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1975
DOI: 10.1093/mnras/170.1.41
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The Radio and Infrared Spectrum of Early-type Stars Undergoing Mass Loss

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Cited by 628 publications
(587 citation statements)
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“…These power laws can be interpreted as free-free emission: optically thin for the positive slopes between 2 and 4.5 µm in April 17 and 23, and the negative slope (λ −0.6 ) corresponding to the intermediate regime between optically thin and optically thick free-free emission. This −0.6 slope is the exact theoretical spectral index for the free-free emission from an ionized homogeneous wind flowing out from a star with a spherical expansion and at a constant velocity (Panagia & Felli 1975;Wright & Barlow 1975). This is characteristic of hot stars with strong winds, such as O and WR stars (Cohen et al 1975).…”
Section: Data Fittingmentioning
confidence: 93%
“…These power laws can be interpreted as free-free emission: optically thin for the positive slopes between 2 and 4.5 µm in April 17 and 23, and the negative slope (λ −0.6 ) corresponding to the intermediate regime between optically thin and optically thick free-free emission. This −0.6 slope is the exact theoretical spectral index for the free-free emission from an ionized homogeneous wind flowing out from a star with a spherical expansion and at a constant velocity (Panagia & Felli 1975;Wright & Barlow 1975). This is characteristic of hot stars with strong winds, such as O and WR stars (Cohen et al 1975).…”
Section: Data Fittingmentioning
confidence: 93%
“…Although such spectral indices may also arise from ionized jets, the flux density in IRAS 16333−4807 is too high to be explained in this way with reasonable mass-loss rates. As in the case of IRAS 17347−3139 (de Gregorio-Monsalvo et al 2004), a mass loss rate ofṀ ≃ 10 −4 (D/kpc) 3/2 M⊙ yr −1 , where D is the distance to the source, would be required for a spherical ionized wind to explain the observed radio continuum emission (Wright & Barlow 1975;Panagia & Felli 1975). Even assuming a collimated wind, and following the formulation by Reynolds (1986), the required mass loss rate is as high as ≃ 3 × 10 −6 (D/kpc) 3/2 M⊙ yr −1 , and this is a lower limit, assuming that the wind is fully ionized.…”
Section: The Nature Of Iras 16333−4807 As a Planetary Nebulamentioning
confidence: 98%
“…For emission from a spherically symmetric wind with an arbitrary µ a -n r density profile the expected spectral dependence of free-free emission is (Wright & Barlow 1975). n turn is the frequency where the wind becomes partially optically thick, and is determined by the radius of the inner boundary of the ionized envelope.…”
Section: Estimating the Free-free Emission Spectrummentioning
confidence: 99%