{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"Similar to the cases of 3d(n) ions in 4-fold (or 8-fold) and 6-fold cubic coordinations, a simple and uniform method that calculates the spin-lattice coupling coefficients G11 and G44 for those ions in the more complex 12-fold cubic coordination from the derivatives of zero-field splittings in low symmetries with respect to the distinct structural parameters has been established. Through this method, the analytic expressions of G11 and G44 for 3d5 ions in this cubic coordination based on various mechanisms and models have been given. The results are rather different from those in 4-fold (or 8-fold) and 6-fold cubic coordinations. As an example, the coefficients G11 and G44 for Fe3+ in K+ site ( 12-fold cubic coordination) as well as Ta5+ site (6-fold cubic coordination) of KTaO3 crystal are studied from the important spin-orbit coupling mechanism. When we compare these results with the experimental findings, it appears that the Fe3+ ion is in a Ta5+ site, and not in a K+ site as shown by some researchers.","authors":[],"categoryName":"|","doi":"","fpage":"35","id":"0f1c5243-a28b-45ed-a5c7-4f2ad08156a9","issue":"1","journal":{"abbrevTitle":"PBM","id":"b1289047-807c-4b57-bffc-a126ac2ffa2a","issnPpub":"0921-4526","publisherId":"PBM","title":"Physica B-Condensed Matter"},"keywords":[{"id":"a40c8bb1-9704-4df6-9c6e-543425ceb7f7","keyword":"s-6-state ions;symmetry;formulas","originalKeyword":"s-6-state ions;symmetry;formulas"}],"language":"en","publisherId":"0921-4526_1992_1_1","title":"SPIN-LATTICE COUPLING-COEFFICIENTS G(11) AND G(44) FOR 3D(5) IONS IN 12-FOLD CUBIC COORDINATION","volume":"179","year":"1992"},{"abstractinfo":"The local structures and the g factors g (//) and g (aSyen) for the isoelectronic 3d(9) ions Cu(2+) and Ni(+) in CdS are theoretically investigated from the perturbation formulas of these parameters for a 3d(9) ion under trigonally distorted tetrahedral environments. In consideration of significant covalency of the [MS(4)] combinations (M = Cu and Ni), the ligand orbital and spin-orbit coupling contributions are taken into account using the cluster approach. Based on the studies, the substitutional impurity Cu(2+) (or Ni(+)) on Cd(2+) site is found to undergo a small inward displacement 0.026 (or a slight outward shift 0.017 ) towards (or away from) the ligand triangle along C (3) axis. The theoretical g factors for both ions based on the above impurity displacements are in good agreement with the experimental data.","authors":[],"categoryName":"|","doi":"","fpage":"483","id":"d001d26e-a3f0-46a4-be3e-0a0310199cef","issue":"9","journal":{"abbrevTitle":"PACOM","id":"a33fbe7a-b9a6-47f0-bc33-74bfc411a55a","issnPpub":"0342-1791","publisherId":"PACOM","title":"Physics and Chemistry of Minerals"},"keywords":[{"id":"641815fc-a516-4ef7-a908-3b540dca0863","keyword":"Electron paramagnetic resonance;Defect structures;Crystal-fields and;spin Hamiltonians;Cu(2+);Ni(+);CdS;electron-paramagnetic-resonance;atomic screening constants;defect;structures;crystal-field;3d impurities;scf functions;semiconductors;parameters;epr;spectra","originalKeyword":"Electron paramagnetic resonance;Defect structures;Crystal-fields and;spin Hamiltonians;Cu(2+);Ni(+);CdS;electron-paramagnetic-resonance;atomic screening constants;defect;structures;crystal-field;3d impurities;scf functions;semiconductors;parameters;epr;spectra"}],"language":"en","publisherId":"0342-1791_2009_9_1","title":"Theoretical investigations of the local structures and the g factors for 3d(9) ions in CdS","volume":"36","year":"2009"},{"abstractinfo":"By successively taking into account various interactions for d(2) ions in trigonally distorted cubic crystal fields, detailed analyses, derivations and calculations of the zero-field splitting (ZFS) and g factors of the ground state have been carried out; and their physical essentials and origins have been clearly revealed. The mistakes and shortcomings in some references have been corrected and improved. The calculated results are in excellent agreement with experimental data and much better than those of previous work. It is found that both the combined action of the trigonal field and spin-orbit interaction and the interaction between the ground state and excited states are quite necessary for causing ZFS of the ground state, and both the spin-orbit interaction and the admixture between the ground state and excited states are necessary for causing the deviation of g factors of the ground state from spin-only values.","authors":[],"categoryName":"|","doi":"","fpage":"373","id":"c6a0f23a-b097-4950-b26e-4e5817363995","issue":"3","journal":{"abbrevTitle":"CITP","id":"45f28bf6-874e-4b98-936f-4562e2c56a77","issnPpub":"0253-6102","publisherId":"CITP","title":"Communications in Theoretical Physics"},"keywords":[{"id":"b5add049-cdb2-4ccb-bc22-523810952e04","keyword":"zero-field splitting;g factors;d(2) ions;crystal field;combined;action;admixture of wavefunction","originalKeyword":"zero-field splitting;g factors;d(2) ions;crystal field;combined;action;admixture of wavefunction"}],"language":"en","publisherId":"0253-6102_1998_3_1","title":"Zero-field splitting and g factors for d(2) ions in trigonally distorted cubic crystal fields","volume":"30","year":"1998"},{"abstractinfo":"The Wang-Landau algorithm is used to study the thermodynamic and magnetic properties of triangular spin-chain system based on two-dimensional Ising model in order to understand the magnetic-order dynamics in Ca(3)Co(2)O(6) compound. The calculated results demonstrate that the equilibrium state of the rigid spins produces the two-step magnetization curve at low temperature even when the random-exchange term is considered. This work indicates that the four-step magnetization behavior observed experimentally must be due to the nonequilibrium magnetization.","authors":[],"categoryName":"|","doi":"","fpage":"","id":"e9390bb3-bf93-4252-99d0-4fe8f8106ef5","issue":"17","journal":{"abbrevTitle":"PRB","id":"48ba155b-d6de-484c-bd85-973be949b8c5","issnPpub":"1098-0121","publisherId":"PRB","title":"Physical Review B"},"keywords":[{"id":"bd83375f-1639-4e72-ac12-cd2db66ceb84","keyword":"calcium compounds;exchange interactions (electron);Ising model;magnetisation;thermodynamics;one-dimensional ca3co2o6;density-of-states;compound ca3co2o6;phase-diagram;proteins;crystal","originalKeyword":"calcium compounds;exchange interactions (electron);Ising model;magnetisation;thermodynamics;one-dimensional ca3co2o6;density-of-states;compound ca3co2o6;phase-diagram;proteins;crystal"}],"language":"en","publisherId":"1098-0121_2009_17_1","title":"Two-step magnetization in a spin-chain system on the triangular lattice: Wang-Landau simulation","volume":"79","year":"2009"},{"abstractinfo":"The g-shifts Ag( = g-g(s), where g(s) approximate to 2.0023 is the free-ion value) of the isoelectronic 3d(3) series Cr3+. Mn4+ and Fe5+ in SrTiO3 crystals are calculated from the high-order perturbation formula based on the cluster approach for 3d3 ion in cubic octahedral site. The formula includes not only the contribution from the crystal-field (CF) mechanism, but also that from the charge-transfer (CT) mechanism (which is omitted in the CF theory). From the calculations, it is found that the contribution Delta g(CT) from the CT mechanism in sign is contrary to the corresponding Delta g(CF) from the CF mechanism and the relative importance of CT mechanism (characterized by vertical bar Delta g(CT)/Delta g(CF)vertical bar) increases with the increasing valence state (and hence the atomic number) of 3d(3) ion. The positive g-shift Delta g of SrTiO3:Fe5+ is due mainly to the contribution of CT mechanism. So, for the explanations of g factors of the high valence state 3d\" ions (e.g. Mn4+ and Fe5+) in crystals, the contributions from both CF and CT mechanisms should be taken into account. (c) 2005 Elsevier Ltd. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"1701","id":"5cbbf474-9bbd-4350-a583-7eedea5d0fa8","issue":"10","journal":{"abbrevTitle":"JOPACOS","id":"6268f571-fbc6-4d83-a6ed-a357d820c3df","issnPpub":"0022-3697","publisherId":"JOPACOS","title":"Journal of Physics and Chemistry of Solids"},"keywords":[{"id":"aa9af8e5-99a7-4737-9bcf-8c24c5215235","keyword":"oxides;crystal fields;electronic paramagnetic resonance;optical;properties;electron-paramagnetic-resonance;atomic screening constants;scf;functions;luminescence;parameters;spectra;temperature;manganese;lattices;csmgbr3","originalKeyword":"oxides;crystal fields;electronic paramagnetic resonance;optical;properties;electron-paramagnetic-resonance;atomic screening constants;scf;functions;luminescence;parameters;spectra;temperature;manganese;lattices;csmgbr3"}],"language":"en","publisherId":"0022-3697_2005_10_1","title":"Studies of EPR g factors of the isoelectronic 3d(3) series Cr3+Mn4+ and Fe5+ in SrTiO3 crystals","volume":"66","year":"2005"},{"abstractinfo":"By the use of a first principles density functional theory, two kinds of models, namely the Rice-Wang thermodynamics model and the Seah quasi-chemical model, are employed to evaluate the embrittling tendency of a grain boundary (GB) due to the 3d element segregation. The first principles method based on those two models is appropriate for calculating the chemical and structural relaxation contributions to the changes of GB cohesion with the 3d segregants. The effects of the 3d transition elements, such as Ti, V, Cr and Mn, on a stable fcc Fe Sigma 11 [1 (1) over bar0]/(11 (3) over bar) GB are studied and the difference between these two models is interpreted. When the chemical and the structural relaxation effects are taken into account, the calculated results for these two models are coincident for most of the elements studied, except for chromium. After analysing their chemical bonding in detail, we find that this discrepancy may be attributable to a lower susceptibility of the Seah model to the bonding anisotropy caused by Cr in the GB. It is proposed that the Seah model should be prudently used for some elements, especially those lying in the middle of a transition period.","authors":[],"categoryName":"|","doi":"","fpage":"8339","id":"37899acc-40b6-41f8-b101-1f656ec7ef0d","issue":"49","journal":{"abbrevTitle":"JOPM","id":"f0e359df-48a6-4a7f-b16d-2389d3e793ee","issnPpub":"0953-8984","publisherId":"JOPM","title":"Journal of Physics-Condensed Matter"},"keywords":[{"id":"50b55621-5ef4-4bf8-aa6d-4843d27b2d2c","keyword":"phosphorus;adsorption;interstitials;decohesion;magnetism;systems;cluster;metals;boron","originalKeyword":"phosphorus;adsorption;interstitials;decohesion;magnetism;systems;cluster;metals;boron"}],"language":"en","publisherId":"0953-8984_2003_49_2","title":"The effects of 3d alloying elements on grain boundary cohesion in gamma-iron: a first principles study on interface embrittlement due to the segregation","volume":"15","year":"2003"},{"abstractinfo":"A uniform und simple method suitable to all d(n) ions is established for the calculation of spin-lattice coupling coefficients G11 and G44 in T(d) symmetry. According to the method, the coefficients G11 and G44 for Fe3+ ion in GaP crystal have been obtained from the high-order perturbation formulae of zero-field splitting in tetragonal and trigonal fields based on the spin-orbit coupling mechanism. The calculated results show good agreement with the experimental findings.","authors":[],"categoryName":"|","doi":"","fpage":"1667","id":"b233426d-25e3-4999-b670-db679a79cdaa","issue":"12","journal":{"abbrevTitle":"NCDSIDFDMAMACPFPB","id":"bcd17c32-87fa-4d95-98ec-1b9776853fad","issnPpub":"0392-6737","publisherId":"NCDSIDFDMAMACPFPB","title":"Nuovo Cimento Della Societa Italiana Di Fisica D-Condensed Matter Atomic Molecular and Chemical Physics Fluids Plasmas Biophysics"},"keywords":[{"id":"e29dba05-8a11-4633-af02-10296ff05c28","keyword":"level splitting and interaction;electron paramagnetic resonance and;relaxation;crystal and ligand fields;d-orbital theory;ions","originalKeyword":"level splitting and interaction;electron paramagnetic resonance and;relaxation;crystal and ligand fields;d-orbital theory;ions"}],"language":"en","publisherId":"0392-6737_1990_12_1","title":"CALCULATION OF THE SPIN-LATTICE COUPLING-COEFFICIENTS G11 AND G44 FOR GAP-FE(3+) CRYSTAL","volume":"12","year":"1990"},{"abstractinfo":"The perturbation formula of g factor for 3d(7) ion in cubic octahedral crystals has been obtained from a cluster approach. In the formula, the parameters related to the configuration interaction and the covalency reduction effect can be obtained from the optical spectra of the crystal under study and so no adjustable parameters are applied. From the formula, the g factors for Co2+ in fluoroperovskites LiBaF3, KMBF3, KZnF3 and CsCdF3 are calculated. The calculated results are in agreement with the observed values. The g factor following the order of LiBaF3 : Co2+ < KMgF3 : Co2+ < KZnF3: Co2+ < CsCdF3 : Co2+ is also explained. (C) 2000 Elsevier Science B.V. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"123","id":"62c668d3-8a7a-4941-ae93-9f4dcb8d2312","issue":"42737","journal":{"abbrevTitle":"PBM","id":"b1289047-807c-4b57-bffc-a126ac2ffa2a","issnPpub":"0921-4526","publisherId":"PBM","title":"Physica B-Condensed Matter"},"keywords":[{"id":"55561ec9-e5ab-430c-854a-11a4884d9adc","keyword":"electron paramagnetic resonance;crystal- and ligand-field theory;Co2+;LiBaF3;KMgF3;KZnF3;CsCdF3;perovskite;transition;impurities;crystals","originalKeyword":"electron paramagnetic resonance;crystal- and ligand-field theory;Co2+;LiBaF3;KMgF3;KZnF3;CsCdF3;perovskite;transition;impurities;crystals"}],"language":"en","publisherId":"0921-4526_2000_42737_3","title":"Investigations of the g factors for Co2+ in fluoroperovskites","volume":"291","year":"2000"},{"abstractinfo":"The EPR g factors of Cr3+ in NaCrS2 and NaCrSe2 crystals are calculated from the high-order perturbation formulas based on the one-spin-orbit (SO)-coupling-parameter (i.e., the SO-coupling-parameter of the central 3d(n) ion) as well as the two-SO-coupling-parameter (i.e., the SO-coupling-parameter of the 3d(n) ion and that of ligands) models for 3d(n) ions in cubic octahedral sites. The calculated results (in particular for NaCrSe2) based on the two-SO-coupling-parameter model are closer to the observed values than those based on the one-SO-coupling-parameter model, suggesting that for calculations of the g factor of 3d(n) ions in covalent crystals the two-SO-coupling-parameter model is preferable to the one-SO-coupling-parameter model. The reasonableness of the calculated results from the two-SO-coupling-parameter model is discussed.","authors":[],"categoryName":"|","doi":"","fpage":"369","id":"7cd913b5-5e5c-4fdb-b635-79afd36e3fcb","issue":"5","journal":{"abbrevTitle":"ZFNSAJOPS","id":"1a5d2a8e-76c4-4142-a409-c3fb08d6eea4","issnPpub":"0932-0784","publisherId":"ZFNSAJOPS","title":"Zeitschrift Fur Naturforschung Section a-a Journal of Physical Sciences"},"keywords":[{"id":"d65d165b-153e-4dc4-b119-bb7b7768dd0c","keyword":"electron paramagnetic resonance;crystal- and ligand-field theory;spin-orbit coupling;Cr3+;NaCrS2;NaCrSe2;atomic screening constants;chromium(iii) sulfides;scf functions;crystals;selenides;resonance;spectra","originalKeyword":"electron paramagnetic resonance;crystal- and ligand-field theory;spin-orbit coupling;Cr3+;NaCrS2;NaCrSe2;atomic screening constants;chromium(iii) sulfides;scf functions;crystals;selenides;resonance;spectra"}],"language":"en","publisherId":"0932-0784_2005_5_1","title":"Investigations of the EPR g factors of NaCrS2 and NaCrSe2","volume":"60","year":"2005"},{"abstractinfo":"This paper presents a cluster approach to the calculation of the g factors for 3d(7) ions in cubic octahedral crystals, in which the parameters related to the configuration interaction and the covalency reduction effects are obtained from optical spectra of the studied crystals, and so no adjustable parameters are applied. From the approach, the g factors for MgO:Co2+ and CaO:Co2+ are calculated. The calculated results show good agreement with the observed values. The experimental values of g < 4.333 (the first order value in absence of configuration and covalency interactions) for MgO:Co2+ and g > 4.333 for CaO:Co2+ are also explained.","authors":[],"categoryName":"|","doi":"","fpage":"249","id":"e6ab3f87-938a-4036-81be-2771c67ff0f7","issue":"42798","journal":{"abbrevTitle":"ZFNSAJOPS","id":"1a5d2a8e-76c4-4142-a409-c3fb08d6eea4","issnPpub":"0932-0784","publisherId":"ZFNSAJOPS","title":"Zeitschrift Fur Naturforschung Section a-a Journal of Physical Sciences"},"keywords":[{"id":"fd41ffcd-60c4-412c-841e-c209e7a591ff","keyword":"electron paramagnetic resonance (EPR);crystal-field theory;Co2+ ion;MgO;CaO","originalKeyword":"electron paramagnetic resonance (EPR);crystal-field theory;Co2+ ion;MgO;CaO"}],"language":"en","publisherId":"0932-0784_2001_42798_2","title":"Theoretical studies of the g factors for Co2+ in MgO and CaO crystals","volume":"56","year":"2001"}],"totalpage":2267,"totalrecord":22670}