C120O2的分子结构和光谱性质的理论研究

用INDO系列方法研究双笼氧化物C₁₂₀O₂分子可能异构体的结构,两个氧以桥键形式分别加成到两个碳笼上,在两个碳笼中间形成呋喃型五元环结构,有6/6连接和6/5连接两种C₂v构型.计算表明,C₁₂₀O₂两种构型中6/6连接的C₂v构型更稳定,其光谱与实验值相符.双笼氧化物C₁₂₀O₂的形成既缓解了C₆₀O环氧处的角张力,又比C₁₂₀O分子获得了更强的笼间相互作用,两个C₆₀靠两个呋喃型五元环连接在一起.两个碳笼的多位置直接键连使两碳笼距离较近,有较强的相互作用,但仍各自表现出一定的独立性.C₁₂₀O₂可发生分解生成新的化合物.     

C120NH的电子光谱和结构的理论研究

用INDO系列方法对双笼化合物C₁₂₀NH进行了理论研究,并预测C₁₂₀NH的形成缓解了C₆₀NH中亚胺基三元环处的角张力,从而较稳定;两碳笼直接键连使其相互间有较弱的相互作用,N仍具有较强的捕获质子能力,且有一定选择性;C₁₂₀NH的电子光谱与母体C₆₀及C₁₂₀O和C₁₂₀CH₂相似.     

双笼羰基化合物C120CO的理论研究

用INDO系列方法对双笼化合物C₁₂₀CO进行了理论研究,结果表明,C₁₂₀CO中O具有较大的电负性,在此位置可形成氢键.分子内电荷转移较大,非线性光学系数可能较大.C₁₂₀CO的电子光谱与C₁₂₀CH₂和C₁₂₀O的相似.     

自由基C69N及双体(C69N)2结构和电子光谱的理论研究

用INDO系列方法对自由基C₆₉N(Cs)及双体(C₆₉N)₂(C₂h)进行了理论研究,结果表明:笼骨架上N的掺入使C₇₀笼发生畸变,N向笼外突出,与氮相连的碳(6-6环上的C)自旋密度较大,2个C₆₉N自由基在这个碳上以C-C单键连接,形成双体为C₂h对称性,N与附近的3个碳均以单键连接,并不断开。理论计算的电子光谱与实验吻合较好,(C₆₉N)₂易分解为单体C₆₉N.     

中间体C60(CH3)-和产物C60(CH3)2的结构及产物

用INDO系列方法对C₆₀^2-与CH₃反应的中间体C₆₀(CH₃)^-进行理论研究,得到具有Cs对称性的构型。结果表明,CH₃加成到C₁₅上,将使与其相邻的双键碳(C₃₀)的电荷密度和自旋密度达极大值,故加成反应部位在C₃₀处;另外,C₁₅的对位C₁₂(或C₂₇)也较其它部位易于反应,且有两个反应场所,因而产物C₆₀(CH₃)₂可能为六元环上的1,2-加成和1,4-加成两种异构体的混合物。同时对两种加成产物的结构和电子光谱进行了理论研究,指认其电子跃迁,并讨论了其光谱红移的原因。     

C59O的结构、电子光谱及NMR谱的理论预测

用INDO系列方法对C₆₀的取代产物C₅₉O进行几何构型优化,得到Cs对称性的稳定构型,以此构型为基础,计算并预测了C₅₉O的电子光谱和NMR谱.最后与C₅₉O的等电子分子体C₆₀^2-及C₆₀O进行了比较.     

CnSi(n=49,50)的理论研究

用量子化学从头算方法研究了C_nSi(n=49,50)的各种可能的构型.结果表明,C₄₉Si为硅取代碳笼C₅₀中一个碳原子而形成的骨架硅杂碳笼,C₄₉Si与C₅₀相比稳定性较低,化学活性较高.C₅₀Si有两种类型结构:Ⅰ为外接型,Ⅱ为四连接型.计算结果表明,对C₅₀Si,外接硅型化合物更稳定,即Ⅰ为主要成分.计算结果与实验结果是一致的.     

聚并苯掺杂C60作锂离子电池负极材料的理论与性能研究

在AM1半经验方法水平上,对不同数目的Li⁺位于C₆₀笼内和笼外时形成的复合物进行几何优化,PAS负极材料由于掺杂C₆₀而吸附更多的Li⁺,并且Li⁺容易嵌入到C₆₀中,从理论上解释了聚并苯(PAS)导电性能改善的原因,并对PAS中掺杂C₆₀的最佳比例进行了预测.     

Ih对称性硼、碳原子簇化合物的从头计算(Ⅱ)─C12B20、C12B20H32的电子结构及稳定性

用价轨道双ζ型基,在B₃₂H₃₂^2-等研究的基础上继续对C₁₂B₂₀、C₁₂B₂₀H₃₂及其正离子进行从头计算,并对照C₂B₃₀、B₃₂和B₃₂H₃₂^2-的计算结果讨论其成键特性、稳定性及得电子反应活性。     

大黄素的电化学氧化还原机理研究

本文利用循环伏安法(CV)、红外光谱循环伏吸法(CVA)和导数循环伏吸法(DCVA)研究大黄素(Q)在乙腈溶剂中的电子转移机理.Q的还原过程中阴离子自由基Q^?-会结合中性分子Q生成二聚物Q₂^?-.Q₂^?-在更负的电位下进一步还原为Q₂^2-.当扫描范围为-0.2 ~ -2.0 V时,经过一个循环伏安过程,在扫描结束物质并没有回到反应物Q,而是Q₂^2-. Q₂^2-会继续发生电化学反应,经历两步一电子过程,分别生成Q₂^3-. 和Q₂^4-.,对应CV图中峰C₃和C₄.当扫描范围扩大至1.0~-2.0 V时,在更正的电位下,观察到两个新的氧化峰A₁和A₂,该范围内的三圈扫描结果表明,在扫描结束物质重新氧化回到Q.当扫描范围缩小至0.3 ~ -1.4 V,A2峰随着扫描圈数的增加而增大,与A2峰对应的氧化产物Q₂^?-在溶液中不断积累.A1峰对应于Q₂^?-氧化回到Q.     

C~1~2~0O的分子结构和光谱性质的理论研究

用INDO系列方法对双笼氧化物C~1~2~0O进行了理论研究,结果表明:双笼氧化物C~1~2~0O的形成缓解了C~6~0O中环氧三元环的角张力,并形成了呋喃型五元环将两碳笼连接在一起。两碳笼的直接键连使两笼距离较近,有较弱的相互作用,但仍各自表现一定的独立性,C~1~2~0O可发生分解生成新的化合物,C~1~2~0O的电子光谱与母体分子C~6~0相似。     

Theoretical study on the structures and electronic spectra of C120On (n=1,2)

ZINDO series calculations have been carried out to study the double‐cage oxides C₁₂₀O_n (n=1,2). The results show that the formation of a furan ring by the bridge‐bond between the two cages connected the two C₆₀ fullerene units and formed the C₁₂₀O with C_2v symmetry. C₁₂₀O₂ has two isomers with C_2v symmetry depending on either 6–6 or 6–5 connection between the two cages. Two furan rings and a pure four‐member ring form in this molecule. The formation of C₁₂₀O assuages the constraint of epoxide structure in C₆₀O, shortens the distance of the monomers, and produces some finite interaction between the two balls. More bonding in C₁₂₀O₂ shortens the distance of the two cages further and brings about stronger interaction. However, the two cages in C₁₂₀O_n (n=1,2) behave somehow independently that the electronic spectra of C₁₂₀O_n (n=1,2) are similar to those of C₆₀. The 6–6 connection isomer of C₁₂₀O₂ is more stable; its spectra are in good agreement with those of the experiment. The calculated electronic spectra of C₁₂₀O not only are in good agreement with the experiment in the ultraviolet region but also get some weak peaks in the visible region (>400 nm) not observed in experiment. © 2000 John Wiley & Sons, Inc. Int J Quant Chem 79: 291–307, 2000     

C120异构富勒烯分子的AM1半经验量子化学研究

以哑铃状2C60聚合体、花生壳状2C60聚合体以及C120富勒烯分子为研究对象,采用AM1半经验量子化学方法,计算了3种C120异构富勒烯分子的几何构型、电子结构、分子能量、疏水常数、极化率与偶极矩;然后,根据计算结果,分析对比了3种C120异构体分子的化学稳定性与物理化学特性.研究结果表明,3种C120分子的形成均为吸热反应,它们的稳定性排序为:C120富勒烯>花生壳状2C60>哑铃状2C60分子.     

High resolution and low-temperature photoelectron spectroscopy of an oxygen-linked fullerene dimer dianion: C(120)O(2-)

C(120)O comprises two C(60) cages linked by a furan ring and is formed by reactions of C(60)O and C(60). We have produced doubly charged anions of this fullerene dimer (C(120)O(2-)) and studied its electronic structure and stability using photoelectron spectroscopy and theoretical calculations. High resolution and vibrationally resolved photoelectron spectra were obtained at 70 K and at several photon energies. The second electron affinity of C(120)O was measured to be 1.02+/-0.03 eV and the intramolecular Coulomb repulsion was estimated to be about 0.8 eV in C(120)O(2-) on the basis of the observed repulsive Coulomb barrier. A low-lying excited state ((2)B(1)) was also observed for C(120)O(-) at 0.09 eV above the ground state ((2)A(1)). The C(120)O(2-) dianion can be viewed as a single electron on each C(60) ball very weakly coupled. Theoretical calculations showed that the singlet and triplet states of C(120)O(2-) are nearly degenerate and can both be present in the experiment. The computed electron binding energies and excitation energies, as well as Franck-Condon factors, are used to help interpret the photoelectron spectra. A C-C bond-cleaved isomer, C(60)-O-C(60) (2-), was also observed with a higher electron binding energy of 1.54 eV.     

Determination of the thermal stability of the fullerene dimers C120, C120O, and C120O2

We have produced the fullerene dimers C(120), C(120)O, and C(120)O(2) by a high-speed vibration milling technique. The thermal stability of C(120), C(120)O, and C(120)O(2) has been studied in the temperature range 150-350 degrees C for up to 4 h under vacuum. The bridging oxygen atoms were found to substantially increase the stability of the fullerene dimer molecules.     

异构体C36O的结构及其相对稳定性的理论研究

用abinitio方法和HF/STO-3G基组对Fullerenes的环氧衍生物C₃₆O所有可能的异构体进行非对称性限制下的结构优化,结合HF/6-31G水平上的单点能计算,确定其相对稳定性,得到等能量异构体的结构.张力分析的结果表明,C-O-C形成的三元环氧桥显著地削弱作用点附近C原子上所释放的张力,决定环氧位置选择性的关键因素不是碳笼上C原子的张力.对等能量异构体的红外光谱进行了理论预测.     

Artifacts in the electron paramagnetic resonance spectra of C60 fullerene ions: inevitable C120O impurity

Aspects of the electron paramagnetic resonance (EPR) spectra of C60n- fulleride ions (n = 2, 3) and the EPR signal observed in solid C60 are reinterpreted. Insufficient levels of reduction and the unrecognized presence of C120O, a ubiquitous and unavoidable impurity in air-exposed C60, have compromised most previously reported spectra of fullerides. Central narrow line width signals ("spikes") are ascribed to C120On- (n = odd). Signals arising from axial triplets (g approximately 2.0015, D = 26-29 G) in the spectrum of C602- are ascribed to C120On- (n = 2 or 4). Their D values are more realistic for C120O than C60. Less distinct signals from "powder" triplets (D approximately 11 G) are ascribed to aggregates of C120On- (n = odd) arising from freezing nonglassing solvents. In highly purified samples of C60, we find no evidence for a broad approximately 30 G signal previously assigned to a thermally accessible triplet of C60(2-). The C60(2-) ion is EPR-silent. Signals previously ascribed to a quartet state of the C60(3-) ion are ascribed to C120O4-. Uncomplicated, authentic spectra of C60- and C60(3-) become available when fully reduced samples are prepared under strictly anaerobic conditions from freshly HPLC-purified C60. Solid off-the-shelf C60 has an EPR signal (g approximately 2.0025, DeltaH(pp) approximately 1.5 G) that is commonly ascribed to the radical cation C60*+. This signal can be reproduced by exposing highly purified, EPR-silent C60 to oxygen in the dark. Doping C60 with an authentic C60*+ salt gives a signal with much greater line width (DeltaH(pp) = 6-8 G). It is suggested that the EPR signal in air-exposed samples of C60 arises from a peroxide-bridged diradical, *C60-O-O-C60* or its decomposition products rather than from C60*+. Solid-state C60 is more sensitive to oxygen than previously appreciated such that contamination with C120O is almost impossible to avoid.