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采用基于密度泛函理论的平面波赝势方法,在局域密度近似下采用线性响应的密度泛函微扰理论研究了具有六角结构的BaVS3化合物的晶格动力学性质,得到了整个声子谱.计算得到的Γ点拉曼频率和实验数据进行了比较,其中E22g模、A1g模和实验测量值符合得比较好.对于E32g模,采用线性响应计算的结果与实验值差别较大.对该模应用冻结声子方法研究后认为差异主要是由于E32g模的较强的非谐性引起的.此外V原子在平面内的振动模E12u出现了虚频.虚频的出现预示着六角相的BaVS3结构的不稳定性,从而很好地解释了该材料由六角相到正交相的结构相变.
关键词:
晶格动力学
密度泛函
赝势方法
3')" href="#">BaVS3 相似文献
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依据量子理论与配位场理论,利用群论和对称性分析的方法探讨了C42+分子在具有D4h对称性构型时,E(b1g+b2g)系统的Jahn-Teller效应中的相关问题.研究了C42+分子的电子态与声子态的对称性及其活跃声子态,讨论了系统声子间的耦合与CG系数,构建了E(b1g+b2g)系统的电声耦合哈密顿量,利用幺正平移变换将系统变换到了无声子激发的空间中,由此计算出了系统无声子激发的基态与激发态及其能级,结果表明由于系统的电声耦合作用缘故,在系统的势能面上形成了四个对称性势阱.无论系统处在哪一个势阱中,在Jahn-Teller畸变之后,系统的二重简并的能级都将发生分裂,分裂后系统电子态的简并性完全被消除.文中利用群论又进一步探讨了系统的Jahn-Teller畸变方向及其基态对称性,发现系统将沿着D4h→D2h方向发生畸变.畸变后C24+分子的基态具有D2h群下的B1u对称性. 相似文献
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测量了LaCoO3单相多晶样品的纵波与横波超声声速和衰减随温度的变化关系, 在材料的自 旋态转变温度附近(≈90K),纵波声速出现明显的软化并伴随一个尖锐的衰减峰,但是在 横波的测量中却没有出现类似的超声异常,分析认为LaCoO3在90K附近的自旋态 转变是由于Co3+离子是从低自旋态(LS,t62ge0 g)转变到中等自旋态(IS,t5 2ge1g ),而不是高等自旋态(HS,t42ge2g).随着温度的升高,在 200K附近纵波和横波测量上都观察到一个伴随着微小声速软化的宽大的衰减峰,这可能是随 机分布的IS态Co3+离子的Jahn-Teller效应导致的局域晶格扭曲所造成的.
关键词:
超声声速与衰减
自旋态转变
Jahn-Teller效应 相似文献
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本文采用Cu2+斜方对称电子顺磁共振(EPR)参量的高阶微扰公式计算了晶体Cu1-xHxZr2(PO4)3中Cu2+的EPR参量(g因子和超精细结构常数A因子).计算结果表明,晶体Cu1-xHxZr2(PO4)3中[CuO6]10-基团的Cu-O键长分别为R||≈0.241 nm,R⊥≈0.215 nm,平面键角τ≈80.1°;由于对称性降低,中心金属离子基态2A1g(θ)和2A1g(ε)有一定程度混合,混合系数α≈0.995.所得EPR谱图的理论计算值与实验数据符合得很好. 相似文献
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报道了H+5的实验结果.分析讨论了H+5的 形成和分解途径.根据理论分析,以稳定的H+3为核心与一个或多个氢分子结合可能形成稳定的H+ sup>n氢团簇离子.另一方面,在高频离子源中, 有发生H+3与H2反应的条件.实 验中,从高频离子源引出的离子束被静电加速器加速,然后用9
关键词:
+5团簇离子')" href="#">H+5团簇离子
3中性团簇')" href="#">H3中性团簇
4中性团簇')" href="#">H4中性团簇 相似文献
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本文利用反应显微成像技术(reaction microscope)研究了54 eV电子入射甲烷分子导致的电离解离过程,详细分析了电离解离产生的CH+2,CH+,C+离子碎片的动能分布情况.实验结果表明,该入射能量下产生CH+2,CH+,C+离子碎片主要贡献来自2a1内价轨道电子的直接电离过程产生的离子态(2a<
关键词:
反应显微成像谱仪
电离解离
能量沉积
动能分布 相似文献
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The low-temperature single-crystal polarized absorption and the luminescence spectra of Cs2[CrCl2(H2O)4]Cl3 are theoretically analyzed in order to determine the electronic structure of the trans-[CrCl2(H2O)4]+ complex. This study, based on the Racah theory, leads to a good agreement between the theoretical and experimental energy levels. The electronic-exited state 4T2g(Oh) is split into 4Eg and 4B2g components due to the lowering of the symmetry from Oh to D4h. The polarized absorption spectrum and the theoretical energies show that the 4Eg(D4h) state is lower in energy than the 4B2g(D4h) state. The resolved vibronic structure in the luminescence spectrum reveals a progression in a non-totally symmetric b1g mode, a manifestation of a Jahn-Teller effect in the emitting state 4T2g(Oh). Both Jahn-Teller and spin-orbit coupling in the orbitally degenerated 4Eg(D4h) state are necessary to account for the spectroscopic observations. 相似文献
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Complete diagonalization of the energy matrix and high order perturbation formulae of spin-Hamiltonian (SH) parameters possessing D4h symmetry for the 4d9 ion based on the crystal- and ligand-field theory in tetragonal symmetry are expressed and applied to the study of local distortion structure of the KCl:Ag2+ crystal. The calculated results agree well with experimental findings. Both complete diagonalization of energy matrix and high order perturbation approach are appropriate for the investigations of SH parameters of 4d9 ions in tetragonal crystals. Tetragonal distortion due to the Jahn-Teller effect for the tetragonal Ag2+ center at the K+ site of KCl crystal is also acquired from the calculations. 相似文献
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R. B. KING 《Molecular physics》2013,111(10):1567-1577
Topological representations (top-reps), which originally were developed to model molecular polyhedral isomerization processes, can be extended to depict the relationships between the polygons and polyhedra involved in Jahn-Teller (JT) distortions. Using this approach, the top-rep of the E ? (b 1g + b 2g) distortion of square planar molecules to rectangle and rhombus isomers becomes a rhombus in which the vertices alternately represent distortions to the rectangle and rhombus isomers. Similarly the top-rep of the E ? e distortion of regular Oh octahedra to elongated D4h tetragonal bipyramids becomes a triangle in which the vertices represent the three distinct tetragonal bipyramids from a given octahedron and the edge midpoints represent lower symmetry rhombic D2h intermediates. A regular octahedron can be used as a top-rep for the T ? (e + t 2) distortions of regular octahedra if the 6 vertices represent distortions to D4h tetragonal bipyramid isomers, the 8 face midpoints represent distortions to D3d trigonal antiprism isomers, and the 12 edge midpoints represent lower symmetry rhombic D2h intermediates. In the case of Jahn-Teller T ? h distortions of regular Ih icosahedra, the corresponding top-rep becomes a regular icosahedron in which the 12 vertices represent distortions to pentagonal D5d isomers, the 20 face midpoints represent distortions to trigonal D3d isomers, and the 30 edge midpoints represent D2h intermediates. A 4-dimensional analogue of the tetrahedron (i.e. the 4-simplex) can be used as a top-rep for the G ? g problem and the H ? g component of the H ? (g + 2h) problem for JT distortions of regular icosahedra. In this case the 5 vertices and the 10 edge midpoints correspond to Th isomers and D3d intermediates, respectively. 相似文献
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ABSTRACTThe variability of planar rings in Si4X4 (X?=?F, Cl, Br, I) molecules caused by the pseudo-Jahn–Teller impact (PJTE) was evaluated as an original PJTE work. Optimisation and the following frequency calculations in these molecules illustrated that in high-symmetry planar (with D4h symmetry) geometry, all of these compounds were unstable and their structures were puckered to lower C2h symmetry stable geometry. Furthermore, the vibronic coupling interaction between 1A1g ground and the first 1Eg excited states through (1A1g?+?1Eg) ? eg PJTE problem was the cause of non-planarity of the four-member ring and the symmetry breaking phenomenon in those series. The calculated gaps (Δ) between the ground state and the Eg excited state, the vibronic coupling (F) and ground state primary force constant values (k1) were obtained from the numerical fitting of the ground state adiabatic potential energy surface with the analytical expressions of these molecules. Finally, natural bond analysis (NBO) was used for the design of the strongest interaction and natural atomic charges of these structures. 相似文献
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Elastic, strength, electronic properties and vibrational spectra of Ne@C60 (I h) in its ground electronic state (X 1Ag) were investigated with density functional theory at B3PW91/6-31G level via structure distortions. The elastic properties were obtained from the potential energy curves (PECs) in all of the five independent distortional directions of the molecule with symmetries of 1. D 5d, 2. D 3d, 3. D 2h, 4. C 2h(1) and 5. C 2h(2). PECs were examined where the structure of Ne@C60 was destroyed. The necessary energies to destroy the structure were thus obtained, which illuminated the stability of Ne@C60. PECs were found to be anisotropic and were accurately fitted to polynomials. Elongations in the direction of D 5d and compression in D 2h encountered potential energy surface cross-linkages, which might be considered as a single electron pump for further application in the design of single electron devices. Time-dependent B3PW91/6-31G analysis predicted significant electronic spectra changes associated with structure distortions. Similarities and differences of the properties were compared with those in C60 and He@C60. 相似文献
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The electron paramagnetic resonance parameters, zero-field splittings (ZFSs) b20, b40, b44, b60, b64 and the g factors for Gd3+ on the tetragonal Y3+ site in KY3F10 are theoretically studied from the superposition model for the ZFSs and the approximation formula for the g factor containing the admixture of the ground 8S7/2 and the excited 6L7/2 (L=P, D, F, G) states via the spin-orbit coupling interactions, respectively. By analysing the above ZFSs, the local structure
information for the impurity Gd3+ is obtained, i.e., the impurity-ligand bonding angles related to the four-fold (C4) axis for the impurity Gd3+ center are found to be about 0.6° larger than those for the host Y3+ site in KY3F10. The calculated ZFSs based on the above angular distortion as well as the g factors are in reasonable agreement with the observed values. The present studies on the ZFSs and the local structure would
be helpful to understand the optical and magnetic properties of this material with Gd dopants.
相似文献