co...
We investigate the far-infrared properties of galaxies selected via deep, narrow-band imaging of the...
The observed evolution of the gas fraction and its associated depletion time in main sequence (MS) g...
We use the Giant Metrewave Radio Telescope (GMRT) Cold-HI AT $z\approx1$ (CAT$z1$) survey, a 510 hr ...
We use observations from the Giant Metrewave Radio Telescope (GMRT) to measure the atomic hydrogen g...
© 2021. The American Astronomical Society. All rights reserved. This is the accepted manuscript vers...
The first epoch of galaxy formation is governed by the infall of neutral, pristine gas. These neutra...
We present new empirical constraints on the evolution of ${\rho }_{{{\rm{H}}}_{2}}$, the cosmologica...
We measure the neutral atomic hydrogen (H i) gas content of field galaxies at intermediate redshifts...
In this paper, we present an attempt to estimate the redshift evolution of the molecular to neutral ...
We study the evolution of the cold gas content of galaxies by splitting the interstellar medium into...
One of the major science goals of the Square Kilometre Array (SKA) is to understand the role played ...
We use observations made with the Giant Metrewave Radio Telescope (GMRT) to probe the neutral hydrog...
In the past decade, molecular gas observations have begun probing the high redshift universe in a sy...
We present IRAM Plateau de Bure interferometric detections of CO (J = 1 -> 0) emission from a 24 mu ...
We use a pressure-based model for splitting cold hydrogen into its atomic (HI) and molecular (H2) co...
We investigate the far-infrared properties of galaxies selected via deep, narrow-band imaging of the...
The observed evolution of the gas fraction and its associated depletion time in main sequence (MS) g...