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Insu Yi

Publications and source records attributed to Insu Yi.

39 records · Page 3Linked to original sources

Advection-Dominated Accretion Model for Sagittarius A$^*$: Evidence for a $10^6\msun$ Black Hole at the Galactic Center

The enigmatic radio source Sagittarius A* at the centre of our Galaxy appears to be a low-luminosity version of active galactic nuclei in other galaxies. By analogy with active galactic nuclei models, it has been proposed that Sgr A* may be a massive accreting black holes. The black hole hypothesis is, however, problematic because no model of Sgr A* has been able to explain the observed spectrum in any self-consistent way, and there is no consensus on either the mass of the black hole or the mass accretion rate. Sgr A* has been observed in the radio, sub-mm, infrared, and X-ray bands, and the various various detections and flux upper limits cover more than ten decades of frequency, from $ν\sles\ 10^9$ Hz (meter wavelength radio bands) up to $ν \sgreat\ 10^{19}$ Hz (150 keV X-rays). We present a robust model of Sgr A* in which a million solar mass black hole accretes at the rate of a few $\times10^{-6}$ solar masses per year. This model fits the entire spectrum self-consistently. The unique feature of the model is that the flow is advection-dominated, i.e. most of the energy viscously dissipated in the differentially rotating flow is carried along with the gas and lost through the horizon. The apparent success of this model in explaining the data may be considered ``proof'' that horizons are real and that a massive black hole does exist at the Galactic center.

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Advection-Dominated Accretion: Self-Similarity and Bipolar Outflows

We consider axisymmetric viscous accretion flows where a fraction f of the viscously dissipated energy is advected with the accreting gas as stored entropy and a fraction 1-f is radiated. When f is small (i.e. very little advection), our solutions resemble standard thin disks in many respects except that they have a hot tenuous corona above. In the opposite {\it advection-dominated} limit ($f\rightarrow1$), the solutions approach nearly spherical accretion. The gas is almost at virial temperature, rotates at much below the Keplerian rate, and the flow is much more akin to Bondi accretion than to disk accretion. We compare our exact self-similar solutions with approximate solutions previously obtained using a height-integrated system of equations. We conclude that the height- integration approximation is excellent for a wide range of conditions. We find that the Bernoulli parameter is positive in all our solutions, especially close to the rotation axis. This effect is produced by viscous transport of energy from small to large radii and from the equator to the poles. In addition, all the solutions are convectively unstable and the convection is especially important near the rotation axis. For both reasons we suggest that a bipolar outflow will develop along the axis of the flows, fed by material from the the surface layers of the equatorial inflow.

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Advection-Dominated Accretion: A Self-Similar Solution

We consider viscous rotating accretion flows in which most of the viscously dissipated energy is stored as entropy rather than being radiated. Such advection-dominated flows may occur when the optical depth is either very small or very large. We obtain a family of self-similar solutions where the temperature of the accreting gas is nearly virial and the flow is quasi-spherical. The gas rotates at much less than the Keplerian angular velocity; therefore, the central stars in such flows will cease to spin up long before they reach the break-up limit. Further, the Bernoulli parameter is positive, implying that advection-dominated flows are susceptible to producing outflows. Convection is likely in many of these flows and, if present, will tend to enhance the above effects. We suggest that advection-dominated accretion may provide an explanation for the slow spin rates of accreting stars and the widespread occurrence of outflows and jets in accreting systems.

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