1,852 research outputs found
Collapse of a Molecular Cloud Core to Stellar Densities: The First Three-Dimensional Calculations
We present results from the first three-dimensional calculations ever to
follow the collapse of a molecular cloud core (~ 10^{-18} g cm^{-3}) to stellar
densities (> 0.01 g cm^{-3}). The calculations resolve structures over 7 orders
of magnitude in spatial extent (~ 5000 AU - 0.1 R_\odot), and over 17 orders of
magnitude in density contrast. With these calculations, we consider whether
fragmentation to form a close binary stellar system can occur during the second
collapse phase. We find that, if the quasistatic core that forms before the
second collapse phase is dynamically unstable to the growth of non-axisymmetric
perturbations, the angular momentum extracted from the central regions of the
core, via gravitational torques, is sufficient to prevent fragmentation and the
formation of a close binary during the subsequent second collapse.Comment: ApJ Letters, in press (will appear in Nov 20 issue; available from
the ApJ Rapid Release web page). 7 pages, incl. 5 figures. Also available at
http://www.mpia-hd.mpg.de/theory/bat
The thermodynamics of collapsing molecular cloud cores using smoothed particle hydrodynamics with radiative transfer
We present the results of a series of calculations studying the collapse of
molecular cloud cores performed using a three-dimensional smoothed particle
hydr odynamics code with radiative transfer in the flux-limited diffusion
approximation. The opacities and specific heat capacities are identical for
each calculation. However, we find that the temperature evolution during the
simulations varies significantly when starting from different initial
conditions. Even spherically-symmetric clouds with different initial densities
show markedly different development. We conclude that simple barotropic
equations of state like those used in some previous calculations provide at
best a crude approximation to the thermal behaviour of the gas. Radiative
transfer is necessary to obtain accurate temperatures.Comment: 8 pages, 9 figures, accepted for publication in MNRA
Formation of Globular Clusters in Galaxy Mergers
We present a high-resolution simulation of globular cluster formation in a
galaxy merger. For the first time in such a simulation, individual star
clusters are directly identified and followed on their orbits. We
quantitatively compare star formation in the merger to that in the unperturbed
galaxies. The merging galaxies show a strong starburst, in sharp contrast to
their isolated progenitors. Most star clusters form in the tidal features. With
a mass range of --, they are
identified as globular clusters. The merger remnant is an elliptical galaxy.
Clusters with different mass or age have different radial distributions in the
galaxy. Our results show that the high specific frequency and bimodal
distribution of metallicity observed in elliptical galaxies are natural
products of gas-rich mergers, supporting a merger origin for the ellipticals
and their globular cluster systems.Comment: ApJL accepted, version with high quality color images can be found in
http://research.amnh.org/~yuexing/astro-ph/0407248.pd
Formation of the First Supermassive Black Holes
We consider the physical conditions under which supermassive black holes
could have formed inside the first galaxies. Our SPH simulations indicate that
metal-free galaxies with a virial temperature ~10^4 K and with suppressed H2
formation (due to an intergalactic UV background) tend to form a binary black
hole system which contains a substantial fraction (>10%) of the total baryonic
mass of the host galaxy. Fragmentation into stars is suppressed without
substantial H2 cooling. Our simulations follow the condensation of ~5x10^6
M_sun around the two centers of the binary down to a scale of < 0.1pc. Low-spin
galaxies form a single black hole instead. These early black holes lead to
quasar activity before the epoch of reionization. Primordial black hole
binaries lead to the emission of gravitational radiation at redshifts z>10 that
would be detectable by LISA.Comment: 11 pages, 9 figures, revised version, ApJ in press (October 10, 2003
Astrometric signatures of self-gravitating protoplanetary discs
We use high resolution numerical simulations to study whether gravitational
instabilities within circumstellar discs can produce astrometrically detectable
motion of the central star. For discs with masses of M_disc = 0.1 M_star, which
are permanantly stable against fragmentation, we find that the magnitude of the
astrometric signal depends upon the efficiency of disc cooling. Short cooling
times produce prominent filamentary spiral structures in the disc, and lead to
stellar motions that are potentially observable with future high precision
astrometric experiments. For a disc that is marginally unstable within radii of
\~10 au, we estimate astrometric displacements of 10-100 microarcsec on decade
timescales for a star at a distance of 100 pc. The predicted displacement is
suppressed by a factor of several in more stable discs in which the cooling
time exceeds the local dynamical time by an order of magnitude. We find that
the largest contribution comes from material in the outer regions of the disc
and hence, in the most pessimistic scenario, the stellar motions caused by the
disc could confuse astrometric searches for low mass planets orbiting at large
radii. They are, however, unlikely to present any complications in searches for
embedded planets orbiting at small radii, relative to the disc size, or Jupiter
mass planets or greater orbiting at large radii.Comment: 6 pages, 9 figures, accepted for publication in MNRA
Competitive accretion in embedded stellar cluster
We investigate the physics of gas accretion in young stellar clusters.
Accretion in clusters is a dynamic phenomenon as both the stars and the gas
respond to the same gravitational potential. Accretion rates are highly
non-uniform with stars nearer the centre of the cluster, where gas densities
are higher, accreting more than others. This competitive accretion naturally
results in both initial mass segregation and a spectrum of stellar masses.
Accretion in gas-dominated clusters is well modelled using a tidal-lobe radius
instead of the commonly used Bondi-Hoyle accretion radius. This works as both
the stellar and gas velocities are under the influence of the same
gravitational potential and are thus comparable. The low relative velocity that
results means that the tidal radius is smaller than the Bondi-Hoyle radius in
these systems. In contrast, when the stars dominate the potential and are
virialised, the Bondi-Hoyle radius is smaller than the tidal radius and thus
Bondi-Hoyle accretion is a better fit to the accretion rates.Comment: 11 pages, 11 figures, MNRAS in pres
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