The Structural, Electronic and Vibrational Properties of LaCrO 3 $$ {}_3 $$ . A Quantum Mechanical Investigation by Using an All Electron Gaussian Type Basis Set and a Full Range Hybrid Functional

IF 4.8 3区 化学 Q2 CHEMISTRY, MULTIDISCIPLINARY Journal of Computational Chemistry Pub Date : 2025-02-04 DOI:10.1002/jcc.27523
Khaled E. El-Kelany, Alexander Platonenko, Klaus Doll, Roberto Dovesi
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Abstract

The geometrical, electronic and vibrational properties of LaCrO 3 $$ {}_3 $$ have been investigated by using an all electron Gaussian type basis set, the B3LYP functional and the CRYSTAL code, and compared with KVF 3 $$ {}_3 $$ : in the two compounds the transition metal is formally in d 3 $$ {}^3 $$ configuration. The high spin t 2 g 3 $$ {}_{2g}^3 $$ ground state excludes the Jahn Teller deformation and the orbital ordering. The energy gain due to the rotation of the octahedra (from the cubic space group Pm 3 ¯ m $$ \overline{3}\mathrm{m} $$ , N. 221, to space group P 4 m bm $$ P\frac{4}{m} bm $$ , N.127, and to I 4 m cm $$ I\frac{4}{m} cm $$ , N. 140) in the oxide is about 70 times larger than in the fluoride (5.4 vs. 0.08 mE h $$ {}_h $$ ), due to the larger electrostatic forces (a factor four, as the formal charge doubles in going from F to O2−) and the consequently reduced B-X distances. In KVF 3 $$ {}_3 $$ , the p states of fluorine are separated by 6.4 eV from the d states of vanadium, whose band is quite narrow (1 eV). In the oxide, on the contrary, the oxygen p states overlap to a large amount with the d states of chromium, whose band is more than 6 eV large. The FM and AFM energy differences, the spin density maps and profiles, and the Mulliken analysis data are also provided for documenting the differences between the oxide and the fluoride.

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LaCrO3的结构、电子和振动性能。全电子高斯型基集和全范围混合泛函的量子力学研究
利用全电子高斯型基集、B3LYP泛函和CRYSTAL代码研究了LaCrO3 $$ {}_3 $$的几何、电子和振动性质,并与KVF3 $$ {}_3 $$进行了比较:在这两种化合物中,过渡金属形式为d3 $$ {}^3 $$构型。高自旋t2∑g3 $$ {}_{2g}^3 $$基态排除了扬特勒变形和轨道有序。八面体在氧化物中的旋转(从立方空间群Pm3¯m $$ \overline{3}\mathrm{m} $$, N. 221,到空间群P²4m²bm $$ P\frac{4}{m} bm $$, N.127,到I²4m²cm $$ I\frac{4}{m} cm $$, N. 140)所获得的能量增益大约是氟原子中的70倍(5.4 vs. 0.08 mEh $$ {}_h $$),这是由于更大的静电力(一个因子4,因为形式电荷在从F−到O2−的过程中加倍)和因此减小的B-X距离。在KVF3 $$ {}_3 $$中,氟的p态与钒的d态相隔6.4 eV,其能带很窄(1 eV)。相反,在氧化物中,氧的p态与铬的d态有大量重叠,其能带大于6 eV。FM和AFM的能量差,自旋密度图和轮廓,以及Mulliken分析数据也提供了记录氧化物和氟化物之间的差异。
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来源期刊
CiteScore
6.60
自引率
3.30%
发文量
247
审稿时长
1.7 months
期刊介绍: This distinguished journal publishes articles concerned with all aspects of computational chemistry: analytical, biological, inorganic, organic, physical, and materials. The Journal of Computational Chemistry presents original research, contemporary developments in theory and methodology, and state-of-the-art applications. Computational areas that are featured in the journal include ab initio and semiempirical quantum mechanics, density functional theory, molecular mechanics, molecular dynamics, statistical mechanics, cheminformatics, biomolecular structure prediction, molecular design, and bioinformatics.
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