1992
DOI: 10.1086/186494
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A determination of the mass of Sagittarius A* from its radio spectral and source size measurements

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Cited by 30 publications
(16 citation statements)
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“…This detection is exciting for several reasons. First, it lies in a region of the spectrum where the intrinsic source size should become apparent over scatter broadening by the intervening screen (Melia, Jokipii, & Narayanan 1992). Second, this component is sufficiently bright to be detected with VLBI techniques at even shorter wavelengths, and third, Sgr A* is sufficiently close that the size scale where general relativistic effects are significant could be resolved with VLBI at submillimeter wavelengths.…”
Section: ϫ3mentioning
confidence: 99%
“…This detection is exciting for several reasons. First, it lies in a region of the spectrum where the intrinsic source size should become apparent over scatter broadening by the intervening screen (Melia, Jokipii, & Narayanan 1992). Second, this component is sufficiently bright to be detected with VLBI techniques at even shorter wavelengths, and third, Sgr A* is sufficiently close that the size scale where general relativistic effects are significant could be resolved with VLBI at submillimeter wavelengths.…”
Section: ϫ3mentioning
confidence: 99%
“…The sharp cutoff at the lowa S ∝ n a ∼ 0.19-0.34 n frequency end (∼0.5 GHz) appears to be due to free-free absorption in the ionized gas along the line of sight (Davies, Walsh, & Booth 1976). In the millimeter region, a spectral bump (Zylka, Mezger, & Lesch 1992;Zylka et al 1995) has been confirmed by simultaneous 20 cm to 1 mm radio observations (Falcke et al 1998), suggesting that a distinct emission component surrounds the event horizon, since the highest frequencies appear to correspond to the smallest spatial scales (Melia, Jokipii, & Narayanan 1992;Melia 1992Melia , 1994Narayan, Yi, & Mahadevan 1995;Falcke et al 1998;. The spectrum turns over in the submillimeter range.…”
mentioning
confidence: 93%
“…Other sce-11 n p 2 # 10 narios, such as the jet model (Falcke & Markoff 2000) and the advection-dominated accretion flow disk model (Narayan, Yi, & Mahadevan 1995), also require that the medium goes transparent across this range of frequencies. The fortunate aspect about this transition is that it happens to occur at about the same set of frequencies where the scatter broadening in the interstellar medium decreases below the intrinsic source size (see also Melia, Jokipii, & Narayanan 1992). showed that taking this effect into account, as well as the finite achievable telescope resolution, the shadow of Sgr A* should be observable with very long baseline interferometry (VLBI) below ∼1 mm; it should be quite distinctive at 0.6 mm.…”
Section: Introductionmentioning
confidence: 99%