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Carlos A. López 《General Relativity and Gravitation》1997,29(9):1095-1098
It is shown that uncharged test particles, released from rest at infinity in the Kerr-Newman field, stop and rebound when the radial coordinate r takes the value r0 = Q2/(2M). This expression corresponds to the position of a stationary source of the Kerr-Newman field found by the author. It represents the surface of a massive oblate ellipsoid of revolution undergoing rigid rotation. Besides, the magnitude of r0 guarantees that no violation of causality occurs throughout spacetime. Although the test particles' angular momenta are always zero, they acquire a rotational motion as a consequence of the dragging of inertial frames. 相似文献
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本文用pH电位法研究了在70%(v/v)乙醇-水溶液中Cd(II)与维生素D3(VD3)和乙二胺(en)或2,2'-联吡啶(bipy)在37±0.1℃和离子强度为0.10(KNO3)条件下, 三元混配配合物的稳定性。结果表明, 上述混合配位体系均形成稳定的1:1:1型混配配合物, 且△logK值均为较大的正值(分别为+1.06和+1.54), 但相应的logX值却并不很大(分别为2.18和2.83)。从统计效应和配合物分子内的配体间疏水相互作用, 讨论了造成这种反应常结果的可能原因, 并针对如何判断三元混配配合物相对稳定性高低等问题提出了作者的见解。 相似文献
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用一维自洽场晶体轨道法探讨了过渡金属夹心高聚物[(C~4BH~5)M]~n(M=Cr,Mn,Fe,Co,Ni)的一维链结构和电子结构.计算表明,堆积单元(C~4BH~5)M中价电子数为奇数的高聚物结构会发生Peierls畸变,而价电子数为偶数的将取规则结构,由能带结构得到, [(C~4BH~5)Mn]~n的前线能带出现交叉,可能会发生进一步的结构畸变,但也有可能保持非满状态,成为异体.[(C~4BH~5)Ni]~n可能是不稳定的.其余三个高聚物为半导体或绝缘体,这系列高聚物电荷载流子通路主要依赖于金属d轨道重叠. 相似文献
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In this paper, nineteen FD mass spectra of cyclic nucletides are repoted. The results indicated that only (M+ + H) peak presents in the spectra of cy-AMP, cy-CMP and cy-UMP. The derivatives of cy-AMP (except 7) have M+, (M+ + H) peaks, and the main fragments corresponding to (B + 1), (T + 1) peaks as shown in Fig. 1 in the Chinese Text. The adenosine 3', 5'-cyclic phosphite and its derivatives with P(III) are somewhat different as compared with P(Ve. In some cases neither M+ nor (M+ + H) is present in their spectra, but there are some characteristic peaks. Their fragmentation process has been shown in Fig. 2 in the Chinese Text. 相似文献
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多重散射Xα方法讨论了氟苯、苯胺、硝基苯和苯腈的电离能、π轨道的电荷分布、π轨道的系数及等值图形. 表明多重散射Xα方法的波函数和电荷分布在描述取代苯活化位置方面存在某种局限性, 讨论了改善的可能途径. 相似文献
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In 1975, Ashtekar and Magnon showed that anenergy condition selects a unique quantization procedurefor hypersurface orthogonal observers in general, curvedspacetimes. We generalize this result in two important ways, by eliminating the need toassume a particular form for the (quantum) Hamiltonian,and by considering the surprisingly nontrivial extensionto non-minimal coupling, for which the classical Hamiltonian differs from the classical energycalculated from the stress-energy tensor. 相似文献