457 research outputs found
Thermal Structure and Radius Evolution of Irradiated Gas Giant Planets
We consider the thermal structure and radii of strongly irradiated gas giant
planets over a range in mass and irradiating flux. The cooling rate of the
planet is sensitive to the surface boundary condition, which depends on the
detailed manner in which starlight is absorbed and energy redistributed by
fluid motion. We parametrize these effects by imposing an isothermal boundary
condition below the photosphere, and then constrain
from the observed masses and radii. We compute the dependence of
luminosity and core temperature on mass, and core entropy,
finding that simple scalings apply over most of the relevant parameter space.
These scalings yield analytic cooling models which exhibit power-law behavior
in the observable age range , and are confirmed by
time-dependent cooling calculations. We compare our model to the radii of
observed transiting planets, and derive constraints on . Only HD
209458 has a sufficiently accurate radius measurement that is
tightly constrained; the lower error bar on the radii for other planets is
consistent with no irradiation. More accurate radius and age measurements will
allow for a determination of the correlation of with the
equilibrium temperature, informing us about both the greenhouse effect and
day-night asymmetries.Comment: submitted to apj. 14 pages, 20 figure
R-modes in Neutron Stars with Crusts: Turbulent Saturation, Spin-down, and Crust Melting
Rossby waves (r-modes) have been suggested as a means to regulate the spin
periods of young or accreting neutron stars, and also to produce observable
gravitational wave radiation. R-modes involve primarily transverse,
incompressive motions of the star's fluid core. However, neutron stars gain
crusts early in their lives: therefore, r-modes also imply shear in the fluid
beneath the crust. We examine the criterion for this shear layer to become
turbulent, and derive the rate of dissipation in the turbulent regime. Unlike
dissipation from a viscous boundary layer, turbulent energy loss is nonlinear
in mode energy and can therefore cause the mode to saturate at amplitudes
typically much less than unity. This energy loss also reappears as heat below
the crust. We study the possibility of crust melting as well as its
implications for the spin evolution of low-mass X-ray binaries. Lastly, we
identify some universal features of the spin evolution that may have
observational consequences.Comment: 12 pages, 4 figures, submitted to Ap
Termination control of electronic phases in oxide thin films and interfaces: LaAlO 3/SrTiO 3(001)
A wealth of intriguing properties emerge in the seemingly simple system composed of the band insulators LaAlO 3 and SrTiO 3 such as a two-dimensional electron gas, superconductivity and magnetism. In this paper, we review the current insight obtained from first principles calculations on the mechanisms governing the behaviour of thin LaAlO 3 films on SrTiO 3(001). In particular, we explore the strong dependence of the electronic properties on the surface and interface termination, the finite film thickness, lattice polarization and defects. A further aspect that is addressed is how the electronic behaviour and functionality can be tuned by an SrTiO 3 capping layer, adsorbates and metallic contacts. Lastly, we discuss recent reports on the coexistence of magnetism and superconductivity in this system for what they might imply about the electronic structure of this system
Bulk viscosity in the nonlinear and anharmonic regime of strange quark matter
The bulk viscosity of cold, dense three-flavor quark matter is studied as a
function of temperature and the amplitude of density oscillations. The study is
also extended to the case of two different types of anharmonic oscillations of
density. We point several qualitative effects due to the anharmonicity,
although quantitatively they appear to be relatively small. We also find that,
in most regions of the parameter space, with the exception of the case of a
very large amplitude of density oscillations (i.e. 10% and above), nonlinear
effects and anharmonicity have a small effect on the interplay of the
nonleptonic and semileptonic processes in the bulk viscosity.Comment: 14 pages, 6 figures; v2: Appendix B is omitted, a few new discussions
added and some new references adde
Constraints on the mass and abundance of black holes in the Galactic halo: the high mass limit
We establish constraints on the mass and abundance of black holes in the
Galactic halo by determining their impact on globular clusters which are
conventionally considered to be little evolved. Using detailed Monte Carlo
simulations and simple analytic estimates, we conclude that, at Galactocentric
radius R~8 kpc, black holes with masses M_bh >~(1-3) x 10^6 M_sun can comprise
no more than a fraction f_bh ~ 0.025-0.05 of the total halo density. This
constraint significantly improves those based on disk heating and dynamical
friction arguments as well as current lensing results. At smaller radius, the
constraint on f_bh strengthens, while, at larger radius, an increased fraction
of black holes is allowed.Comment: 13 pages, 10 figures, revised version, in press, Monthly Notice
Reionization Constraints on the Contribution of Primordial Compact Objects to Dark Matter
Many lines of evidence suggest that nonbaryonic dark matter constitutes
roughly 30% of the critical closure density, but the composition of this dark
matter is unknown. One class of candidates for the dark matter is compact
objects formed in the early universe, with typical masses M between 0.1 and 1
solar masses to correspond to the mass scale of objects found with microlensing
observing projects. Specific candidates of this type include black holes formed
at the epoch of the QCD phase transition, quark stars, and boson stars. Here we
show that accretion onto these objects produces substantial ionization in the
early universe, with an optical depth to Thomson scattering out to z=1100 of
approximately tau=2-4 [f_CO\epsilon_{-1}(M/Msun)]^{1/2} (H_0/65)^{-1}, where
\epsilon_{-1} is the accretion efficiency \epsilon\equiv L/{\dot M}c^2 divided
by 0.1 and f_CO is the fraction of matter in the compact objects. The current
upper limit to the scattering optical depth, based on the anisotropy of the
microwave background, is approximately 0.4. Therefore, if accretion onto these
objects is relatively efficient, they cannot be the main component of
nonbaryonic dark matter.Comment: 12 pages including one figure, uses aaspp4, submitted to Ap
Radiation from condensed surface of magnetic neutron stars
Recent observations show that the thermal X-ray spectra of many isolated
neutron stars are featureless and in some cases (e.g., RX J1856.5-3754) well
fit by a blackbody. Such a perfect blackbody spectrum is puzzling since
radiative transport through typical neutron star atmospheres causes noticeable
deviation from blackbody. Previous studies have shown that in a strong magnetic
field, the outermost layer of the neutron star may be in a condensed solid or
liquid form because of the greatly enhanced cohesive energy of the condensed
matter. The critical temperature of condensation increases with the magnetic
field strength, and can be as high as 10^6 K (for Fe surface at B \sim 10^{13}
G or H surface at B \sim a few times 10^{14} G). Thus the thermal radiation can
directly emerge from the degenerate metallic condensed surface, without going
through a gaseous atmosphere. Here we calculate the emission properties
(spectrum and polarization) of the condensed Fe and H surfaces of magnetic
neutron stars in the regimes where such condensation may be possible. For a
smooth condensed surface, the overall emission is reduced from the blackbody by
less than a factor of 2. The spectrum exhibits modest deviation from blackbody
across a wide energy range, and shows mild absorption features associated with
the ion cyclotron frequency and the electron plasma frequency in the condensed
matter. The roughness of the solid condensate (in the Fe case) tends to
decrease the reflectivity of the surface, and make the emission spectrum even
closer to blackbody. We discuss the implications of our results for
observations of dim, isolated neutron stars and magnetars.Comment: 12 pages, 11 figures. ApJ, accepted (final version; eq.(3) corrected
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