94 research outputs found
Quasi-long range order in the random anisotropy Heisenberg model
The large distance behaviors of the random field and random anisotropy
Heisenberg models are studied with the functional renormalization group in
dimensions. The random anisotropy model is found to have a phase
with the infinite correlation radius at low temperatures and weak disorder. The
correlation function of the magnetization obeys a power law . The
magnetic susceptibility diverges at low fields as . In the random field model the correlation radius is found
to be finite at the arbitrarily weak disorder.Comment: 4 pages, REVTe
Haldane Gapped Spin Chains: Exact Low Temperature Expansions of Correlation Functions
We study both the static and dynamic properties of gapped, one-dimensional,
Heisenberg, anti-ferromagnetic, spin chains at finite temperature through an
analysis of the O(3) non-linear sigma model. Exploiting the integrability of
this theory, we are able to compute an exact low temperature expansion of the
finite temperature correlators. We do so using a truncated `form-factor'
expansion and so provide evidence that this technique can be successfully
extended to finite temperature. As a direct test, we compute the static
zero-field susceptibility and obtain an exact match to the susceptibility
derived from the low temperature expansion of the exact free energy. We also
study transport properties, computing both the spin conductance and the
NMR-relaxation rate, 1/T_1. We find these quantities to show ballistic
behaviour. In particular, the computed spin conductance exhibits a non-zero
Drude weight at finite temperature and zero applied field. The physics thus
described differs from the spin diffusion reported by Takigawa et al. from
experiments on the Haldane gap material, AgVP_2S_6.Comment: 51 pages, 5 figure
Nonthermal Emission from Star-Forming Galaxies
The detections of high-energy gamma-ray emission from the nearby starburst
galaxies M82 & NGC253, and other local group galaxies, broaden our knowledge of
star-driven nonthermal processes and phenomena in non-AGN star-forming
galaxies. We review basic aspects of the related processes and their modeling
in starburst galaxies. Since these processes involve both energetic electrons
and protons accelerated by SN shocks, their respective radiative yields can be
used to explore the SN-particle-radiation connection. Specifically, the
relation between SN activity, energetic particles, and their radiative yields,
is assessed through respective measures of the particle energy density in
several star-forming galaxies. The deduced energy densities range from O(0.1)
eV/cm^3 in very quiet environments to O(100) eV/cm^3 in regions with very high
star-formation rates.Comment: 17 pages, 5 figures, to be published in Astrophysics and Space
Science Proceeding
Detection of diffuse TeV gamma-ray emission from the nearby starburst galaxy NGC 253
We report the TeV gamma-ray observations of the nearby normal spiral galaxy
NGC 253. At a distance of 2.5 Mpc, NGC 253 is one of the nearest
starburst galaxies. This relative closeness, coupled with the high star
formation rate in the galaxy, make it a good candidate TeV gamma-ray source.
Observations were carried out in 2000 and 2001 with the CANGAROO-II 10 m
imaging atmospheric Cerenkov telescope. TeV gamma-ray emission is detected at
the level with a flux of at energies 0.5 TeV. The data indicate that the
emission region is broader than the point spread function of our telescope.Comment: 4 pages, double colomn, 3 figures, aa.cl
Starburst Galaxies and the X-Ray Background
Integrated X-ray spectra of an evolving population of starburst galaxies
(SBGs) are determined based on the observed spectra of local SBGs. In addition
to emission from hot gas and binary systems, our model SBG spectrum includes a
nonthermal component from Compton scattering of relativistic electrons by the
intense ambient far-IR and the (steeply evolving) CMB radiation fields. We use
these integrated spectra to calculate the levels of contribution of SBGs to the
cosmic X-ray background assuming that their density evolves as (1+z)^q up to a
maximal redshift of 5. We find that at energies <10 keV this contribution is at
a level of few percent for q up to 3, and in the range of 5%-15% for q ~ 4.5.
The Compton component is predicted to be the main SBG emission at high
energies, and its relative contribution gets progressively higher for
increasing redshift.Comment: 10 pages, 5 figures; accepted for publication in A&
Evidence of TeV gamma-ray emission from the nearby starburst galaxy NGC 253
TeV gamma-rays were recently detected from the nearby normal spiral galaxy
NGC 253 (Itoh et al., 2002). Observations to detect the Cherenkov light images
initiated by gamma-rays from the direction of NGC 253 were carried out in 2000
and 2001 over a total period of 150 hours. The orientation of images in
gamma-ray--like events is not consistent with emission from a point source, and
the emission region corresponds to a size greater than 10 kpc in radius. Here,
detailed descriptions of the analysis procedures and techniques are given.Comment: 16 pages, 27 figures, aa.cl
Quasi-long-range order in the random anisotropy Heisenberg model: functional renormalization group in 4-\epsilon dimensions
The large distance behaviors of the random field and random anisotropy O(N)
models are studied with the functional renormalization group in 4-\epsilon
dimensions. The random anisotropy Heisenberg (N=3) model is found to have a
phase with the infinite correlation radius at low temperatures and weak
disorder. The correlation function of the magnetization obeys a power law <
m(x) m(y) >\sim |x-y|^{-0.62\epsilon}. The magnetic susceptibility diverges at
low fields as \chi \sim H^{-1+0.15\epsilon}. In the random field O(N) model the
correlation radius is found to be finite at the arbitrarily weak disorder for
any N>3. The random field case is studied with a new simple method, based on a
rigorous inequality. This approach allows one to avoid the integration of the
functional renormalization group equations.Comment: 12 pages, RevTeX; a minor change in the list of reference
Weak reaction freeze-out constraints on primordial magnetic fields
We explore constraints on the strength of the primordial magnetic field based
upon the weak reaction freeze-out in the early universe. We find that limits on
the strength of the magnetic field found in other works are recovered simply by
examining the temperature at which the rate of weak reactions drops below the
rate of universal expansion ( H). The temperature for which the
ratio at freeze-out leads to acceptable helium production implies limits
on the magnetic field. This simplifies the application of magnetic fields to
other cosmological variants of the standard big-bang. As an illustration we
also consider effects of neutrino degeneracy on the allowed limits to the
primordial magnetic field.Comment: Submitted to Phys. Rev. D., 6 pages, 2 figure
RXTE View of the Starburst Galaxies M82 and NGC 253
The two nearby starburst galaxies M82 and NGC 253 were observed for 100 ksec
over a 10-month period in 1997. An increase of the M82 flux by a factor ~2 was
measured during the period July-November, when compared with the flux measured
earlier in 1997. The flux measured in the field centered on M82 includes ~38 of
the emission from the Seyfert 1 galaxy M81. The best-fitting model for the
earlier emission from M82 is thermal with kT = 6.7 +/- 0.1 keV. In the high
flux state, the emission additionally includes either an absorbed second
thermal component or absorbed power-law component, with the former providing a
much better fit. A likely origin for the temporal variability is a single
source in M82. The flux of NGC 253, which did not vary significantly during the
period of observations, can be well fit by either a thermal spectrum with kT ~
3.8 +/- 0.3 keV, or by a power law with photon index of 2.7 +/- 0.10. We have
also attempted fitting the measurements to more realistic composite models with
thermal and power-law components, such as would be expected from a dominant
contribution from binary systems, or Compton scattering of (far) IR radiation
by radio emitting electrons. However, the addition of any amount of a power-law
component, even with cutoff at 20 keV, only increases chi-square. The 90%
confidence upper limit for power law emission with (photon) index 1.5 is only
2.4% of the 2 -- 10 keV flux of M82; the corresponding limit for NGC 253, with
index 2.0, is 48%.Comment: 18 pages, 4 figures, accepted for publication in A&
Nonthermal radiation mechanisms
In this paper we review the possible radiation mechanisms for the observed
non-thermal emission in clusters of galaxies, with a primary focus on the radio
and hard X-ray emission. We show that the difficulty with the non-thermal,
non-relativistic Bremsstrahlung model for the hard X-ray emission, first
pointed out by Petrosian (2001) using a cold target approximation, is somewhat
alleviated when one treats the problem more exactly by including the fact that
the background plasma particle energies are on average a factor of 10 below the
energy of the non-thermal particles. This increases the lifetime of the
non-thermal particles, and as a result decreases the extreme energy
requirement, but at most by a factor of three. We then review the synchrotron
and so-called inverse Compton emission by relativistic electrons, which when
compared with observations can constrain the value of the magnetic field and
energy of relativistic electrons. This model requires a low value of the
magnetic field which is far from the equipartition value. We briefly review the
possibilities of gamma-ray emission and prospects for GLAST observations. We
also present a toy model of the non-thermal electron spectra that are produced
by the acceleration mechanisms discussed in an accompanying paper.Comment: 17 pages, 6 figures, accepted for publication in Space Science
Reviews, special issue "Clusters of galaxies: beyond the thermal view",
Editor J.S. Kaastra, Chapter 10; work done by an international team at the
International Space Science Institute (ISSI), Bern, organised by J.S.
Kaastra, A.M. Bykov, S. Schindler & J.A.M. Bleeke
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