Exact shearing box solutions of magnetohydrodynamic flows with resistivity, viscosity and cooling
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY 381:1 (2007) 319-333
Migration and the formation of systems of hot super-earths and neptunes
Astrophysical Journal 654:2 I (2007) 1110-1120
An exact, three-dimensional, time-dependent wave solution in local keplerian flow
Astrophysical Journal 652:2 I (2006) 1020-1027
Abstract:
We present an exact three-dimensional wave solution to the shearing-sheet equations of motion. The existence of this solution argues against transient amplification as a route to turbulence in unmagnetized disks. Moreover, because the solution covers an extensive dynamical range in wavenumber space, it is an excellent test of the dissipative properties of numerical codes. © 2006. The American Astronomical Society. All rights reserved.The RAVE Survey: Constraining the Local Galactic Escape Speed
ArXiv astro-ph/0611671 (2006)
Abstract:
We report new constraints on the local escape speed of our Galaxy. Our analysis is based on a sample of high velocity stars from the RAVE survey and two previously published datasets. We use cosmological simulations of disk galaxy formation to motivate our assumptions on the shape of the velocity distribution, allowing for a significantly more precise measurement of the escape velocity compared to previous studies. We find that the escape velocity lies within the range $498\kms < \ve < 608 \kms$ (90 per cent confidence), with a median likelihood of $544\kms$. The fact that $\ve^2$ is significantly greater than $2\vc^2$ (where $\vc=220\kms$ is the local circular velocity) implies that there must be a significant amount of mass exterior to the Solar circle, i.e. this convincingly demonstrates the presence of a dark halo in the Galaxy. For a simple isothermal halo, one can calculate that the minimum radial extent is $\sim58$ kpc. We use our constraints on $\ve$ to determine the mass of the Milky Way halo for three halo profiles. For example, an adiabatically contracted NFW halo model results in a virial mass of $1.42^{+1.14}_{-0.54}\times10^{12}M_\odot$ and virial radius of $305^{+66}_{-45}$ kpc (90 per cent confidence). For this model the circular velocity at the virial radius is $142^{+31}_{-21}\kms$. Although our halo masses are model dependent, we find that they are in good agreement with each other.Clues from microquasars to the origin of radio-loudness of quasars
ArXiv astro-ph/0611166 (2006)