29 research outputs found
Enhancement of magnetic anisotropy barrier in long range interacting spin systems
Magnetic materials are usually characterized by anisotropy energy barriers
which dictate the time scale of the magnetization decay and consequently the
magnetic stability of the sample. Here we present a unified description, which
includes coherent rotation and nucleation, for the magnetization decay in
generic anisotropic spin systems. In particular, we show that, in presence of
long range exchange interaction, the anisotropy energy barrier grows as the
volume of the particle for on site anisotropy, while it grows even faster than
the volume for exchange anisotropy, with an anisotropy energy barrier
proportional to , where is the particle volume, is the range of interaction and is the embedding dimension. These
results shows a relevant enhancement of the anisotropy energy barrier w.r.t.
the short range case, where the anisotropy energy barrier grows as the particle
cross sectional area for large particle size or large particle aspect ratio.Comment: 7 pages, 6 figures. Theory of Magnetic decay in nanosystem. Non
equilibrium statistical mechanics of many body system
Magnetic and thermodynamic properties of cobalt doped iron pyrite: Griffiths Phase in a magnetic semiconductor
Doping of the band insulator FeS with Co on the Fe site introduces a
small density of itinerant carriers and magnetic moments. The lattice constant,
AC and DC magnetic susceptibility, magnetization, and specific heat have been
measured over the range of Co concentration. The variation of
the AC susceptibility with hydrostatic pressure has also been measured in a
small number of our samples. All of these quantities show systematic variation
with including a paramagnetic to disordered ferromagnetic transition at
. A detailed analysis of the changes with temperature and
magnetic field reveal small power law dependencies at low temperatures for
samples near the critical concentration for magnetism, and just above the Curie
temperature at higher . In addition, the magnetic susceptibility and
specific heat are non-analytic around H=0 displaying an extraordinarily sharp
field dependence in this same temperature range. We interpret this behavior as
due to the formation of Griffiths phases that result from the quenched disorder
inherent in a doped semiconductor.Comment: 22 pages including 27 figure
Integral Relaxation Time of Single-Domain Ferromagnetic Particles
The integral relaxation time \tau_{int} of thermoactivating noninteracting
single-domain ferromagnetic particles is calculated analytically in the
geometry with a magnetic field H applied parallel to the easy axis. It is shown
that the drastic deviation of \tau_{int}^{-1} from the lowest eigenvalue of the
Fokker-Planck equation \Lambda_1 at low temperatures, starting from some
critical value of H, is the consequence of the depletion of the upper potential
well. In these conditions the integral relaxation time consists of two
competing contributions corresponding to the overbarrier and intrawell
relaxation processes.Comment: 8 pages, 3 figure