3,335 research outputs found

    Lattice Distortion and Magnetism of 3d-t2gt_{2g} Perovskite Oxides

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    Several puzzling aspects of interplay of the experimental lattice distortion and the the magnetic properties of four narrow t2gt_{2g}-band perovskite oxides (YTiO3_3, LaTiO3_3, YVO3_3, and LaVO3_3) are clarified using results of first-principles electronic structure calculations. First, we derive parameters of the effective Hubbard-type Hamiltonian for the isolated t2gt_{2g} bands using newly developed downfolding method for the kinetic-energy part and a hybrid approach, based on the combination of the random-phase approximation and the constraint local-density approximation, for the screened Coulomb interaction part. Then, we solve the obtained Hamiltonian using a number of techniques, including the mean-field Hartree-Fock (HF) approximation, the second-order perturbation theory for the correlation energy, and a variational superexchange theory. Even though the crystal-field splitting is not particularly large to quench the orbital degrees of freedom, the crystal distortion imposes a severe constraint on the form of the possible orbital states, which favor the formation of the experimentally observed magnetic structures in YTiO3_3, YVO_, and LaVO3_3 even at the HF level. Beyond the HF approximation, the correlations effects systematically improve the agreement with the experimental data. Using the same type of approximations we could not reproduce the correct magnetic ground state of LaTiO3_3. However, we expect that the situation may change by systematically improving the level of approximations for dealing with the correlation effects.Comment: 30 pages, 17 figures, 8 tables, high-quality figures are available via e-mai

    Realization of anisotropic compass model on the diamond lattice of Cu2+^{2+} in CuAl2_2O4_4

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    Spin-orbit (SO) Mott insulators are regarded as a new paradigm of magnetic materials, whose properties are largely influenced by SO coupling and featured by highly anisotropic bond-dependent exchange interactions between the spin-orbital entangled Kramers doublets, as typically manifested in 5d5d iridates. Here, we propose that a very similar situation can be realized in cuprates when the Cu2+^{2+} ions reside in a tetrahedral environment, like in spinel compounds. Using first-principles electronic structure calculations, we construct a realistic model for the diamond lattice of the Cu2+^{2+} ions in CuAl2_2O4_4 and show that the magnetic properties of this compound are largely controlled by anisotropic compass-type exchange interactions that dramatically modify the magnetic ground state by lifting the spiral spin-liquid degeneracy and stabilizing a commensurate single-q\boldsymbol{q} spiral

    Hybridization and spin-orbit coupling effects in quasi-one-dimensional spin-1/2 magnet Ba3Cu3Sc4O12

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    We study electronic and magnetic properties of the quasi-one-dimensional spin-1/2 magnet Ba3Cu3Sc4O12 with a distinct orthogonal connectivity of CuO4 plaquettes. An effective low-energy model taking into account spin-orbit coupling was constructed by means of first-principles calculations. On this basis a complete microscopic magnetic model of Ba3Cu3Sc4O12, including symmetric and antisymmetric anisotropic exchange interactions, is derived. The anisotropic exchanges are obtained from a distinct first-principles numerical scheme combining, on one hand, the local density approximation taking into account spin-orbit coupling, and, on the other hand, projection procedure along with the microscopic theory by Toru Moriya. The resulting tensors of the symmetric anisotropy favor collinear magnetic order along the structural chains with the leading ferromagnetic coupling J1 = -9.88 meV. The interchain interactions J8 = 0.21 meV and J5 = 0.093 meV are antiferromagnetic. Quantum Monte Carlo simulations demonstrated that the proposed model reproduces the experimental Neel temperature, magnetization and magnetic susceptibility data. The modeling of neutron diffraction data reveals an important role of the covalent Cu-O bonding in Ba3Cu3Sc4O12.Comment: 11 pages, 12 figure

    Low-Temperature Spin Dynamics of Doped Manganites: roles of Mn-t2g and eg and O-2p states

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    The low-temperature spin dynamics of doped manganites have been analyzed within a tight-binding model, the parameters of which are estimated by mapping the results of ab initio density functional calculations onto the model. This approach is found to provide a good description of the spin dynamics of the doped manganites, observed earlier within the ab initio calculations. Our analysis not only provides some insight into the roles of the eg and the t2g states but also indicates that the oxygen p states play an important role in the spin dynamics. This may cast doubt on the adaptability of the conventional model Hamiltonian approaches to the analysis of spin dynamics of doped manganites.Comment: 12 pages; Includes 5 figure

    Ferromagnetic zigzag chains and properties of the charge ordered perovskite manganites

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    The low-temperature properties of the so-called ''charge ordered'' state in 50% doped perovskite manganites are described from the viewpoint of the magnetic spin ordering. In these systems, the zigzag antiferromagnetic ordering, combined with the double-exchange physics, effectively divides the whole sample into the one-dimensional ferromagnetic zigzag chains and results in the anisotropy of electronic properties. The electronic structure of one such chain is described by an effective 3Γ—\times3 Hamiltonian in the basis of Mn(3deg3de_g) orbitals. We treat this problem analytically and consider the following properties: (i) the nearest-neighbor magnetic interactions; (ii) the distribution of the Mn(3deg3de_g) and Mn(4p4p) states near the Fermi level, and their contribution to the optical conductivity and the resonant x-ray scattering near the Mn KK-absorption edge. We argue that the anisotropy of magnetic interactions in the double-exchange limit, combined with the isotropic superexchange interactions, readily explains both the local and the global stability of the zigzag antiferromagnetic state. The two-fold degeneracy of ege_g levels plays a very important role in the problem and explains the insulating behavior of the zigzag chain, as well as the appearance of the orbital ordering in the double-exchange model. Importantly, however, the charge ordering itself is expected to play only a minor role and is incompatible with the ferromagnetic coupling within the chain. We also discuss possible effects of the Jahn-Teller distortion and compare the tight-binding picture with results of band structure calculations in the local-spin-density approximation.Comment: 35 pages, 8 figure

    Half-magnetization plateaux in Cr spinels

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    Magnetization plateaux, visible as anomalies in magnetic susceptibility at low temperatures, are one of the hallmarks of frustrated magnetism. An extremely robust half-magnetization plateau is observed in the spinel oxides CdCr2O4 and HgCr2O4, where it is accompanied by a substantial lattice distortion. We give an overview of the present state experiment for CdCr2O4 and HgCr2O4, and show how such a half-magnetization plateau arises quite naturally in a simple model of these systems, once coupling to the lattice is taken into account.Comment: 8 pages latex using IOP macros, from review talk given at RHMF 2006 (Sendai

    Origin of the giant magnetic moments of Fe impurities on and in Cs films

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    To explore the origin of the observed giant magnetic moments (∼7μB\sim 7 \mu_B) of Fe impurities on the surface and in the bulk of Cs films, we have performed the relativistic LSDA + U calculations using the linearized muffin-tin orbital (LMTO) band method. We have found that Fe impurities in Cs behave differently from those in noble metals or in Pd. Whereas the induced spin polarization of Cs atoms is negligible, the Fe ion itself is found to be the source of the giant magnetic moment. The 3d electrons of Fe in Cs are localized as the 4f electrons in rare-earth ions so that the orbital magnetic moment becomes as large as the spin magnetic moment. The calculated total magnetic moment of M=6.43μBM = 6.43 \mu_B, which comes mainly from Fe ion, is close to the experimentally observed value.Comment: 4 pages including 3 figures and 1 table. Submitted to PR

    НСобычный случай лСчСния ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π° с химичСским ΠΎΠΆΠΎΠ³ΠΎΠΌ ΠΏΠΈΡ‰Π΅Π²ΠΎΠ΄Π° ΠΈ ΠΏΠ΅Ρ€Ρ„ΠΎΡ€Π°Ρ†ΠΈΠ΅ΠΉ ΠΆΠ΅Π»ΡƒΠ΄ΠΊΠ°

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    Treatment of patients with chemical burns of the esophagus and stomach is a difficult task.Perforation of the stomach or the formation of strictures of the esophagus, stomach, duodenum, and even the initial parts of the jejunum can be the outcome of chemical burns.Patients with concomitant esophageal and gastric strictures are the most difficult to treat, which often requires multi-stage operations.This article describes a clinical case of surgical treatment of a patient with a combined chemical burn of the esophagus and stomach with hydrochloric acid. One week after hospitalization, the patient had gastric perforation. The patient was urgently operated in the course of peritonitis. The peculiarity of the operation was that the surgeons, having made a gastrectomy, removed the esophageal stump to the anterior abdominal wall in the epigastrium and applied an enterostomy. In such a state with significant alimentary depletion (body mass index β€” BMI 15) on 11.10.02 the patient was taken to a Moscow clinic. A year later, the main surgical reconstructive treatment was performed β€” retrosternal bypass esophagoplasty of the right half of the large intestine and the terminal ileum in the isoperistaltic position, as well as extirpation of the esophagus. As a result of long-term treatment and several surgical interventions, a good short-term and long-term result was obtained.Β Π›Π΅Ρ‡Π΅Π½ΠΈΠ΅ Π±ΠΎΠ»ΡŒΠ½Ρ‹Ρ… с химичСскими ΠΎΠΆΠΎΠ³Π°ΠΌΠΈ ΠΏΠΈΡ‰Π΅Π²ΠΎΠ΄Π° ΠΈ ΠΆΠ΅Π»ΡƒΠ΄ΠΊΠ° прСдставляСт ΡΠ»ΠΎΠΆΠ½ΡƒΡŽ Π·Π°Π΄Π°Ρ‡Ρƒ. Π˜ΡΡ…ΠΎΠ΄ΠΎΠΌ химичСских ΠΎΠΆΠΎΠ³ΠΎΠ² ΠΌΠΎΠΆΠ΅Ρ‚ Π±Ρ‹Ρ‚ΡŒ пСрфорация ΠΆΠ΅Π»ΡƒΠ΄ΠΊΠ° ΠΈΠ»ΠΈ Ρ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ стриктур ΠΏΠΈΡ‰Π΅Π²ΠΎΠ΄Π°, ΠΆΠ΅Π»ΡƒΠ΄ΠΊΠ°, двСнадцатипСрстной ΠΈ Π΄Π°ΠΆΠ΅ Π½Π°Ρ‡Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΎΡ‚Π΄Π΅Π»ΠΎΠ² Ρ‚ΠΎΡ‰Π΅ΠΉ кишки.Π‘ΠΎΠ»ΡŒΠ½Ρ‹Π΅ с сочСтанными ΠΎΠΆΠΎΠ³ΠΎΠ²Ρ‹ΠΌΠΈ стриктурами ΠΏΠΈΡ‰Π΅Π²ΠΎΠ΄Π° ΠΈ ΠΆΠ΅Π»ΡƒΠ΄ΠΊΠ° ΡΠ²Π»ΡΡŽΡ‚ΡΡ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ слоТными для лСчСния, ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ΅ часто Ρ‚Ρ€Π΅Π±ΡƒΠ΅Ρ‚ многоэтапных ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΉ.Π’ Π΄Π°Π½Π½ΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Π΅ описан клиничСский случай хирургичСского лСчСния ΠΏΠ°Ρ†ΠΈΠ΅Π½Ρ‚Π° с сочСтанным химичСским ΠΎΠΆΠΎΠ³ΠΎΠΌ ΠΏΠΈΡ‰Π΅Π²ΠΎΠ΄Π° ΠΈ ΠΆΠ΅Π»ΡƒΠ΄ΠΊΠ° соляной кислотой. Π§Π΅Ρ€Π΅Π· нСдСлю послС госпитализации ΠΏΡ€ΠΎΠΈΠ·ΠΎΡˆΠ»Π° пСрфорация ΠΆΠ΅Π»ΡƒΠ΄ΠΊΠ°. ΠŸΠ°Ρ†ΠΈΠ΅Π½Ρ‚ Π±Ρ‹Π» экстрСнно ΠΎΠΏΠ΅Ρ€ΠΈΡ€ΠΎΠ²Π°Π½ Π½Π° Ρ„ΠΎΠ½Π΅ ΠΏΠ΅Ρ€ΠΈΡ‚ΠΎΠ½ΠΈΡ‚Π°. ΠžΡΠΎΠ±Π΅Π½Π½ΠΎΡΡ‚ΡŒ ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΈ Π·Π°ΠΊΠ»ΡŽΡ‡Π°Π»Π°ΡΡŒ Π² Ρ‚ΠΎΠΌ, Ρ‡Ρ‚ΠΎ Ρ…ΠΈΡ€ΡƒΡ€Π³ΠΈ, сдСлав Π³Π°ΡΡ‚Ρ€ΡΠΊΡ‚ΠΎΠΌΠΈΡŽ, Π²Ρ‹Π²Π΅Π»ΠΈ ΠΊΡƒΠ»ΡŒΡ‚ΡŽ ΠΏΠΈΡ‰Π΅Π²ΠΎΠ΄Π° Π½Π° ΠΏΠ΅Ρ€Π΅Π΄Π½ΡŽΡŽ Π±Ρ€ΡŽΡˆΠ½ΡƒΡŽ стСнку Π² эпигастрии ΠΈ Π½Π°Π»ΠΎΠΆΠΈΠ»ΠΈ энтСростому. Π’ Ρ‚Π°ΠΊΠΎΠΌ состоянии с Π²Ρ‹Ρ€Π°ΠΆΠ΅Π½Π½Ρ‹ΠΌ Π°Π»ΠΈΠΌΠ΅Π½Ρ‚Π°Ρ€Π½Ρ‹ΠΌ истощСниСм (индСкс массы Ρ‚Π΅Π»Π° (ИМВ) β€” 15) 11.10.2002 больной Π±Ρ‹Π» доставлСн Π² ΠΌΠΎΡΠΊΠΎΠ²ΡΠΊΡƒΡŽ ΠΊΠ»ΠΈΠ½ΠΈΠΊΡƒ. Π’ качСствС основного хирургичСского лСчСния (спустя 1 Π³ΠΎΠ΄) Π±Ρ‹Π»Π° Π²Ρ‹ΠΏΠΎΠ»Π½Π΅Π½Π° рСконструктивная опСрация β€” загрудинная ΡˆΡƒΠ½Ρ‚ΠΈΡ€ΡƒΡŽΡ‰Π°Ρ эзофагопластика ΠΏΡ€Π°Π²ΠΎΠΉ ΠΏΠΎΠ»ΠΎΠ²ΠΈΠ½ΠΎΠΉ толстой кишки ΠΈ Ρ‚Π΅Ρ€ΠΌΠΈΠ½Π°Π»ΡŒΠ½Ρ‹ΠΌ ΠΎΡ‚Π΄Π΅Π»ΠΎΠΌ подвздошной кишки Π² ΠΈΠ·ΠΎΠΏΠ΅Ρ€ΠΈΡΡ‚Π°Π»ΡŒΡ‚ΠΈΡ‡Π΅ΡΠΊΠΎΠΉ ΠΏΠΎΠ·ΠΈΡ†ΠΈΠΈ, Π° Ρ‚Π°ΠΊΠΆΠ΅ экстирпация ΠΏΠΈΡ‰Π΅Π²ΠΎΠ΄Π°. Π’ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ лСчСния ΠΈ Π½Π΅ΡΠΊΠΎΠ»ΡŒΠΊΠΈΡ… ΠΎΠΏΠ΅Ρ€Π°Ρ‚ΠΈΠ²Π½Ρ‹Ρ… Π²ΠΌΠ΅ΡˆΠ°Ρ‚Π΅Π»ΡŒΡΡ‚Π² Π±Ρ‹Π»ΠΈ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ Ρ…ΠΎΡ€ΠΎΡˆΠΈΠ΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ Π² блиТайшСм ΠΈ ΠΎΡ‚Π΄Π°Π»Π΅Π½Π½ΠΎΠΌ ΠΏΠ΅Ρ€ΠΈΠΎΠ΄Π°Ρ….
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