766 research outputs found
Nonlinear dynamos at infinite magnetic Prandtl number
The dynamo instability is investigated in the limit of infinite magnetic
Prandtl number. In this limit the fluid is assumed to be very viscous so that
the inertial terms can be neglected and the flow is slaved to the forcing. The
forcing consist of an external forcing function that drives the dynamo flow and
the resulting Lorentz force caused by the back reaction of the magnetic field.
The flows under investigation are the Archontis flow, and the ABC flow forced
at two different scales. The investigation covers roughly three orders of
magnitude of the magnetic Reynolds number above onset. All flows show a weak
increase of the averaged magnetic energy as the magnetic Reynolds number is
increased. Most of the magnetic energy is concentrated in flat elongated
structures that produce a Lorentz force with small solenoidal projection so
that the resulting magnetic field configuration was almost force-free. Although
the examined system has zero kinetic Reynolds number at sufficiently large
magnetic Reynolds number the structures are unstable to small scale
fluctuations that result in a chaotic temporal behavior
Vacuum shell in the Schwarzschild-de Sitter world
We construct the classification scheme for all possible evolution scenarios
and find the corresponding global geometries for dynamics of a thin spherical
vacuum shell in the Schwarzschild-de Sitter metric. This configuration is
suitable for the modelling of vacuum bubbles arising during cosmological phase
transitions in the early Universe. The distinctive final types of evolution
from the local point of view of a rather distant observer are either the
unlimited expansion of the shell or its contraction with a formation of black
hole (with a central singularity) or wormhole (with a baby universe in
interior).Comment: 15 pages, 8 figure
Atomic Collapse and Quasi-Rydberg States in Graphene
Charge impurities in graphene can host an infinite family of Rydberg-like
resonance states of massless Dirac particles. These states, appearing for
supercritical charge, are described by Bohr-Sommerfeld quantization of
collapsing classical trajectories that descend on point charge, in analogy to
Rydberg states relation with planetary orbits. We argue that divalent and
trivalent charge impurities in graphene is an ideal system for realization of
this atomic collapse regime. Strong coupling of these states to the Dirac
continuum via Klein tunneling leads to striking resonance effects with direct
signatures in transport, local properties and enhancement of the Kondo effect.Comment: 5 pages, 4 figure
Creation of Dirac Particles in the Presence of a Constant Electric Field in an Anisotropic Bianchi I Universe
In this article we compute the density of Dirac particles created by a
cosmological anisotropic Bianchi I universe in the presence of a constant
electric field. We show that the particle distribution becomes thermal when one
neglects the electric interaction.Comment: 9 page
Gravitational mechanisms to self-tune the cosmological constant: obstructions and ways forward
Gravitational models of self-tuning are those in which vacuum energy has no observable effect on spacetime curvature, even though it is a priori unsuppressed below the cut-off. We complement Weinberg's no go theorem by studying field theoretic completions of self-adjustment allowing for broken translations as well as other generalisations, and identify new obstructions. Our analysis uses a very general Källén-Lehmann spectral representation of the exchange amplitude for conserved sources of energy-momentum and exploits unitarity and Lorentz invariance to show that a transition from self-tuning of long wavelength sources to near General Relativity on shorter scales is generically not possible. We search for novel ways around our obstructions and highlight two interesting possibilities. The first is an example of a unitary field configuration on anti-de Sitter space with the desired transition from self-tuning to GR. A second example is motivated by vacuumenergy sequestering
Zeldovich flow on cosmic vacuum background: new exact nonlinear analytical solution
A new exact nonlinear Newtonian solution for a plane matter flow superimposed
on the isotropic Hubble expansion is reported. The dynamical effect of cosmic
vacuum is taken into account. The solution describes the evolution of nonlinear
perturbations via gravitational instability of matter and the termination of
the perturbation growth by anti-gravity of vacuum at the epoch of transition
from matter domination to vacuum domination. On this basis, an `approximate' 3D
solution is suggested as an analog of the Zeldovich ansatz.Comment: 9 pages, 1 figure
Vacuum Polarization and Screening of Supercritical Impurities in Graphene
Screening of charge impurities in graphene is analyzed using the exact
solution for vacuum polarization obtained from the massless Dirac-Kepler
problem. For the impurity charge below certain critical value no density
perturbation is found away from the impurity, in agreement with the linear
response theory result. For supercritical charge, however, the polarization
distribution is shown to have a power law profile, leading to screening of the
excess charge at large distances. The Dirac-Kepler scattering states give rise
to standing wave oscillations in the local density of states which appear and
become prominent in the supercritical regime.Comment: 5 pages, 2 figure
Elastic scattering theory and transport in graphene
Electron properties of graphene are described in terms of Dirac fermions.
Here we thoroughly outline the elastic scattering theory for the
two-dimensional massive Dirac fermions in the presence of an axially symmetric
potential. While the massless limit is relevant for pristine graphene, keeping
finite mass allows for generalizations onto situations with broken symmetry
between the two sublattices, and provides a link to the scattering theory of
electrons in a parabolic band. We demonstrate that the Dirac theory requires
short-distance regularization for potentials which are more singular than 1/r.
The formalism is then applied to scattering off a smooth short-ranged
potential. Next we consider the Coulomb potential scattering, where the Dirac
theory is consistent for a point scatterer only for the effective impurity
strength below 1/2. From the scattering phase shifts we obtain the exact
Coulomb transport cross-section in terms of the impurity strength. The results
are relevant for transport in graphene in the presence of impurities that do
not induce scattering between the Dirac points in the Brillouin zone.Comment: 17 pages, 4 figures. Published versio
Entropy, Contact Interaction with Horizon and Dark Energy
We present some arguments suggesting that the mismatch between Bekenstein-
Hawking entropy and the entropy of entanglement for vector fields is due to the
same gauge configurations which saturate the contact term in topological
susceptibility in QCD. In both cases the extra term with a "wrong sign" is due
to distinct topological sectors in gauge theories. This extra term has
non-dispersive nature, can not be restored from conventional spectral function
through dispersion relations, and can not be associated with any physical
propagating degrees of freedom. We make few comments on some profound
consequences of our findings. In particular, we speculate that the source of
the observed dark energy may also be related to the same type of gauge
configurations which are responsible for the mismatch between black hole
entropy and the entropy of entanglement in the presence of causal horizon.Comment: final version to appear in Phys. Rev. D (2011
Critical nucleus charge in a superstrong magnetic field: effect of screening
A superstrong magnetic field stimulates the spontaneous production of
positrons by naked nuclei by diminishing the value of the critical charge
Z_{cr} . The phenomenon of screening of the Coulomb potential by a superstrong
magnetic field which has been discovered recently acts in the opposite
direction and prevents the nuclei with Z52
for a nucleus to become critical stronger B are needed than without taking
screening into account.Comment: 13 pages, 2 figures, version to be published in Physical Review
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