ﻻ يوجد ملخص باللغة العربية
Observations of the four $^{2}Pi_{3/2},~J = 3/2$~ground state transitions of the hydroxyl radical (OH) have emerged as an informative tracer of molecular gas in the Galactic ISM. We discuss an OH spectral feature known as the `flip, in which the satellite lines at 1612 and 1720,MHz flip -- one from emission to absorption and the other the reverse -- across a closely blended double feature. We highlight 30 examples of the flip from the literature, 27 of which exhibit the same orientation with respect to velocity: the 1720,MHz line is seen in emission at more negative velocities. These same examples are also observed toward bright background continuum, many (perhaps all) show stimulated emission, and 23 of these are coincident in on-sky position and velocity with Htextsc{ii}~radio recombination lines. To explain these remarkable correlations we propose that the 1720,MHz stimulated emission originates in heated and compressed post-shock gas expanding away from a central Htextsc{ii}~region, which collides with cooler and more diffuse gas hosting the 1612,MHz stimulated emission. The foreground gas dominates the spectrum due to the bright central continuum, hence the expanding post-shock gas is blue-shifted relative to the stationary pre-shock gas. We employ non-LTE excitation modelling to examine this scenario, and find that indeed FIR emission from warm dust adjacent to the Htextsc{ii}~region radiatively pumps the 1612 MHz line in the diffuse, cool gas ahead of the expanding shock front, while collisional pumping in the warm, dense shocked gas inverts the 1720 MHz line.
We investigate the turbulence driving mode of ionizing radiation from massive stars on the surrounding interstellar medium (ISM). We run hydrodynamical simulations of a turbulent cloud impinged by a plane-parallel ionization front. We find that the i
The hydroxyl radical (OH) is found in various environments within the interstellar medium (ISM) of the Milky Way and external galaxies, mostly either in diffuse interstellar clouds or in the warm, dense environments of newly formed low-mass and high-
Context. The derived physical parameters for young HII regions are normally determined assuming the emission region to be optically thin. However, this assumption is unlikely to hold for young HII regions such as hyper-compact HII(HCHII) and ultra-co
Magnetic fields play an important role during star formation. Direct magnetic field strength observations have proven specifically challenging in the extremely dynamic protostellar phase. Because of their occurrence in the densest parts of star formi
Because of their relatively simple morphology, bubble HII regions have been instrumental to our understanding of star formation triggered by HII regions. With the far-infrared (FIR) spectral coverage of the Herschel satellite, we can access the wavel