4,028 research outputs found
Low-lying excitations and thermodynamics of an antiferromagnetic Heisenberg fractal system of a dimension between one and two
We investigate a frustrated Heisenberg spin-1/2 antiferromagnet on a fractal
lattice of dimension d=ln3/ln2 (Sierpinski gasket). Calculations were performed
using (a) exact diagonalization of all eigenstates and eigenvectors for systems
up to N=15 and (b) the Decoupled-Cell Quantum-Monte-Carlo method for systems up
to N=366. We present the low-lying spectrum and the specific heat. The specific
heat shows a second maximum in the low-temperature region. This behavior is
similar to the behavior of the quantum Heisenberg antiferromagnet on a kagome
lattice and suggests a disordered ground state and a spin gap in the considered
system.Comment: 2 pages, LaTeX, 3 eps figures, to appear in JMM
Quasi-periodic Variations in the Hard X-ray emission of a Large Arcade Flare
Quasi-periodic oscillations of the hard X-ray (HXR) emission of the large
flare of 2 November 1991 have been investigated using HXR light curves and soft
X-ray and HXR images recorded by the {\sl Yohkoh} X-ray telescopes. The results
of the analysis of these observations are the following: i) The observations
confirm that electrons are accelerated in oscillating magnetic traps which are
contained within the cusp magnetic structure. ii) The amplitude of the HXR
pulses increase due to the increase in the amplitude of the magnetic trap
oscillations and the increase in the density within the traps caused by the
chromospheric evaporation upflow. iii) The increase in the amplitude of the HXR
pulses terminates when further increase in the density inside the traps
inhibits the acceleration of electrons. iv) The model of oscillating magnetic
traps is able to explain time variation of the electron precipitation, strong
asymmetry in precipitation of accelerated electrons, and systematic differences
in the precipitation of 15 and 25 keV electrons. v) We have obtained a direct
observational evidence that strong HXR pulses are the result of the inflow of
dense plasma coming from the chromospheric evaporation, into the acceleration
volume.Comment: 18 pages, 12 figures, accepted by Solar Physic
Flare Hybrids
Svestka (Solar Phys. 1989, 121, 399) on the basis of the Solar Maximum
Mission observations introduced a new class of flares, the so-called flare
hybrids. When they start, they look as typical compact flares (phase 1), but
later on they look like flares with arcades of magnetic loops (phase 2). We
summarize the features of flare hybrids in soft and hard X-rays as well as in
extreme-ultraviolet; these allow us to distinguish them from other flares.
Additional energy release or long plasma cooling timescales have been suggested
as possible cause of phase 2. Estimations of frequency of flare hybrids have
been given. Magnetic configurations supporting their origin have been
presented. In our opinion, flare hybrids are quite frequent and a difference
between lengths of two interacting systems of magnetic loops is a crucial
parameter for recognizing their features.Comment: 15 pages, 4 figures, to appear in Solar Physic
On the existence conditions of surface spin wave modes in (Ga,Mn)As thin films
Spin-wave resonance (SWR) is a newly emerged method for studying surface
magnetic anisotropy and surface spin-wave modes (SSWMs) in (Ga,Mn)As thin
films. The existence of SSWMs in (Ga,Mn)As thin films has recently been
reported in the literature; SSWMs have been observed in the in-plane
configuration (with variable azimuth angle between the in-plane
magnetization of the film and the surface [100] crystal axis), in the azimuth
angle range between two in-plane critical angles and .
We show here that cubic surface anisotropy is an essential factor determining
the existence conditions of the above-mentioned SSWMs: conditions favorable for
the occurrence of surface spin-wave modes in a (Ga,Mn)As thin film in the
in-plane configuration are fulfilled for those azimuth orientations of the
magnetization of the sample that lie around the hard axes of cubic magnetic
anisotropy. This implies that a hard cubic anisotropy axis can be regarded in
(Ga,Mn)As thin films as an easy axis for surface spin pinning
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