The temperature of the neutral Interstellar Medium in the Galaxy
Narendra Nath Patra, Nirupam Roy
arXiv:2403.11653v1 Announce Type: new
Abstract: Atomic Hydrogen-21 cm transition (HI) is an excellent tracer to study and understand the properties of the atomic gas in the Galaxy. Using the Westerbork Synthesis Radio Telescope (WSRT), we observed 12 quasar sightlines to detect galactic HI in absorption. We achieve an optical depth RMS of $sim 1-2 times 10^{-3}$, essential to detect the Warm Neutral Medium (WNM). We detect HI absorption in all our sightlines except along 1006+349, for which we set a strict upper limit on the spin temperature as $langle T_s rangle > 570$ K. We find around 50% of our sightlines have $langle T_s rangle > 500$ K, indicating a WNM dominance. Further, we calculate an upper limit of the CNM fraction along our sightlines and find a median CNM fraction of $sim 0.12$. With our observations, we reconfirm the existence of a threshold column density of $sim 2 times 10^{20} cm^{-2}$ to form CNM in the ISM. Using a two-temperature model of the HI disk, we explore the distribution of spin temperature in the Galactic ISM. We find that a simple fixed axisymmetric two-temperature model could not produce either the observed column density or the integral optical depth. This indicates the existence of a more complex distribution of spin temperatures in the Galaxy.arXiv:2403.11653v1 Announce Type: new
Abstract: Atomic Hydrogen-21 cm transition (HI) is an excellent tracer to study and understand the properties of the atomic gas in the Galaxy. Using the Westerbork Synthesis Radio Telescope (WSRT), we observed 12 quasar sightlines to detect galactic HI in absorption. We achieve an optical depth RMS of $sim 1-2 times 10^{-3}$, essential to detect the Warm Neutral Medium (WNM). We detect HI absorption in all our sightlines except along 1006+349, for which we set a strict upper limit on the spin temperature as $langle T_s rangle > 570$ K. We find around 50% of our sightlines have $langle T_s rangle > 500$ K, indicating a WNM dominance. Further, we calculate an upper limit of the CNM fraction along our sightlines and find a median CNM fraction of $sim 0.12$. With our observations, we reconfirm the existence of a threshold column density of $sim 2 times 10^{20} cm^{-2}$ to form CNM in the ISM. Using a two-temperature model of the HI disk, we explore the distribution of spin temperature in the Galactic ISM. We find that a simple fixed axisymmetric two-temperature model could not produce either the observed column density or the integral optical depth. This indicates the existence of a more complex distribution of spin temperatures in the Galaxy.