1969
DOI: 10.1086/180305
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The Spectra of Opaque Radio Sources

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Cited by 546 publications
(414 citation statements)
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“…The brightness temperature is well below the inverse-Compton limit of 10 12 K (Kellermann & Pauliny-Toth 1969) and is consistent with the equipartition limit of ∼10 11 K (Readhead 1994). Additionally, we fitted a circular Gaussian distribution to the "hot spot" by only deleting the  components within this region and measured a brightness temperature of about 10 7 K.…”
Section: Tanami Vlbi Imagesupporting
confidence: 70%
“…The brightness temperature is well below the inverse-Compton limit of 10 12 K (Kellermann & Pauliny-Toth 1969) and is consistent with the equipartition limit of ∼10 11 K (Readhead 1994). Additionally, we fitted a circular Gaussian distribution to the "hot spot" by only deleting the  components within this region and measured a brightness temperature of about 10 7 K.…”
Section: Tanami Vlbi Imagesupporting
confidence: 70%
“…In this model, the intrinsic brightness temperatures cannot exceed 10 11 -10 12 K (Kellermann & Pauliny-Toth 1969;Readhead 1994). Typical Doppler boosting is expected to be able to raise this temperature by a factor of ∼10 (see also Hovatta et al 2009;Lister et al 2013).…”
Section: Introductionmentioning
confidence: 94%
“…It is commonly considered that inverse Compton losses limit the intrinsic brightness temperature for incoherent synchrotron sources, such as AGNs, to about 10 12 K (Kellermann & Pauliny-Toth 1969). In the case of a strong flare, the "Compton catastrophe" is calculated to take about one day to drive the brightness temperature below 10 12 K. Moreover, Readhead (1994) has argued that, for sources near the equipartition of energy between the magnetic field and radiating particles, a more accurate upper value for the intrinsic brightness temperature is about 10 11 K (see also Lähteenmäki et al 1999;Hovatta et al 2009), which is often called the equipartition brightness temperature.…”
Section: Brightness Temperaturementioning
confidence: 99%
“…The synchrotron process encounters an absolute limit when the radiating electrons are cooled by inverse Compton scattering on their own emission. This 'inverse Compton catastrophe' sets in at about 10 12 K (Kellermann & Pauliny-Toth 1969). Assuming equipartition of the energy densities between the radiating particles and the magnetic field and using the magnetic field estimate from the spectral peak caused by synchrotron self-absorption, Readhead (1994) has derived an upper limit on the synchrotron brightness temperature of a few times 10 11 K (depending on the spectral index).…”
Section: Vlbi and Emission Processmentioning
confidence: 99%