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1.
在RHF(基离子在UHF和ROHF)/6-31G、6-31G、6-31+G和6-31+G水平优化得到C4O2S2m-(m=0,1,2,3,4)的平衡几何构型,发现从中性分子到-4价离子经历了一个从非芳香性体系到芳香性体系再到反芳香性体系的有趣变化过程,它们的稳定性顺序为:C4O2S2-·>C4O2S22->C4O2S2>C4O2S23-·>C4O2S24-.  相似文献   

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在RHF(基离子在UHF)/6-31G,6-31G*和6-31+G水平用从头算和Boys定域化方法计算了C4S4m-(m=0,1,2,3,4)的电子结构、电离势和定域化分子轨道。讨论了其成键特征和电离势与ΔESCF的关系。在6-31G水平用abinitio解析方法计算它们的谐振动频率。电子结构计算结果和Boys定域化分子轨道及振动分析结果与优化的平衡几何和相对稳定性相一致  相似文献   

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用从头算方法,在HF/STO-3G、HF/3-21G和HF/6-31G水平上研究了小硅化物SiX^m4的成键倾向性。计算结果表明,所研究的分子势能曲线均有稳定的极小值(SiLi4除外)。与已知的稳定分子SiH1、SiF4和SiCl4比较,含惰性元素的未知分子SiHe^4+4、SiNe^4+4和SiAr^4+4比含碱金属和碱土金属的未知分子SiLI4、SiNa4、SiBe^4+4和SiMg^4+4有  相似文献   

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以6-31G^*基组利用HF、MP2和DFT方法优化了超价化合物NLi4^n+和OLi4^n-的几何构型。研究结果表明,MP2和DFT法计算出的OLi4分子解离出Li和Li2的反应能与已有的实验值吻合,对于NLi4分子,得到其解离出Li和Li2的反应能分别为191.78和515.37kJ/mol(MP2值)。并预测了OLi4^n+和NLi4^n+分子的基振动频率。  相似文献   

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通过Fe3(CO)12、硫醇(硫酚)和EtMgBr所形成的络盐[(μ-CO)(μ-RS)Fe2(CO6)》-Mg^+Br与氯代芳酰氯的原位反应,合成了通式为(μ-RS)(μ-o-ClC6H4CO)Fe2(CO6)和(μ-RS)(μ-m-ClC6H4CO)Fe2(CO)6(R=n-Bu,t-Bu,Ph)的6个新桥芳酰基铁硫配合物,并用C/H分析、IR和^1HNMR表征了它们的结构。  相似文献   

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测得并解析了2个蝶状铁硒取代衍生物(μ-p-MeC6H4Se)2Fe2(CO)2(Ph2PCH2CH2PPh2)(A)和(μ-p-MeC6H4Se)2Fe2(CO)4(cis-Ph2PCH=CHPPH2)(B)的^1H-^1HCOSY谱和^1H-^15CCOSY谱以及A的^1H-^1HNOESR谱,从而进一不确证了它们的结构。  相似文献   

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将含不同负离子的苄基紫精分散在混合有PVP的MMA-HEMA共聚物基质中可制成耐水的光致变色膜。它们的光致变色速度的大小随紫精负离子的不同而有如下序列:V6(PF6^-)〉V5(BF4^-) ̄V4(ClO4^-)〉V3(CH3-苯环-SO3^-)〉V2(Br^-) ̄V1(Cl^-)。这与这些紫精在DMF中的溶解度以及在共聚物基质中的溶解性大小的序列相一致。负离子对这些光致变色膜在空气中的氧化退色速  相似文献   

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C4H5N-(NH3)n氢键团簇的多光子电力与从头计算   总被引:2,自引:0,他引:2  
在355和532nm激光波长下用TOF质谱仪研究了C4H5N-(NH3)n系列氢键团簇体系的多光子电离,实验发现,两波长下除了得到一系列团簇离子C4H5N-(NH3)n^+外,还观测到一系列质子化产物C4H5N-(NH3)n-H^+,这些质子化产物来自于光电离过程中团簇内部的质子转移反应;C4H5N-(NH3)n^+系列离子出现反常强度变化,即C4H5N-(NH3)2^+离子强度较C4H5N-(N  相似文献   

9.
宋礼成  伍伯牧 《结构化学》1995,14(5):393-398
通过η^5-CH3COC5H4(CO)3MoNa与(μ3-S)FeCo2(CO)9的反应俣成了(μ3-S)FeMoCo(η^5-CH3COC5H4(CO)81,1进一步(η^5-C5H5)Ni的反应合成了(μ3-S)-FeMoNi(η^5-CH3COC5H4)(CO)52,(μ3-S)FeMoNi(η^5-C5H5(η^5-C5H5)-(CO)53及(μ3-S)FeMoCo(η5-C5H5)(CO  相似文献   

10.
在6-31G水平上对3,4-二硫方酸(3,4-二巯基-3-环丁烯-1,2-二酮)的3种平面构象异构体进行SCF计算.结果表明,ZZ型异构体最稳定,ZE型次之,从等键反应能量分析3,4-二硫方酸的稳定性,与苯作比较探讨其芳香性.并在6-31G水平上计算了3种构象的振动频率.  相似文献   

11.
The crystal structure of LaIr4B4 has been refined from single crystal counter data. LaIr4B4 is tetragonal,P42/n,Z=2, isotypic with NdCo4B4, |F|/|F o|=0.039 for 312 independent reflections [|F o|>2 (F o)]. ThIr4B4 and ThOs4B4 also belong to the NdCo4B4-type structure. URu4B4 and UOs4B4 were found to crystallize with LuRu4B4-type structure. The crystal chemistry of (RE)T 4B4-phases is discussed and simple geometric relations are shown to exist between them.Dedicated to Prof.B. T. Matthias in celebration of his 60th birthday.  相似文献   

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Vibrational Spectra of As4S4 and As4Se4 The vibrational spectra of solid α- and β-As4S4 and the Raman spectrum of molten As4S4 have been recorded. The assignments of the frequencies are proposed mainly based on polarization data. The Raman melt spectra suggest that As4S4 molecules (symmetry D2d) are retained in the molten state. A partial decomposition of the melt by prolonged laser irradiation was observed. The Raman spectrum of solid As4Se4 is presented and the frequencies are tentatively assigned to an As4Se4 molecule of the cradle type, possessing D2d symmetry.  相似文献   

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Die erstmals dargestellten isotypen Verbindungen Ba4SiAs4, Ba4GeAs4, Sr4SiAs4 und Sr4GeAs4 kristallisieren kubisch, Raumgruppe P4 3n, mit 8 Formeleinheiten in der Elementarzelle: In den Strukturen liegen isolierte, d.h. nur von Ba-Ionen umgebene SiAs - bzw. GeAs -Tetraeder vor. Die Verbindungen sind die bisher eindrucksvollsten Beispiele für Zintlphasen mit komplexen Anionen. Zintl Phases with Isolated SiAs4 or GeAs4 Anions: Preparation and Structure of Ba4SiAs4, Ba4GeAs4, Sr4SiAs4, and Sr4GeAs4 The new compounds Ba4SiAs4, Ba4GeAs4, Sr4SiAs4, and Sr4GeAs4 have been prepared and their structures determined. They crystallize in the cubic system, P4 3n, with axes: data see “Inhaltsübersicht”. There are isolated SiAs or GeAs tetrahedra in the structures. The compounds can be interpreted as Zintl phases with complex anions.  相似文献   

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On K4PbO4 and Rb4PbO4 For the first time single crystals of K4[PbO4] have been prepared by heating K4PbO3 in O2. The structure has been refined [K4[PbO4]: 3029 I0(hkl), four circle diffractometer PW 1100, ω-scan, MoKα, R = 6.73%, Rw = 6.64%, P1 ; a = 658.62(15), b = 658.41(12), c = 986.64(21) pm, α = 79.74(2)°, β = 108.45(2)°, γ = 112.49(2)°, dx = 3.79 g · cm?3, dpyk = 3.78 g · cm?3, Z = 2; Rb4[PbO4]: a = 686.94(18), b = 684.43(18), c = 1020.73(21) pm, α = 79.28(2)°, β = 108.40(2)°, γ = 113.02(2)°, dx = 4.87 g · cm?3, dpyk = 4.85 g · cm?3, Z = 2, (from Rb2PbO3 and Rb2O)]. Both compounds are isotypic with K4SnO4. The Effective Coordination Numbers, ECoN, these via Mean Fictive Ionic Radii, MEFIR, are calculated.  相似文献   

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