In this paper, we combine the stellar spectral synthesis code STARBURST99, the nebular modeling code MAPPINGS IIIq, a one-dimensional dynamical evolution model of H II regions around massive clusters of young stars, and a simplified model of synchrotron emissivity to produce purely theoretical self-consistent synthetic spectral energy distributions (SEDs) for (solar metallicity) starbursts lasting ± 10<sup>8</sup> yr. These SEDs extend from the Lyman limit to beyond 21 cm. We find that two ISM parameters control the form of the SED: the pressure in the diffuse phase of the ISM (or, equivalently, its density), and the molecular cloud dissipation timescale. In particular, the shape of the far-infrared (dust re-emission) bump is strongly depen...
We apply the da Cunha et al. (2008, MNRAS, 388, 1595) model of the spectral energy distrib...
To understand and interpret the observed spectral energy distributions (SEDs) of starbursts, theoret...
We examine, froma theoretical viewpoint, how the physical parameters of H ii regions are controlled ...
In this paper, we combine the stellar spectral synthesis code STARBURST99, the nebular modeling code...
In this paper, we combine the stellar spectral synthesis code STARBURST99, the nebular modeling code...
In this paper, we combine the stellar spectral synthesis code STARBURST 99, the nebular modelling co...
We combine the stellar spectral synthesis code Starburst99, the nebular modeling code MAPPINGS III a...
Using the codes STARBURST 99, and MAPPINGS 3r, we construct a set of theoretical spectral energy dis...
This thesis presents a starburst model for far-infrared/sub-millimeter/millimeter (FIR/sub-mm/mm) ...
We build, as far as theory will permit, self-consistent model H II regions around central clusters o...
We build, as far as theory will permit, self-consistent model H II regions around central clusters o...
We examine, from a theoretical viewpoint, how the physical parameters of H II regions are controlled...
We apply the da Cunha et al. (2008, MNRAS, 388, 1595) model of the spectral energy distribution (SED...
We examine, from a theoretical viewpoint, how the physical parameters of H II regions are controlled...
Aims. By using the spectral energy distribution (SED) from the near-infrared to the radio of a stati...
We apply the da Cunha et al. (2008, MNRAS, 388, 1595) model of the spectral energy distrib...
To understand and interpret the observed spectral energy distributions (SEDs) of starbursts, theoret...
We examine, froma theoretical viewpoint, how the physical parameters of H ii regions are controlled ...
In this paper, we combine the stellar spectral synthesis code STARBURST99, the nebular modeling code...
In this paper, we combine the stellar spectral synthesis code STARBURST99, the nebular modeling code...
In this paper, we combine the stellar spectral synthesis code STARBURST 99, the nebular modelling co...
We combine the stellar spectral synthesis code Starburst99, the nebular modeling code MAPPINGS III a...
Using the codes STARBURST 99, and MAPPINGS 3r, we construct a set of theoretical spectral energy dis...
This thesis presents a starburst model for far-infrared/sub-millimeter/millimeter (FIR/sub-mm/mm) ...
We build, as far as theory will permit, self-consistent model H II regions around central clusters o...
We build, as far as theory will permit, self-consistent model H II regions around central clusters o...
We examine, from a theoretical viewpoint, how the physical parameters of H II regions are controlled...
We apply the da Cunha et al. (2008, MNRAS, 388, 1595) model of the spectral energy distribution (SED...
We examine, from a theoretical viewpoint, how the physical parameters of H II regions are controlled...
Aims. By using the spectral energy distribution (SED) from the near-infrared to the radio of a stati...
We apply the da Cunha et al. (2008, MNRAS, 388, 1595) model of the spectral energy distrib...
To understand and interpret the observed spectral energy distributions (SEDs) of starbursts, theoret...
We examine, froma theoretical viewpoint, how the physical parameters of H ii regions are controlled ...