351 research outputs found
Two Body Relaxation in Simulated Cosmological Haloes
This paper aims at quantifying discreetness effects, born of finite particle
number, on the dynamics of dark matter haloes forming in the context of
cosmological simulations. By generalising the standard calculation of two body
relaxation to the case when the size and mass distribution are variable, and
parametrising the time evolution using established empirical relations, we find
that the dynamics of a million particle halo is noise-dominated within the
inner percent of the final virial radius. Far larger particle numbers (~ 10^8)
are required for the RMS perturbations to the velocity to drop to the 10 %
level there. The radial scaling of the relaxation time is simple and strong:
t_relax ~ r^2, implying that numbers >> 10^8 are required to faithfully model
the very inner regions; artificial relaxation may thus constitute an important
factor, contributing to the contradictory claims concerning the persistence of
a power law density cusp to the very centre. The cores of substructure haloes
can be many relaxation times old. Since relaxation first causes their expansion
before recontraction occurs, it may render them either more difficult or easier
to disrupt, depending on their orbital parameters. It may thus modify the
characteristics of the subhalo distribution and effects of interactions with
the parent. We derive simple closed form formulas for the characteristic
relaxation times, as well as for the weak N-scaling reported by Diemand et al.
when the main contribution comes from relaxing subhaloes (abridged).Comment: 11 Pages, 7 figs, Monthly Notices styl
From cusps to cores: a stochastic model
The cold dark matter model of structure formation faces apparent problems on
galactic scales. Several threads point to excessive halo concentration,
including central densities that rise too steeply with decreasing radius. Yet,
random fluctuations in the gaseous component can 'heat' the centres of haloes,
decreasing their densities. We present a theoretical model deriving this effect
from first principles: stochastic variations in the gas density are converted
into potential fluctuations that act on the dark matter; the associated force
correlation function is calculated and the corresponding stochastic equation
solved. Assuming a power law spectrum of fluctuations with maximal and minimal
cutoff scales, we derive the velocity dispersion imparted to the halo particles
and the relevant relaxation time. We further perform numerical simulations,
with fluctuations realised as a Gaussian random field, which confirm the
formation of a core within a timescale comparable to that derived analytically.
Non-radial collective modes enhance the energy transport process that erases
the cusp, though the parametrisations of the analytical model persist.
In our model, the dominant contribution to the dynamical coupling driving the
cusp-core transformation comes from the largest scale fluctuations. Yet, the
efficiency of the transformation is independent of the value of the largest
scale and depends weakly (linearly) on the power law exponent; it effectively
depends on two parameters: the gas mass fraction and the normalisation of the
power spectrum. This suggests that cusp-core transformations observed in
hydrodynamic simulations of galaxy formation may be understood and parametrised
in simple terms, the physical and numerical complexities of the various
implementations notwithstanding.Comment: Minor revisions to match version to appear in MNRAS; Section~2.3
largely rewritten for clarit
Regular and chaotic motion in softened gravitational systems
The stability of the dynamical trajectories of softened spherical
gravitational systems is examined, both in the case of the full -body
problem and that of trajectories moving in the gravitational field of
non-interacting background particles. In the latter case, for ,
some trajectories, even if unstable, had exceedingly long diffusion times,
which correlated with the characteristic e-folding timescale of the
instability. For trajectories of systems this timescale
could be arbitrarily large --- and thus appear to correspond to regular orbits.
For centrally concentrated systems, low angular momentum trajectories were
found to be systematically more unstable. This phenomenon is analogous to the
well known case of trajectories in generic centrally concentrated non-spherical
smooth systems, where eccentric trajectories are found to be chaotic. The
exponentiation times also correlate with the conservation of the angular
momenta along the trajectories. For up to a few hundred, the instability
timescales of -body systems and their variation with particle number are
similar to those of the most chaotic trajectories in inhomogeneous
non-interacting systems. For larger (up to a few thousand) the values of
the these timescales were found to saturate, increasing significantly more
slowly with . We attribute this to collective effects in the fully
self-gravitating problem, which are apparent in the time-variations of the time
dependent Liapunov exponents. The results presented here go some way towards
resolving the long standing apparent paradoxes concerning the local instability
of trajectories of gravitational systems (abridged).Comment: 16 pages, 11 figures, Monthly Notices styl
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