10,678 research outputs found
Collisional interaction limits between dark matters and baryons in `cooling flow' clusters
Presuming weak collisional interactions to exchange the kinetic energy
between dark matter and baryonic matter in a galaxy cluster, we re-examine the
effectiveness of this process in several `cooling flow' galaxy clusters using
available X-ray observations and infer an upper limit on the heavy dark matter
particle (DMP)proton cross section . With a relative
collisional velocity dependent power-law form of where , our inferred upper
limit is \sigma_0/m_{\rm x}\lsim 2\times10^{-25} {\rm cm}^2 {\rm GeV}^{-1}
with being the DMP mass. Based on a simple stability analysis of
the thermal energy balance equation, we argue that the mechanism of
DMPbaryon collisional interactions is unlikely to be a stable
nongravitational heating source of intracluster medium (ICM) in inner core
regions of `cooling flow' galaxy clusters.Comment: 8 pages, 2 figures, MNRAS accepte
General Polytropic Magnetofluid under Self-Gravity: Voids and Shocks
We study the self-similar magnetohydrodynamics (MHD) of a quasi-spherical
expanding void (viz. cavity or bubble) in the centre of a self-gravitating gas
sphere with a general polytropic equation of state. We show various analytic
asymptotic solutions near the void boundary in different parameter regimes and
obtain the corresponding void solutions by extensive numerical explorations. We
find novel void solutions of zero density on the void boundary. These new void
solutions exist only in a general polytropic gas and feature shell-type density
profiles. These void solutions, if not encountering the magnetosonic critical
curve (MCC), generally approach the asymptotic expansion solution far from the
central void with a velocity proportional to radial distance. We identify and
examine free-expansion solutions, Einstein-de Sitter expansion solutions, and
thermal-expansion solutions in three different parameter regimes. Under certain
conditions, void solutions may cross the MCC either smoothly or by MHD shocks,
and then merge into asymptotic solutions with finite velocity and density far
from the centre. Our general polytropic MHD void solutions provide physical
insight for void evolution, and may have astrophysical applications such as
massive star collapses and explosions, shell-type supernova remnants and hot
bubbles in the interstellar and intergalactic media, and planetary nebulae.Comment: 21 pages, 15 figures, accepted for publication on New Astronom
Adiabatic Perturbations in Homologous Conventional Polytropic Core Collapses of a Spherical Star
We perform a non-radial adiabatic perturbation analysis on homologous
conventional polytropic stellar core collapses. The core collapse features a
polytropic exponent relativistic gas under self-gravity of
spherical symmetry while three-dimensional perturbations involve an adiabatic
exponent with such that the Brunt-Visl buoyancy frequency does not
vanish. With proper boundary conditions, we derive eigenvalues and
eigenfunctions for different modes of oscillations. In reference to stellar
oscillations and earlier results, we examine behaviours of different modes and
the criterion for instabilities. The acoustic pmodes and surface fmodes
remain stable. For , convective instabilities appear as unstable
internal gravity gmodes. For , sufficiently low-order
internal gravity gmodes are stable, whereas sufficiently high-order
gmodes, which would have been stable in a static star, become unstable
during self-similar core collapses. For supernova explosions, physical
consequences of such inevitable gmode instabilities are speculated.Comment: 5 pages, 4 figures, accepted for publication in MNRA
Intermediate-Mass Black Holes in Globular Clusters
There have been reports of possible detections of intermediate-mass black
holes (IMBHs) in globular clusters (GCs). Empirically, there exists a tight
correlation between the central supermassive black hole (SMBH) mass and the
mean velocity dispersion of elliptical galaxies, "pseudobulges" and classical
bulges of spiral galaxies. We explore such a possible correlation for IMBHs in
spherical GCs. In our model of self-similar general polytropic quasi-static
dynamic evolution of GCs, a criterion of forming an IMBH is proposed. The key
result is M(BH) = L o^1/(1-n) where M(BH) is the IMBH mass, o is the GC mean
stellar velocity, L is a coefficient, and 2/3 < n < 1
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