1,505 research outputs found
The spin angular gradient approximation in the density functional theory
A spin angular gradient approximation for the exchange correlation magnetic
field in the density functional formalism is proposed. The usage of such
corrections leads to a consistent spin dynamical approach beyond the local
approximation. The proposed technique does not contain any approximations for
the form of potential and can be used in modern full potential band structure
methods. The obtained results indicate that the direct 'potential' exchange in
3d magnets is rather small compared to the indirect 'kinetic' exchange, thus
justifies the dynamical aspect of the local density approximation in 3d metals
Electronic Structure and Magnetic Properties of Solids
We review basic computational techniques for simulations of various magnetic
properties of solids. Several applications to compute magnetic anisotropy
energy, spin wave spectra, magnetic susceptibilities and temperature dependent
magnetisations for a number of real systems are presented for illustrative
purposes.Comment: Review article; To appear in Journal of Computational Crystallograph
Electron energy spectrum and magnetic interactions in high-T(sub c) superconductors
The character of magnetic interactions in La-Sr-Cu-O and Y-Ba-Cu-O systems is of primary importance for analysis of high-T(sub c) superconductivity in these compounds. Neutron diffraction experiments showed the antiferromagnetic ground state for nonsuperconducting La2CuO4 and YBa2Cu3O6 with the strongest antiferromagnetic superexchange being in the ab plane. The nonsuperconducting '1-2-3' system has two Neel temperatures T sub N1 and T sub N2. The first one corresponds to the ordering of Cu atoms in the CuO2 planes; T sub N2 reflects the antiferromagnetic ordering of magnetic moments in CuO chains relatively to the moments in the planes T sub N1 and T sub N2 depend strongly on the oxygen content. Researchers describe magnetic interactions in high-T superconductors based on the Linear Muffin-Tin Orbitals (LMTO) band structure calculations. Exchange interaction parameters can be defined from the effective Heisenberg hamiltonian. When the magnetic moments are not too large, as copper magnetic moments in superconducting oxides, J sub ij parameters can be defined through the non-local magnetic susceptibility of spin restricted solution for the crystal. The results of nonlocal magnetic susceptibility calculations and the values of exchange interaction parameters for La CuO and YBa2Cu3O7 systems are given in tabular form. Strong anisotropy of exchange interactions in the ab plane and along the c axis in La2CuO4 is obviously seen. The value of Neel temperature found agrees well with the experimental data available. In the planes of '1-2-3' system there are quite strong antiferromagnetic Cu-O and O-O interaction which appear due to holes in oxygen subbands. These results are in line with the magnetic model of oxygen holes pairing in high-T(sub c) superconductors
Cycle of the needs satisfaction, and information support of the society development simulation system
The report focuses on some of the key points of constructing a model of an artificial society. It is based on the processes of emergence and implementation of the needs of specific agents, depending on the internal processes in the agents, and external environmental factors. Unlike in other approaches, the basis of the modeled system agents' behavior is the concept of needs as the necessity of implementation of the agents' transition from one state to another. This article presents an algorithm of the needs satisfaction of the agent, starting with the event that caused the need for, and ending its satisfaction, or the message that it is impossible to satisfy. The basis of objective knowledge in the system are a model of active and passive agents, as well as recipes meet the needs of the active agents and the relationships between them. Β© 2017 Author(s)
Spin wave dispersion based on the quasiparticle self-consistent method: NiO, MnO and -MnAs
We present spin wave dispersions in MnO, NiO, and -MnAs based on the
quasiparticle self-consistent method (\qsgw), which determines an optimum
quasiparticle picture. For MnO and NiO, \qsgw results are in rather good
agreement with experiments, in contrast to the LDA and LDA+U description. For
-MnAs, we find a collinear ferromagnetic ground state in \qsgw, while
this phase is unstable in the LDA.Comment: V2: add another figure for SW life time. Formalism is detaile
Spin-density fluctuations and the fluctuation-dissipation theorem in 3d ferromagnetic metals
Spatial and time scales of spin density fluctuations (SDF) were analyzed in
3d ferromagnets using ab initio linear response calculations of complete
wavevector and energy dependence of the dynamic spin susceptibility tensor. We
demonstrate that SDF are spread continuously over the entire Brillouin zone and
while majority of them reside within the 3d bandwidth, a significant amount
comes from much higher energies. A validity of the adiabatic approximation in
spin dynamics is discussed. The SDF spectrum is shown to have two main
constituents: a minor low-energy spin wave contribution and a much larger
high-energy component from more localized excitations. Using the
fluctuation-dissipation theorem (FDT), the on-site spin correlator (SC) and the
related effective fluctuating moment were properly evaluated and their
universal dependence on the 3d band population is further discussed
Land management cluster zonningβs methods summary
The article focuses on methods of land management cluster zoning analysis. The authors have analyzed a lot of articles and books about zoning and concluded that there was insufficient attention to zoning methods. The article goal is to study different methods of cluster zoning (clustering of the municipal districts of a Russian region) for purposes of land management information support. The authors have defined the concept of βland management cluster zoningβ, have analyzed the tree model method, the integrated zoning method and zoning based on the criterion of the efficiency of land management. These methods allow for cluster zoning of municipal districts. These methods have been tested using data from Novgorod Region. Based on the results of the study the authors have concluded that various zoning methods have yielded results close to 80%, but the choice of method should take into account the zoning purposes. For example, the tree model method is the most suitable one in the case of zoning based on indicators that have identical impact on land management. The method of integrated zoning is the most appropriate for application in the case of indications having different impact on land management. Zoning based on the criterion of land management efficiency separates municipal districts by one indicator. But this indicator is the key one.Π‘ΡΠ°ΡΡΡ ΠΏΠΎΡΠ²ΡΡΠ΅Π½Π° Π²ΠΎΠΏΡΠΎΡΠ°ΠΌ Π°Π½Π°Π»ΠΈΠ·Π° ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΠΊΠ»Π°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠ΅ΡΡΠΈΡΠΎΡΠΈΡ ΡΠ΅Π³ΠΈΠΎΠ½Π° Π΄Π»Ρ ΡΠ΅Π»Π΅ΠΉ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ Π·Π΅ΠΌΠ΅Π»ΡΠ½ΡΠΌΠΈ ΡΠ΅ΡΡΡΡΠ°ΠΌΠΈ. ΠΠ²ΡΠΎΡΡ ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π»ΠΈ ΠΈΠΌΠ΅ΡΡΠΈΠΉΡΡ ΠΌΠ°ΡΡΠΈΠ² Π»ΠΈΡΠ΅ΡΠ°ΡΡΡΠ½ΡΡ
ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠΎΠ² ΠΏΠΎ ΡΠ΅ΠΌΠ΅ ΠΈ ΡΠ΄Π΅Π»Π°Π»ΠΈ Π²ΡΠ²ΠΎΠ΄ ΠΎ Π½Π΅Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠΌ Π²Π½ΠΈΠΌΠ°Π½ΠΈΠΈ, ΠΊΠΎΡΠΎΡΠΎΠ΅ ΡΠ΄Π΅Π»ΡΠ΅ΡΡΡ Π½Π΅ΠΏΠΎΡΡΠ΅Π΄ΡΡΠ²Π΅Π½Π½ΠΎ ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ. Π¦Π΅Π»ΡΡ ΡΡΠ°ΡΡΠΈ ΡΠ²Π»ΡΠ΅ΡΡΡ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΊΠ»Π°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠ΅Π³ΠΈΠΎΠ½Π° (ΠΊΠ»Π°ΡΡΠ΅ΡΠΈΠ·Π°ΡΠΈΠΈ Π°Π΄ΠΌΠΈΠ½ΠΈΡΡΡΠ°ΡΠΈΠ²Π½ΡΡ
ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠΉ, Π²Ρ
ΠΎΠ΄ΡΡΠΈΡ
Π² ΡΡΠ±ΡΠ΅ΠΊΡ Π€Π΅Π΄Π΅ΡΠ°ΡΠΈΠΈ) Π΄Π»Ρ ΡΠ΅Π»Π΅ΠΉ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠ΅Π½ΠΈΡ ΠΏΡΠΎΡΠ΅ΡΡΠ° ΡΡΡΠ°ΡΠ΅Π³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ Π·Π΅ΠΌΠ΅Π»ΡΠ½ΡΠΌΠΈ ΠΈ ΠΏΡΠΈΡΠΎΠ΄Π½ΡΠΌΠΈ ΡΠ΅ΡΡΡΡΠ°ΠΌΠΈ ΡΠ΅Π³ΠΈΠΎΠ½Π°. ΠΠ»Ρ Π΄ΠΎΡΡΠΈΠΆΠ΅Π½ΠΈΡ ΡΠΊΠ°Π·Π°Π½Π½ΠΎΠΉ ΡΠ΅Π»ΠΈ Π±ΡΠ»ΠΎ Π΄Π°Π½ΠΎ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΊΠ»Π°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π΄Π»Ρ ΡΠ΅Π»Π΅ΠΉ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ Π·Π΅ΠΌΠ΅Π»ΡΠ½ΡΠΌΠΈ ΡΠ΅ΡΡΡΡΠ°ΠΌΠΈ, ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Ρ ΠΌΠ΅ΡΠΎΠ΄Ρ Π΄ΡΠ΅Π²ΠΎΠ²ΠΈΠ΄Π½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ, Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΈΠ½ΡΠ΅Π³ΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Ρ ΠΈ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡΠΈΠ΅ ΡΠ°Π·Π΄Π΅Π»ΠΈΡΡ ΠΏΡΠΎΠ²Π΅ΡΡΠΈ ΠΊΠ»Π°ΡΡΠ΅ΡΠ½ΠΎΠ΅ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΌΡΠ½ΠΈΡΠΈΠΏΠ°Π»ΡΠ½ΡΡ
ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠΉ ΡΠ΅Π³ΠΈΠΎΠ½Π°. Π‘ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠΊΠ°Π·Π°Π½Π½ΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΎ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΡΠ΅ΡΡΠΈΡΠΎΡΠΈΠΈ ΠΠΎΠ²Π³ΠΎΡΠΎΠ΄ΡΠΊΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ. ΠΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ°ΠΌ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΡΠ΄Π΅Π»Π°Π½Ρ Π²ΡΠ²ΠΎΠ΄Ρ, ΡΡΠΎ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ ΠΌΠ΅ΡΠΎΠ΄Ρ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π² 80 % Π΄Π°Π»ΠΈ ΡΡ
ΠΎΠΆΠΈΠ΅ ΠΌΠ΅ΠΆΠ΄Ρ ΡΠΎΠ±ΠΎΠΉ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ, Π½ΠΎ ΡΠ°Π·Π»ΠΈΡΠΈΡ Π² ΠΎΡΠ½ΠΎΠ²Π΅ ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΠΈΠ· ΡΡΠ΅Ρ
ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΠΌΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡ Π²ΡΡΠ°Π±ΠΎΡΠ°ΡΡ ΡΠ΅ΠΊΠΎΠΌΠ΅Π½Π΄Π°ΡΠΈΠΈ ΠΏΠΎ ΠΈΡ
ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ, ΠΈΡΡ
ΠΎΠ΄Ρ ΠΈΠ· ΡΠ΅Π»Π΅ΠΉ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ. ΠΠ°ΠΏΡΠΈΠΌΠ΅Ρ, ΠΌΠ΅ΡΠΎΠ΄ Π΄ΡΠ΅Π²ΠΎΠ²ΠΈΠ΄Π½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΠ΅Π»Π΅ΡΠΎΠΎΠ±ΡΠ°Π·Π½ΠΎ ΠΏΡΠΈΠΌΠ΅Π½ΡΡΡ ΠΏΡΠΈ Π½Π°Π»ΠΈΡΠΈΠΈ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ° ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ, ΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡΠΈΡ
ΠΎΠ΄ΠΈΠ½Π°ΠΊΠΎΠ²ΠΎΠ΅ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΠ΅ Π·Π΅ΠΌΠ΅Π»ΡΠ½ΡΠΌΠΈ ΡΠ΅ΡΡΡΡΠ°ΠΌΠΈ. ΠΠ΅ΡΠΎΠ΄ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠ³ΠΎ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΡΠ°Π·ΡΠΌΠ½Π΅Π΅ Π²ΡΠ΅Π³ΠΎ ΠΏΡΠΈΠΌΠ΅Π½ΡΡΡ Π² ΡΠ»ΡΡΠ°ΡΡ
, ΠΊΠΎΠ³Π΄Π° Π·Π½Π°ΡΠΈΠΌΠΎΡΡΡ ΡΠ°ΠΊΡΠΎΡΠΎΠ², Π²Π»ΠΈΡΡΡΠΈΡ
Π½Π° ΡΠΈΡΡΠ΅ΠΌΡ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ Π·Π΅ΠΌΠ΅Π»ΡΠ½ΡΠΌΠΈ ΡΠ΅ΡΡΡΡΠ°ΠΌΠΈ, ΡΠΈΠ»ΡΠ½ΠΎ ΡΠ°Π·Π»ΠΈΡΠ°Π΅ΡΡΡ. ΠΠ΅ΡΠΎΠ΄ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎ ΠΊΡΠΈΡΠ΅ΡΠΈΡ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ ΡΠ°Π·Π΄Π΅Π»ΡΠ΅Ρ ΠΌΡΠ½ΠΈΡΠΈΠΏΠ°Π»ΡΠ½ΡΠ΅ ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎ ΠΎΠ΄Π½ΠΎΠΌΡ, Π½ΠΎ ΠΊΠ»ΡΡΠ΅Π²ΠΎΠΌΡ Π΄Π»Ρ ΡΠΈΡΡΠ΅ΠΌΡ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ Π·Π΅ΠΌΠ΅Π»ΡΠ½ΡΠΌΠΈ ΡΠ΅ΡΡΡΡΠ°ΠΌΠΈ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Ρ. Π¨ΠΈΡΠΎΠΊΠΈΠ΅ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ ΠΎΡΠΊΡΡΠ²Π°ΡΡΡΡ Π΄Π»Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΎΠ² ΠΊΠ»Π°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ Π² ΡΠΈΡΡΠ΅ΠΌΠ΅ ΡΡΡΠ°ΡΠ΅Π³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΏΠ»Π°Π½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ Π·Π΅ΠΌΠ΅Π»ΡΠ½ΡΡ
ΡΠ΅ΡΡΡΡΠΎΠ² Π½Π° ΡΠ΅Π³ΠΈΠΎΠ½Π°Π»ΡΠ½ΡΡ
ΠΈ ΠΌΡΠ½ΠΈΡΠΈΠΏΠ°Π»ΡΠ½ΡΡ
ΡΡΠΎΠ²Π½ΡΡ
, Ρ. ΠΊ. Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΠΏΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΊΠ»Π°ΡΡΠ΅ΡΠ½ΠΎΠ³ΠΎ Π·ΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΎΠ±ΡΠ°Π·ΡΡΡΡΡ Π³ΡΡΠΏΠΏΡ ΠΌΡΠ½ΠΈΡΠΈΠΏΠ°Π»ΡΠ½ΡΡ
ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΠΉ, ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΡΡ
ΠΏΠΎ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΠΌ, Π²Π»ΠΈΡΡΡΠΈΠΌ Π½Π° ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ Π·Π΅ΠΌΠ΅Π»ΡΠ½ΡΡ
ΡΠ΅ΡΡΡΡΠΎΠ², ΠΈΠ»ΠΈ ΠΎΠ΄Π½ΠΎΡΠΎΠ΄Π½ΡΡ
ΠΏΠΎ ΠΊΠ°ΡΠ΅ΡΡΠ²Ρ ΡΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ ΠΈΠΌΠΈ
Magnetic susceptibility, exchange interactions and spin-wave spectra in the local spin density approximation
Starting from exact expression for the dynamical spin susceptibility in the
time-dependent density functional theory a controversial issue about exchange
interaction parameters and spin-wave excitation spectra of itinerant electron
ferromagnets is reconsidered. It is shown that the original expressions for
exchange integrals based on the magnetic force theorem (J. Phys. F14 L125
(1984)) are optimal for the calculations of the magnon spectrum whereas static
response function is better described by the ``renormalized'' magnetic force
theorem by P. Bruno (Phys. Rev. Lett. 90, 087205 (2003)). This conclusion is
confirmed by the {\it ab initio} calculations for Fe and Ni.Comment: 12 pages, 2 figures, submitted to JPC
Spin-polarized scanning tunneling microscopy of half-metallic ferromagnets: Non-quasiparticle contributions
The role of the many-body (spin-polaronic) effects in the scanning tunneling
spectroscopy of half-metallic ferromagnets (HMF) is considered. It is shown
that the non-quasiparticle (NQP) states exist in the majority or minority spin
gap in the presence of arbitrary external potential and, in particular, at the
surfaces and interfaces. Energy dependence of the NQP density of states is
obtained in various models of HMF, an important role of the hybridization
nature of the energy gap being demonstrated. The corresponding temperature
dependence of spin polarization is calculated. It is shown that the NQP states
result in a sharp bias dependence of the tunneling conductance near zero bias.
Asymmetry of the NQP states with respect to the Fermi energy provides an
opportunity to separate phonon and magnon peaks in the inelastic spectroscopy
by STM.Comment: 13 pages, 6 figure
- β¦