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首页> 外文期刊>The Journal of Chemical Physics >The electron-spin magnetic moments (g factors) of O-3(-), O3Li, and O3Na: An ab initio study
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The electron-spin magnetic moments (g factors) of O-3(-), O3Li, and O3Na: An ab initio study

机译:O-3(-),O3Li和O3Na的电子自旋磁矩(g因子):从头算研究

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The electron-spin magnetic moments of O-3(-), O3Li, and O3Na, as parametrized by the g factors, are studied at the uncorrelated restricted open Hartree-Fock (ROHF) and correlated multireference configuration interaction (MRCI) ab initio levels. The present method, which uses a perturbative approach complete to second order, is based on a Breit-Pauli Hamiltonian. The calculated Delta g values, with Delta g=g-g(e), are very similar for all three species, confirming that the O-3(-) moiety is retained in the ozonides O3M. In the standard C-2v notation, Delta g(yy)>Delta g(zz)much greater thanDelta g(xx). The perpendicular component Delta g(xx) is small and negative, while the in-plane components Delta g(yy) and Delta g(zz) are large and positive. The MRCI results for Delta g(xx), Delta g(yy), Delta g(zz) (in ppm) are: -475, 16 673, 10 121 for O-3(-); -679, 13 894, 9308 for O3Li; and -494, 12 298, 8690 for O3Na. The ROHF values of Delta g(yy) and Delta g(zz) are smaller than the MRCI data, due to a general overestimation of the excitation energies. The MRCI Delta g values for isolated O-3(-) reproduce the experimental results for O-3(-) trapped in crystals or adsorbed on MgO surfaces (in ppm, -500-1200 for Delta g(xx), 12 400-16 400 for Delta g(yy), and 6900-10 000 for Delta g(zz)). For O3Na, the experimental Delta g(xx), Delta g(yy) Delta g(zz) data (-100, 14 200, 9800 ppm) are again satisfactorily described by our correlated results. No experimental g shifts are available for O3Li. In all systems studied here, the Delta g(xx) component is dictated by first-order terms (ground state expectation values); Delta g(yy) is governed by the second-order magnetic coupling between X B-2(1) and 1 (2)A(1) [electron excitation from the highest a(1) molecular orbital (MO) into the b(1)(pi*) singly occupied MO]; and Delta g(zz), by the coupling with two B-2(2) states (excitations from the two highest b(2) MOs into pi*). (C) 1998 American Institute of Physics. [S0021-9606(98)30744-8]. [References: 65]
机译:在不相关的受限开放式Hartree-Fock(ROHF)和相关的多参考构型相互作用(MRCI)从头计算水平下,研究了由g因子参数化的O-3(-),O3Li和O3Na的电子自旋磁矩。 。本方法使用完全二阶的摄动方法,基于Breit-Pauli Hamiltonian。对于所有三个物种,计算出的Delta g值与Delta g = g-g(e)极为相似,从而确认O-3(-)部分保留在臭氧化物O3M中。在标准C-2v表示法中,Delta g(yy)> Delta g(zz)远大于 Delta g(xx)。垂直分量Delta g(xx)小且为负,而平面内分量Delta g(yy)和Delta g(zz)大且为正。 Δg(xx),Δg(yy),Δg(zz)(以ppm为单位)的MRCI结果为:O-3(-)为-475、16 673、10 121; -O3Li -679、13 894、9308; O3Na为-494、12 298、8690。由于通常高估了激发能,所以Delta g(yy)和Delta g(zz)的ROHF值小于MRCI数据。分离的O-3(-)的MRCI Delta g值再现了晶体中捕获或吸附在MgO表面的O-3(-)的实验结果(以ppm为单位,Delta g(xx)为-500-1200,12400- Delta g(yy)为16400,Delta g(zz)为6900-10 000)。对于O3Na,我们的相关结果再次令人满意地描述了实验Delta g(xx),Delta g(yy)Delta g(zz)数据(-100、14 200、9800 ppm)。没有可用于O3Li的实验性g偏移。在本文研究的所有系统中,Delta g(xx)分量均由一阶项(基态期望值)决定; δg(yy)由X B-2(1)和1(2)A(1)之间的二阶磁耦合控制[从最高a(1)分子轨道(MO)进入b( 1)(pi *)单占MO];和Delta g(zz),通过与两个B-2(2)状态耦合(从两个最高的b(2)MO激发到pi *)。 (C)1998美国物理研究所。 [S0021-9606(98)30744-8]。 [参考:65]

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