Abstract:Abstract. This work is devoted to the analysis of the orbital ordering patterns and associated interatomic magnetic interactions in the centrosymmetric monoclinic structures of BiMnO 3 , which have been recently determined experimentally. First, we set up an effective lattice fermion model for the manganese 3d bands and derive parameters of this model from first-principles electronic structure calculations. Then, we solve this model in terms of the mean-field Hartree-Fock method and obtain parameters of intera… Show more
“…For example, in BiMnO 3 such a mechanism facilitates the formation of the "##" AFM structure, which breaks the inversion symmetry. 16) Nevertheless, in RMnO 3 the situation appears to be different. For all considered compounds, the NN interactions calculated in the E-phase satisfy the following condition: J k 1 ð""Þ < J k 1 ð"#Þ, where the notations "" and "# are referred to the FM and AFM bonds, respectively (Fig.…”
Section: Solution and Analysis Of The Modelmentioning
confidence: 99%
“…16,27,31) After the solution for each magnetic state, the total energy changes corresponding to infinitesimal rotations of the spin magnetic moments near this state were mapped onto the Heisenberg model: 34,35) E Heis ¼ À 1 2…”
Section: Solution and Analysis Of The Modelmentioning
With the increase of the lattice distortion, the orthorhombic manganites RMnO 3 (R ¼ La, Pr, Nd, Tb, and Ho) are known to undergo the phase transition from the layered A-type antiferromagnetic (AFM) state to the zigzag E-type AFM state. We consider the microscopic origin of this transition. Our approach consists of the two parts. First, we construct an effective low-energy model for the manganese 3d-bands and derive parameters of this model from the first-principles electronic structure calculations. Then, we solve this model in the Hartree-Fock approximation (HFA) and analyze the behavior of the interatomic magnetic interactions. We argue that the nearest-neighbor interactions decrease with the increase of the distortion and at certain stage start to compete with the longer range (particularly, second-and thirdneighbor) AFM interactions in the orthorhombic ab-plane, which trigger the formation of the E-phase. The origin of these interactions is closely related to the orbital ordering, which takes place in the distorted orthorhombic structure. The model is able to capture the main experimental trends and explain why LaMnO 3 develops the A-type AFM order and why it tends to transform to the E-type AFM order in the more distorted compounds. Nevertheless, the quantitative agreement with the experimental data crucially depends on other factors, such as the magnetic polarization of the oxygen sites as well as the correlation interactions beyond HFA.
“…For example, in BiMnO 3 such a mechanism facilitates the formation of the "##" AFM structure, which breaks the inversion symmetry. 16) Nevertheless, in RMnO 3 the situation appears to be different. For all considered compounds, the NN interactions calculated in the E-phase satisfy the following condition: J k 1 ð""Þ < J k 1 ð"#Þ, where the notations "" and "# are referred to the FM and AFM bonds, respectively (Fig.…”
Section: Solution and Analysis Of The Modelmentioning
confidence: 99%
“…16,27,31) After the solution for each magnetic state, the total energy changes corresponding to infinitesimal rotations of the spin magnetic moments near this state were mapped onto the Heisenberg model: 34,35) E Heis ¼ À 1 2…”
Section: Solution and Analysis Of The Modelmentioning
With the increase of the lattice distortion, the orthorhombic manganites RMnO 3 (R ¼ La, Pr, Nd, Tb, and Ho) are known to undergo the phase transition from the layered A-type antiferromagnetic (AFM) state to the zigzag E-type AFM state. We consider the microscopic origin of this transition. Our approach consists of the two parts. First, we construct an effective low-energy model for the manganese 3d-bands and derive parameters of this model from the first-principles electronic structure calculations. Then, we solve this model in the Hartree-Fock approximation (HFA) and analyze the behavior of the interatomic magnetic interactions. We argue that the nearest-neighbor interactions decrease with the increase of the distortion and at certain stage start to compete with the longer range (particularly, second-and thirdneighbor) AFM interactions in the orthorhombic ab-plane, which trigger the formation of the E-phase. The origin of these interactions is closely related to the orbital ordering, which takes place in the distorted orthorhombic structure. The model is able to capture the main experimental trends and explain why LaMnO 3 develops the A-type AFM order and why it tends to transform to the E-type AFM order in the more distorted compounds. Nevertheless, the quantitative agreement with the experimental data crucially depends on other factors, such as the magnetic polarization of the oxygen sites as well as the correlation interactions beyond HFA.
“…Therefore the origin of ferroelectricity in these two compounds seems to be different. In BiMnO 3 the emergence of electric moment is connected with inversion symmetry breaking by the AFM order induced by particular orbital order below T = 474 K [42,43]. Another scenario for the onset of electric moment is possible in BiFeO 3 : an extensive investigation of ferroelectricity in BiFeO 3 in the framework of density functional theory was reported in reference [44].…”
Section: Calculated Magnetic Properties Of Bixo 3 (X = Mn Cr Fe)mentioning
The candidate multiferroic BiCrO 3 and its chemical neighbors BiMnO 3 and BiFeO 3 are known to be ferromagnetic and ferroelectric respectively. With structural distortions driven by the strongly polarizable Bi ions, we present results of the first-principles density functional calculations using the (FP-LMTO) method with the spin-orbit coupling for those materials in the pseudo-cubic perovskite phase. The results showed that the valence bands in these compounds are formed by the 6p orbitals of bismuth and 3d orbital's of the transition metals. Our results indicate that these materials have metallic behavior for spin-up polarization but being a clear tandance for semiconductor spin-down BiMnO 3 .
“…However, the results of recent experiments [7,8] have shown that this ferromagnetic crystal belongs to the C2/c symmetry group, which excludes the exist ence of spontaneous polarization [5][6][7][8][9]. External fac tors (temperature, pressure) can alter the magnetic structure of BiMnO 3 crystals so as to stabilize antifer romagnetism [8,9].…”
Section: Introductionmentioning
confidence: 97%
“…Bismuth manganite BiMnO 3 has been treated in many investigations as a multiferroelectric compound [1][2][3][4][5][6]. However, the results of recent experiments [7,8] have shown that this ferromagnetic crystal belongs to the C2/c symmetry group, which excludes the exist ence of spontaneous polarization [5][6][7][8][9].…”
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