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通过比较相同电子成分轨道的实验和DFT-B3LYP/6-311+G*理论的电子动量分布,系统研究了CF3Cl,CF2Cl2 和CFCl3分子外价壳层的轨道特性.研究结果表明CF3Cl,CF2Cl2 和CFCl3分子的Cl(3p)孤对电子轨道随着Cl原子个数增多,分子内相互作用逐渐增强,Cl原子3p轨道电子动量分布的特征逐渐淹没;F孤对电子轨道和的电子动量分布在高动量区出现了一个弱结构,且随Cl原子个数增多和F原子个数减少逐渐消失,这可能是由于部分轨道C-Cl 键电子成分的贡献;除3a1轨道外,C-F成键轨道和的理论的电子动量分布均在低动量端低于实验结果,可能是由于“d-like” 轨道低动量端的扭曲波效应;3a1轨道理论的电子动量分布均在 范围内低于实验结果,可能是由于扭曲波效应和电子关联等效应的影响. 相似文献
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自从70年代实现(e,2e)电子动量谱测量以来,电子动量谱学获得了巨大的发展,成为探测物质结构的强有力的手段[1]。它可以分辨壳层来获得原子分子价壳层轨道的动量空间的电子密度分布,尤其是对低动量端的电子分布非常敏感。二氧化碳分子是一种典型的线性分子,对其结构的深入研究,具有相当的应用价值,尤其在环境保护领域。以前,CO2分子的电子动量谱曾被测量过三次[2-4],但由于能量分辨或动量分辨较低,研究结果不能令人满意。因此,用电子动量谱学的实验手段,进一步研究CO2分子,是非常有意义的。…… 相似文献
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报道了环己烯(C6H10)分子2b和3a轨道电子动量谱的首次研究,并且给出了价轨道的电离能谱信息,实验在非共面对称几何条件下的能量多道型电子动量谱仪下完成,入射电子的能量为1200eV加结合能.通过Hartree-Fock和密度泛函方法计算得到了C6H10分子2b和3a轨道的动量谱,在动量大于0.25a.u.区域理论与实验结果符合较好,实验结果与理论计算相比在低动量端出现“上翘”的现象,这可能是由于分子的扭曲波效应引起的. 相似文献
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在600 eV, 1200 eV, 2400 eV三个入射能下首次实验测量了环己二烯的价壳层电离能谱和内价分子轨道4a的电子动量谱,并将实验结果与密度泛函理论和Hatree-Fock在不同基组下的计算作了比较. 相似文献
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在600 eV,1200 eV,2400 eV三个入射能下首次实验测量了环己二烯的价壳层电离能谱和内价分子轨道4a的电子动量谱,并将实验结果与密度泛函理论和Hatree-Fock在不同基组下的计算作了比较. 相似文献
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本文根据CS5Eu(N3)8的结构,用M.Reid的程序计算了它的晶场参数和强度参数,由此得出计算光谱图,同时通过能级拟合,对晶场能级进行了指认,并给出实验中的晶场参数.对它们的对称性进行了讨论. 相似文献
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研究包括连续通道等非处理通道的复极化势对(e,2e)碰撞过程三重微分截面的影响,即将耦合通道光学势方法得到的复极化势附加到畸变波玻恩近似方法的畸变势中,在靶态的HF近似下,计算了Ar原子和Ne原子在非共面对称几何条件下(e,2e)反应的三重微分截面.对于较高的入射能量,在实验的误差范围内,计算结果与电子动量谱的实验数据符合较好,复极化势的影响很小;对于较低的入射能量,复极化势的作用明显增大.
关键词:
复极化势
(e;2e)反应
三重微分截面
电子动量谱 相似文献
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精确的甲烷分子实验光谱参数在大气科学和天文探测等领域有着广泛的应用,特别是谱线的展宽系数及其温度依赖系数对于甲烷分子浓度廓线的研究尤为重要。精密的实验测量是获得准确谱线参数的重要手段。采用实验测量获取谱线参数时,需要在已知实验条件(浓度,温度,总压力,吸收光程以及气体分子种类的混合比等)的情况下,多次扫描同一波段范围得到多组实验室吸收光谱,然后利用基于非线性最小二乘法的拟合程序处理这些光谱,反演获得所需要的光谱参数。然而,一般常用的单光谱拟合程序处理实验光谱既费时又容易引起拟合过程中的误差传递。针对此问题,采用最小二乘拟合技术和Levenberg-Marquardt迭代算法编写了一款适用于处理由可调谐半导体激光吸收光谱技术(TDLAS)所获得的吸收光谱的多光谱拟合程序。该程序可同时处理多张实验光谱,并基于全局拟合方法获得一套光谱参数。详细介绍了该程序的原理、使用方法及数据处理过程。利用多光谱拟合程序中的Voigt线型处理了2 958~2 959 cm-1波数内甲烷(12CH4)分子6条跃迁谱线的实验光谱,获得了296.0,251.0,223.0,198.0和173.0 K共5组温度下12CH4分子6条谱线的空气展宽系数。与之前文献报道的该波段内采用单光谱拟合程序得到的相应数据对比结果表明:获得的各温度下的空气展宽系数与参考文献中相应数据差值的百分比处在-4.97%~1.58%之间,两者数据整体符合较好,并且在30组对比数据中,有4组由单光谱拟合程序得到的空气展宽系数的误差值小于由多光谱拟合程序得到的相应数值,有2组数据显示由两种方法获得的误差值相等,其余24组由多光谱拟合程序获得的数据拟合误差小于由单光谱拟合程序获得的相应数值,表明多光谱拟合程序具有良好的可靠性,适用于气体分子吸收光谱的处理。 相似文献
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本文应用 Gaussian03 程序包中提供的完全活性空间自洽场 (CASSCF) 方法,采用标准基组 6-311++G(3d,2p) 对 BH 分子X1∑+和B1∑+态势能曲线进行了单点能计算.在此基础上,利用相关理论将计算结果拟合到 Murrell-Sorbie函数得到了与各电子态相对应的光谱常数和力常数,并将计算结果与实验和其他理论结果进行了比较.同时,我们还利用光谱常数与力常数以及 Murrell-Sorbie函数之间的关系计算了与实验光谱数据相对应的力常数和 Murrell-Sorbie 函数,并与CASSCF结果进行了比较得出了一些有价值的结论.最后,对于具有双极小值的B1∑+态给出了更精确的定量的信息. 相似文献
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《Journal of Electron Spectroscopy and Related Phenomena》2005,142(3):325-334
Electron momentum spectroscopy (EMS) study of the neon valence satellites is reported. The experiments were performed at impact energies of 1250, 1450 and 1670 eV using a multichannel spectrometer that features high sensitivity. Binding energy spectra up to 100 eV and momentum profiles for the 2p−1 and 2s−1 primary transitions as well as the satellites are presented. The results are used to examine impact energy dependence of the relative intensities and shapes of the satellite momentum profiles. The results are also used to determine symmetries and spectroscopic factors of the satellites, and are compared with the previous experiments by EMS and photoelectron spectroscopy and sophisticated theoretical calculations. The present study has largely resolved controversies in the previous studies. 相似文献
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《Journal of Electron Spectroscopy and Related Phenomena》1998,87(3):231-251
The purpose of this paper is to first give an overview of the information obtained by electron momentum spectroscopy (EMS) on the electronic structure of different forms of solid carbon (single crystal graphite, polycrystalline carbon, different forms of amorphous carbon, and fullerenes). We show for sp2 bonded carbon that, with decreasing order, the structures observed change but certain basic features remain. sp3-bonded carbon films and fullerene films both have electronic structures different from these graphitic films. The results of EMS are compared with the results of other spectroscopic and scattering techniques. It is argued that the combination of energy and momentum resolution is crucial in order to get a clear picture of the changes in the electronic structure due to the changes in atomic arangements. Only EMS resolves both energy and momentum for all these solids. 相似文献
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《Journal of Physics and Chemistry of Solids》2003,64(3):495-505
The electronic band structures of Be and BeO have been measured by transmission electron momentum spectroscopy (EMS). The low atomic number of beryllium and the use of ultrathin solid films in these experiments reduce the probability of electron multiple scattering within the sample, resulting in very clean ‘benchmark’ measurements for the EMS technique. Experimental data are compared to tight-binding (LCAO) electronic structure calculations using Hartree–Fock , and local density (LDA-VWN), gradient corrected (PBE) and hybrid (PBE0) density functional theory. Overall, DFT calculations reproduce the EMS data for metallic Be reasonably well. PBE predictions for the valence bandwidth of Be are in excellent agreement with EMS data, provided the calculations employ a large basis set augmented with diffuse functions. For BeO, PBE calculations using a moderately sized basis set are in reasonable agreement with experiment, slightly underestimating the valence bandgap and overestimating the O(2s) and O(2p) bandwidths. The calculations also underestimate the EMS intensity of the O(2p) band around the Γ-point. Simulation of the effects of multiple scattering in the calculated oxide bandstructures do not explain these systematic differences. 相似文献
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《Journal of Electron Spectroscopy and Related Phenomena》1998,95(1):71-93
The development of a range of VAMAS format data files containing synthetic test spectra and their use in evaluating the peak fitting routines of three commercial XPS data analysis systems A, B and C, is reported. The synthetic spectra allow tests for: (1) acceptance of VAMAS formats with kinetic energy or binding energy scales that may have positive or negative abscissa increments; (2) Gaussian–Lorentzian sum or product function peaks; (3) effectiveness of Shirley background subtraction; (4) effectiveness of Tougaard background subtraction; (5) peak synthesis with partly resolved peaks with no background; and (6) peak synthesis with a Shirley background. The results show that all the data systems studied accept VAMAS format files but not all would accept both of the options of direction of scan. In addition, each data system had programming faults, some of which were later rectified.Synthetic spectra approximating the carbon 1s peaks for poly(methyl methacrylate), poly(vinyl acetate), poly(vinyl chloride) and poly(isobutylene) allow an analysis of accuracy of the fits in these tests. One full set of spectra is constructed with Gauss–Lorentz product function peaks and a second full set with Gauss–Lorentz sum function peaks since each software was designed for fitting only one of these options. The fitting of the individual peaks is only good for software using the same peak shapes as those of the data. The fit quality can deteriorate markedly for fitting to a peak shape different to that used in the peak fitting algorithm (ie fitting sum function peaks with product function software or vice versa). For unresolved peaks additional information is required to provide meaningful intensities. The three software systems studied all have different facilities but it is clear that the quality of convergence to the correct result gives a general order of preference in the fitting algorithm of B, A and C. Other aspects can favour software A which has more facilities. 相似文献