Radio observations of oh in the interstellar medium.
Existence of oh in interstellar medium, detected in radio absorption spectrum of cassiopeia-a
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Existence of oh in interstellar medium, detected in radio absorption spectrum of cassiopeia-a
IR emission lines possibly originating from galactic, interstellar and stellar hydrogen regions
Computation of equivalent widths of UV absorption lines of molecular hydrogen to be measured in spectra of early-type stars by future satellite telescope
Oort model of stars and interstellar cloud formation and destruction mathematically formulated, obtaining time-dependent cloud-mass spectrum equations
Cosmic rays leading to inflation of galactic magnetic fields produce halo of cosmic rays and field around galaxy
Interstellar gas-cosmic radiation relationship for inflation of galactic magnetic field and halo production around galaxy
IR emission lines possibly originating from galactic, interstellar and stellar hydrogen regions
Interstellar molecular hydrogen abundance and possible source from giant stars
Molecular hydrogen structure, considering planetary and stellar atmospheres and interstellar space
Thermal instabilities role in star formation, discussing intercloud medium, magnetic pressure and gravitational collapse
Electromagnetic radiation due to cosmic ray energy dissipation in interstellar hydrogen
Secular increase of stellar noncircular velocities in disk portions of galactic systems, noting gravitational disturbances
Photodissociation of hydrogen molecules in H I regions of interstellar medium, evaluating lifetime and density
Low- and high-dispersion ultraviolet spectra obtained by the IUE of the early B-type close binary V Puppis are reported. The continuum derived from the low-dispersion images is consistent with a solar abundance model of effective temperature 25,000 K and log surface gravity 4.0. The high-dispersion spectra show shallow double lines, representing Doppler-resolved stellar lines, which are broadened as expected for the fast rotational velocities given by Levato (1974). The equivalent widths of the silicon lines, however, do not agree with the temperature derived for the star, while the silicon and carbon absorptions indicate a disordered photosphere in the presence of circumstellar gas. Several interstellar lines are also observed for the first time.
A high-resolution spectroscopic investigation was made of interstellar lines of sodium. From identifications of D1 and D2 line components concentrations of interstellar sodium gas were studied. Some preliminary data are provided on the spatial distribution of stronger sodium concentrations.
The so-called anomalous cosmic ray component, which occurs at energies of about 10 MeV/nucleon and consists only of He, N, O, and Ne, has been a subject of interest for more than a decade. The origin of this component is generally considered to be interstellar neutral gas that is ionized and accelerated in the solar wind. The mechanism and the location for the acceleration, however, remains an unsolved problem. A model is used which includes the effects of gradient and curvature drifts and considers the implications of observed spatial gradients of the anomalous component for the location of the acceleration region. It is concluded that if drifts are important the acceleration region cannot lie at the solar poles. It is also concluded that there is no single region for the acceleration which can account for both the observed intensities and gradients in models which include drift effects.
Accurate Monte Carlo computations of the X-ray secondary electron heating, ionization, and excitation of H and He gas in interstellar space and in quasar emission-line clouds, are presented. The fraction of energy deposited in each form is sensitive to the background ionization fraction, x = n(H+)/n(Htot), and can affect the temperature, ionization state, and line emissivities at large depths in X-ray photoionized clouds. Analytic fits are provided for these energy fractions over the range 0.0001-1 for primary electron energies up to many keV. In both broad-line and narrow-line clouds, emission lines sensitive to the energy budget and electron density may be strongly affected.