295 research outputs found
Ab Initio Exchange Interactions and Magnetic Properties of Intermetallic Compound Gd(2)Fe(17-x)Ga(x)
Intermetallic compounds R2Fe17 are perspective for applications as permanent
magnets. Technologically these systems must have Curie temperature Tc much
higher than room temperature and preferably have easy axis anisotropy. At the
moment highest Tc among stoichiometric R2Fe17 materials is 476 K, which is not
high enough. There are two possibilities to increase Tc: substitution of Fe
ions with non-magnetic elements or introduction of light elements into
interstitial positions. In this work we have focused our attention on
substitution scenario of Curie temperature rising observed experimentally in
Gd(2)Fe(17-x)Ga(x) (x=0,3,6) compounds. In the framework of the LSDA approach
electronic structure and magnetic properties of the compounds were calculated.
Ab initio exchange interaction parameters within the Fe sublattice for all
nearest Fe ions were obtained. Employing the theoretical values of exchange
parameters Curie temperatures Tc of Gd(2)Fe(17-x)Ga(x) within mean-field theory
were estimated. Obtained values of Tc agree well with experiment. Also LSDA
computed values of total magnetic moment coincide with experimental ones.Comment: 4 pages, 4 figures, 4 tables, Proceedings for EASTMAG-2010, June 28 -
July 2 2010, Ekaterinburg, Russi
Magnetization and magnetic entropy change of a three-dimensional isotropic ferromagnet near the Curie temperature in the random phase approximation
The behavior of a three-dimensional isotropic Heisenberg ferromagnet in the presence of a magnetic field H is investigated in the random phase approximation (RPA) near the Curie temperature Tc. It is shown that the magnetization M at the Curie temperature Tc is described by the law M(T=Tc)∼H1/5 and the initial magnetic susceptibility χ0 at temperatures T≥Tc is given by χ0(T≥Tc)∼(T-Tc)-2. It means that in the RPA the critical exponents for a three-dimensional Heisenberg ferromagnet coincide with the critical exponents for the Berlin-Kac spherical model of a ferromagnet rather than with the critical exponents of the mean field approximation (MFA). Hence it follows as well that, when a magnetic field H is risen from H=0 to H=Ha, the magnetic entropy SM will be decreased as ΔSM(T=Tc)∼-Ha 4/5 at the Curie temperature Tc and as ΔS M(T>Tc)∼-(T-Tc)-3H a 2 at temperatures T>Tc. © 2013 Elsevier B.V
On the probability of down-crossing and up-crossing rogue waves
By means of the direct numerical simulation of directional waves on the
surface of deep water it is shown that extreme waves can exhibit such asymmetry
that the occurrence of deeper troughs is several times more likely on the wave
rear slopes. This effect becomes most pronounced in the case of steep
short-crested waves. It is not related to the Benjamin - Feir instability, but
is a result of complex contribution from nonlinear combination harmonics,
mainly cubic in nonlinearity. The discovered asymmetry can lead to remarkably
different estimates of the rogue wave probability based on either down- or
up-zero-crossing methods for individual wave selection, commonly used in the
oceanography
Theoretical investigation of TbNi_{5-x}Cu_x optical properties
In this paper we present theoretical investigation of optical conductivity
for intermetallic TbNi_{5-x}Cu_x series. In the frame of LSDA+U calculations
electronic structure for x=0,1,2 and on top of that optical conductivities were
calculated. Disorder effects of Ni for Cu substitution on a level of LSDA+U
densities of states (DOS) were taken into account via averaging over all
possible Cu ion positions for given doping level x. Gradual suppression and
loosing of structure of optical conductivity at 2 eV together with simultaneous
intensity growth at 4 eV correspond to increase of Cu and decrease of Ni
content. As reported before [Knyazev et al., Optics and Spectroscopy 104, 360
(2008)] plasma frequency has non monotonic doping behaviour with maximum at
x=1. This behaviour is explained as competition between lowering of total
density of states on the Fermi level N(E_F) and growing of number of carriers.
Our theoretical results agree well with variety of recent experiments.Comment: 4 pages, 3 figure
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