42 research outputs found
Magnetic field reversals and galactic dynamos
We argue that global magnetic field reversals similar to those observed in
the Milky Way occur quite frequently in mean-field galactic dynamo models that
have relatively strong, random, seed magnetic fields that are localized in
discrete regions. The number of reversals decreases to zero with reduction of
the seed strength, efficiency of the galactic dynamo and size of the spots of
the seed field. A systematic observational search for magnetic field reversals
in a representative sample of spiral galaxies promises to give valuable
information concerning seed magnetic fields and, in this way, to clarify the
initial stages of galactic magnetic field evolution
Biermann Mechanism in Primordial Supernova Remnant and Seed Magnetic Fields
We study generation of magnetic fields by the Biermann mechanism in the
pair-instability supernovae explosions of first stars. The Biermann mechanism
produces magnetic fields in the shocked region between the bubble and
interstellar medium (ISM), even if magnetic fields are absent initially. We
perform a series of two-dimensional magnetohydrodynamic simulations with the
Biermann term and estimate the amplitude and total energy of the produced
magnetic fields. We find that magnetic fields with amplitude
G are generated inside the bubble, though the amount of
magnetic fields generated depend on specific values of initial conditions. This
corresponds to magnetic fields of erg per each supernova
remnant, which is strong enough to be the seed magnetic field for galactic
and/or interstellar dynamo.Comment: 12 pages, 3 figure
Mean magnetic field generation in sheared rotators
A generalized mean magnetic field induction equation for differential
rotators is derived, including a compressibility, and the anisotropy induced on
the turbulent quantities from the mean magnetic field itself and a mean
velocity shear. Derivations of the mean field equations often do not emphasize
that there must be anisotropy and inhomogeneity in the turbulence for mean
field growth. The anisotropy from shear is the source of a term involving the
product of the mean velocity gradient and the cross-helicity correlation of the
isotropic parts of the fluctuating velocity and magnetic field,
\lb{\bfv}\cdot{\bfb}\rb^{(0)}. The full mean field equations are derived to
linear order in mean fields, but it is also shown that the cross-helicity term
survives to all orders in the velocity shear. This cross-helicity term can
obviate the need for a pre-existing seed mean magnetic field for mean field
growth: though a fluctuating seed field is necessary for a non-vanishing
cross-helicity, the term can produce linear (in time) mean field growth of the
toroidal field from zero mean field. After one vertical diffusion time, the
cross-helicity term becomes sub-dominant and dynamo exponential
amplification/sustenance of the mean field can subsequently ensue. The
cross-helicity term should produce odd symmetry in the mean magnetic field, in
contrast to the usually favored even modes of the dynamo amplification in
sheared discs. This may be important for the observed mean field geometries of
spiral galaxies. The strength of the mean seed field provided by the cross-
helicity depends linearly on the magnitude of the cross-helicity.Comment: 15 pages, LaTeX, matches version accepted to ApJ, minor revision
Biermann Mechanism in Primordial Supernova Remnant and Seed Fields
We have studied the generation of magnetic fields by the Biermann mechanism
in the pair-instability supernovae explosions of the first stars. The Biermann
mechanism produces magnetic fields in the shocked region between the bubble and
interstellar medium (ISM), even if magnetic fields are absent initially. We
have performed a series of two-dimensional magnetohydrodynamic simulations with
the Biermann term and estimate the amplitude and total energy of the produced
magnetic fields. We find that magnetic fields with amplitude
G are generated inside the bubble, though the amount of
magnetic fields generated depend on specific values of initial conditions. This
corresponds to magnetic fields of ergs per each supernova
remnant, which is strong enough to be the seed magnetic field for a galactic
and/or interstellar dynamo.Comment: 4pages, 2figures, to appear in the Proc. of the Int. Conference on
"The Origin and Evolution of Cosmic Magnetism", Bologna, 29 August - 2
September 2005, eds. R. Beck, G. Brunetti, L. Feretti and B. Gaensler
(Atronomische Nachrichten, Wiley, 2005
The effects of vertical outflows on disk dynamos
We consider the effect of vertical outflows on the mean-field dynamo in a
thin disk. These outflows could be due to winds or magnetic buoyancy. We
analyse both two-dimensional finite-difference numerical solutions of the
axisymmetric dynamo equations and a free-decay mode expansion using the
thin-disk approximation. Contrary to expectations, a vertical velocity can
enhance dynamo action, provided it is not too strong. In the nonlinear regime
this can lead to super-exponential growth of the magnetic field.Comment: 14 pages, final version after referee comments, accepted in A&
In Situ Origin of Large Scale Galactic Magnetic Fields Without Kinetic Helicity?
The origin and sustenance of large scale galactic magnetic fields has been a
long standing and controversial astrophysical problem. Here an alternative to
the ``standard'' \a-\Omega mean field dynamo and primordial theories is
pursued. The steady supply of supernovae induced turbulence exponentiates the
total field energy, providing a significant seed mean field that can be
linearly stretched by shear. The observed micro-Gauss fields would be produced
primarily within one vertical diffusion time since it is only during this time
that linear stretching can compete with diffusion. This approach does not
invoke exponential mean field dynamo growth from the helicity \a-effect but
does employ turbulent diffusion, which limits the number of large scale
reversals. The approach could be of interest if the helicity effect is
suppressed independently of the turbulent diffusion. This is an important but
presently unresolved issue.Comment: 15 pages TeX, accepted, ApJ
Galactic dynamos with captured magnetic flux and an accretion flow
We examine the behaviour of an axisymmetric galactic dynamo model with a
radial accretion flow in the disc. We also introduce a vertical magnetic flux
through the galactic midplane, to simulate the presence of a large scale
magnetic field trapped by the galaxy when forming. The trapped vertical flux is
conserved and advected towards the disc centre by the radial flow. We confirm
that accretion flows of magnitude several km/s through a significant part of
the galactic disc can markedly inhibit dynamo action. Moreover, advection of
the vertical flux in general results in mixed parity galactic fields. However,
the effect is nonlinear and non-additive -- global magnetic field energies are
usually significantly smaller that the sum of purely dynamo generated and
purely advected field energies. For large inflow speeds, a form of
`semi-dynamo' action may occur.
We apply our results to the accumulation and redistribution, by a radial
inflow, of a vertical magnetic flux captured by the Galactic disc. Taking
representative values, it appears difficult to obtain mean vertical fields near
the centre of the Milky Way that are much in excess of 10 microgauss, largely
because the galactic dynamo and turbulent magnetic diffusion modify the
external magnetic field before it can reach the disc centre.Comment: 18 pages, 12 figures, LaTE
Modeling the total and polarized emission in evolving galaxies: "spotty" magnetic structures
Future radio observations with the SKA and its precursors will be sensitive
to trace spiral galaxies and their magnetic field configurations up to redshift
. We suggest an evolutionary model for the magnetic configuration in
star-forming disk galaxies and simulate the magnetic field distribution, the
total and polarized synchrotron emission, and the Faraday rotation measures for
disk galaxies at z\la 3. Since details of dynamo action in young galaxies are
quite uncertain, we model the dynamo action heuristically relying only on
well-established ideas of the form and evolution of magnetic fields produced by
the mean-field dynamo in a thin disk. We assume a small-scale seed field which
is then amplified by the small-scale turbulent dynamo up to energy
equipartition with kinetic energy of turbulence. The large-scale galactic
dynamo starts from seed fields of 100 pc and an averaged regular field strength
of 0.02\,G, which then evolves to a "spotty" magnetic field configuration
in about 0.8\,Gyr with scales of about one kpc and an averaged regular field
strength of 0.6\,G. The evolution of these magnetic spots is simulated
under the influence of star formation, dynamo action, stretching by
differential rotation of the disk, and turbulent diffusion. The evolution of
the regular magnetic field in a disk of a spiral galaxy, as well as the
expected total intensity, linear polarization and Faraday rotation are
simulated in the rest frame of a galaxy at 5\,GHz and 150\,MHz and in the rest
frame of the observer at 150\,MHz. We present the corresponding maps for
several epochs after disk formation. (abridged)Comment: 13 pages, 6 figures, 2 tables, revised version is accepted for
publication in Astronomische Nachrichte
Pulsar rotation measures and the magnetic structure of our Galaxy
We have obtained 63 rotation measures (RMs) from polarization observations of
southern pulsars, of which 54 are new measurements and 3 are varied from
previous values. The new pulsar RM data at high Galactic latitudes are mostly
consistent with the antisymmetric RM distribution found previously. For the
Galactic disc, evidence for a field reversal near the Perseus arm, and possibly
another beyond it, is presented. Inside the Solar Circle, in addition to the
two known field reversals in or near the Carina-Sagittartus arm and the
Crux-Scutum arm, a further reversal in the Norma arm is tentatively identified.
These reversals, together with the pitch angle derived from pulsar RM and
stellar polarization distributions, are consistent with bisymmetric spiral
(BSS) models for the large-scale magnetic field structure in the disc of our
Galaxy. However, discrimination between models is complicated by the presence
of smaller-scale irregularities in the magnetic field, as well as uncertainties
in the theoretical modelling.Comment: 10pages; 8 figures; Accepted by MNRA