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ENERGIES AND STRUCTURES OF ROTATING ARGON CLUSTERS - ANALYTIC DESCRIPTIONS AND NUMERICAL SIMULATIONS

机译:旋转氩气团的能量和结构-分析说明和数值模拟

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The dependence of the rotational energy of small argon clusters on the magnitude and direction of their rotational angular momenta is obtained by two different methods, namely, by analytic descriptions parametric in structural variables (centrifugal displacements) and by classical simulations carried out in rotating frames so that rotational angular momenta are conserved. Potential energies are taken as additive Ar, pair potentials [R. A. Aziz, J. Chem. Phys. 99, 4518 (1993)], augmented in some cases by three-body Axilrod-Teller interactions, thus complementing our earlier studies of rare-gas clusters modeled by additive Lennard-Jones oscillator (LJO) pair potentials [L. L. Lohr and C. H. Huben, J. Chem. Phys. 99, 6369 (1993)]. Quartic and sextic spectroscopic constants are found to be approximately 10% smaller when the Aziz pair potential is used, reflecting its greater stiffness as compared to the LJO potential. The sign of the sextic tensor coefficient for both tetrahedral Ar, and octahedral Ar-6 is such that for sufficiently high J the C-2v (or D-2h) structures with J parallel to a pseudo-C-2 (or true C-2) axis (saddle points on the rotational energy surface at low J) become local energy maxima, the D-2d (or D-4h) structures with J parallel to an S-4 (or C-4) axis representing the energy minima. The trigonal bipyramidal cluster Ar-4 resembles both Ar-3 and Ar-4 in its rotational characteristics but with reduced manifestations of nonrigidity. As found with an LJO pair potential [D. H. Li and J. Jellinek, Z. Phys. D 12, 177 (1989)], the icosahedral Ar-13 cluster displays a very slight preference for D-3d structures with J parallel to a C-3 axis, while the D-5d structures with J parallel to a C-5 axis are energy maxima and the D-2h structures with J parallel to a C-2 axis are saddle points on the rotational energy surface. The scalar quartic spectroscopic coefficient for Ar-13 is found to be 2.15 x 10(-4) times that for the reference diatomic Ar-2. A variety of structural instabilities are described for Ar-13 clusters with very high rotational energies. (C) 1996 John Wiley & Sons, Inc. [References: 30]
机译:小氩气团簇的旋转能量对它们的旋转角动量的大小和方向的依赖关系通过两种不同的方法来获得,即通过对结构变量(离心位移)的参数化分析描述以及在旋转框架中进行的经典模拟来获得。保持旋转角动量。势能被作为加成Ar,成对势[R。 A.Aziz,J.Chem。物理99,4518(1993)],在某些情况下通过三体Axilrod-Teller相互作用而增强,从而补充了我们先前对由累加Lennard-Jones振荡器(LJO)对势建模的稀有气体团簇的研究[L。 L.Lohr和C.H.Huben,J.Chem。物理99,6369(1993)]。发现当使用阿齐兹对电位时,四次和六性光谱常数小大约10%,反映出与LJO电位相比,其更大的刚度。四面体Ar和八面体Ar-6的六方张量系数的符号是​​这样的:对于足够高的J,C-2v(或D-2h)结构的J与伪C-2(或真实C- 2)轴(在低J处旋转能量表面上的鞍点)成为局部能量最大值,D-2d(或D-4h)结构的J平行于S-4(或C-4)轴,表示能量最小值。三角双锥团簇Ar-4的旋转特性类似于Ar-3和Ar-4,但具有减少的非刚性表现。如发现具有LJO对电位[D. H. Li和J. Jellinek,Z. Phys。 D 12,177(1989)],二十面体Ar-13簇显示J平行于C-3轴的D-3d结构非常偏爱,而J平行于C-5轴的D-5d结构是能量最大值,J平行于C-2轴的D-2h结构是旋转能面上的鞍点。发现Ar-13的标量四次光谱系数是参考双原子Ar-2的2.15 x 10(-4)倍。描述了具有非常高的旋转能的Ar-13团簇的各种结构不稳定性。 (C)1996 John Wiley&Sons,Inc. [参考:30]

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