实时直接分析高分辨质谱技术研究碳硼烷类化合物

该文运用高分辨质谱技术对实时直接分析(Direct analysis in real time,DART)离子化条件下碳硼烷化合物的质谱行为进行了研究,对碳硼烷化合物DART高分辨质谱中所得到的同位素峰簇进行了表征与归属。研究结果表明,选取的碳硼烷化合物在DART负离子条件下均能得到较好的质谱信号,这可能与硼笼结构的“缺电性”有关。含10个B原子的碳硼烷化合物形成的离子同位素峰簇信号中,通常情况下相对丰度最高的同位素峰中含2个10B以及8个11B。将碳硼烷化合物高分辨质谱分析的精确m/z数据信息与图谱中同位素峰轮廓分析相结合,是碳硼烷化合物有效的质谱定性分析与表征策略。     

C60-N-甲基吡咯烷衍生物直接进样电喷雾离子阱质谱表征

通过直接进样方式,采用电喷雾电离质谱技术分析了8个合成的富勒烯-N-甲基吡咯烷衍生物,详细研究了其在电喷雾条件下的质谱行为。由结果可知,该类化合物在电喷雾电离过程中易得到电子而负离子化;当衍生物结构中有相对易质子化基团或有活泼氢时,则可获得质子化和去质子的正负离子谱图;衍生物在负离子模式下容易失去吡咯环产生富勒烯负离子,且在合适能量碰撞下易发生衍生化基团内部的逆环加成反应,通过失去1个中性小分子物质CH2‖N—CH3,产生新的一取代亚甲基富勒烯衍生物。基于电喷雾电离源技术联合离子阱分析器建立的质谱分析方法,不但能提供准确的分子量信息,还能通过获得高分辨同位素谱峰和丰富的二级碎片离子峰,进一步确认化合物的分子结构,是一种先进、快速的富勒烯吡咯烷衍生物定性分析方法。     

MALDI质谱检测蛋白质与富勒醇的非共价复合物

基质辅助激光解吸电离(MALDI)质谱由于受到酸性基质、样品制备、激光诱导聚合和基质加合物的形成等条件的限制而难以用于非共价复合物的检测.本文以芥子酸为基质,观察到蛋白质与富勒醇的特殊相互作用,一些质谱特征,如质量数迁移、宽的加合峰和定量结合比表明,在蛋白质和富勒醇之间形成了特殊的非共价复合物.其中,血红蛋白与富勒醇的结合比是1:4,而肌红蛋白与富勒醇的结合比是1:1.实验结果表明:富勒醇可用来保护血红蛋白,有在酸性介质中防止其分解的作用.因此,通过在基质组份中添加特性有机化合物保护被测样品,有可能实现用MALDI质谱测定四级结构蛋白质的分子量.     

骨架掺硼富勒烯的合成及表征

在富勒佛被合成后不久，Smalley等人就开始利用B、N、St等元素制备非碳富勒烯和骨架掺杂富勒烯的研究，合成出了骨架掺氮富勒佛一C59N，在质谱中观察到了微观量的骨架接棚富勒烯C。。B等［’－’］，但迄今尚未见非碳富勒烯和骨架掺棚富勒烯宏观是合成的报导．用础部分取代富勒     

C75N+位置异构体的电子结构和光谱研究

杂原子的介入可改变纯碳笼的电子结构, 使其在超导、光电子器件及有机铁磁体等方面得到应用, 还可改善其氧化还原性能, 提高反应活性, 因而引起人们的研究兴趣[1～3]. Averdung[1]研究了C59N+与H的反应, 用质谱检测到C59NH和C59NH+2, 并用AM1方法优化其结构; Lamparth[2]以双氮杂富勒烯为前体, 合成了C59N+和C69N+, 测定中间体的 1H NMR谱、 UV谱及产物的FAB质谱, 并用 15N标记法证实了最强的碎片峰是N原子进入母体碳笼骨架所致. Diederich[3]观察到C76氮化物的FAB质谱信号, 但未给出进一步信息. 本文用INDO系列方法对氮杂富勒烯C75N+位置异构体的结构和稳定性进行理论研究, 找出最稳定的异构体, 计算其电子吸收光谱, 为实验室合成分离提供理论依据.     

高效液相色谱-串联质谱法测定稻谷和糙米中的溴硝醇

建立了稻谷和糙米中溴硝醇的高效液相色谱-串联质谱检测方法。样品采用酸性乙腈提取,经HLB固相萃取柱净化,以Hypersil GOLD-C₁₈柱分离,在负离子模式下采集数据,基质外标法定量。溴硝醇在电喷雾负离子模式下的母离子m/z 167.8,实际为溴硝醇发生反应后的产物2-溴-2-硝基乙醇的分子离子峰。溴硝醇在0～5.0μg/mL浓度范围内呈良好线性,线性相关系数大于0.99,平均回收率为86.2%～94.6%,相对标准偏差不超过13%。该方法适用于大批量粮谷样品中溴硝醇的快速检测。     

MAWLDI质谱检测蛋白质与富勒醇的非共价复合物

基质辅助激光解吸电离质谱由于受到酸性基质，样品制备，激光诱导聚合和基质加合物的形成等条件的限制而难以用于非共价复合物的检测。本文以芥子酸为基质，观察到蛋白质与富勒醇的特殊相互作用，一些质谱特征，如质量数迁移，宽的加合峰和定量结合比表明，在蛋白质和富勒醇之间形成了特殊的非共价复合物。     

sp2碳分子π电子构型和富勒醇结构模型

本文介绍了笔者课题组对富勒醇(含内嵌金属富勒醇)结构的理论研究结果。改进了传统Clar模型,使之可预测含杂原子、加成基团及配位金属的sp~2碳分子体系的化学稳定性,从而发展了富勒醇化学稳定性规则。利用该规则预测了化学稳定的富勒醇分子表面官能团的分布位置。通过计算和实验相结合的方法鉴定了富勒醇表面官能团的种类,建立了富勒醇的准确结构模型。编写了可自动筛选化学稳定的富勒醇分子结构的计算机程序。研究结果也可为其他sp~2碳材料多加成衍生物的结构预测提供参考。     

液相色谱-大气压化学电离质谱法分析人参中的人参皂甙

研究了用反相高效液相色谱-大气压化学电离质谱(HPLC/APCI-MS)分析人参皂甙的方法。液相色谱采用乙腈-水流动相进行梯度洗脱,质谱采用正负离子同时扫描并结合二级质谱进行定性,用选择反应离子模式(SRM)测定检测限。实验发现虽然人参皂甙是热不稳定物质,但在大气压化学电离质谱的高温汽化过程中仍能检测到很强的负离子分子离子峰,而且随着汽化温度的升高,人参皂甙的负离子分子离子峰的强度增加。该方法对人参皂甙Rb1和Rg1的检测限分别为1.2×10-13 g和3.0×10-14 g,并检测出白参中包括丙二酰人参皂甙在内的29种人参皂甙。该法灵敏度高,重复性好,结果准确,能有效地对药材提取物中的多种人参皂甙进行检测和结构分析。     

芦丁的电喷雾离子阱质谱分析

研究了芦丁在电喷雾离子阱质谱(ESI-MS)下的主要特征碎片离子及其裂解规律。应用电喷雾离子阱质谱技术研究芦丁的结构和正、负离子扫描条件下芦丁的主要特征碎片离子及其裂解规律。芦丁在正、负离子模式下均可得到较好的质谱信息,在正离子模式下,容易与Na+形成[M+Na]+的准分子离子,并裂解形成碎片m/z 605,487,331,325,313,185等,在负离子模式下,形成[M-H]-的准分子离子,并进一步碎裂形成碎片m/z 301,283,257,255,229,227,211等。分别阐明了芦丁在正、负离子模式下的电喷雾质谱碎裂规律,并对主要特征碎片离子进行归属,为进一步芦丁的结构优化和修饰提供了有价值的依据。     

Efficient and Convenient Preparation of Water-Soluble Fullerenol

An efficient and convenient preparation of fullerenols was described. With polyethylene glycol (PEG) 400 as catalyst, fullerenols were conveniently synthesized via the direct reaction of fullerene with aqueous NaOH. By control of reaction conditions, either water-soluble C60 fullerenol or water-insoluble C60 fullerenol could be obtained selectively.     

富勒醇清除OH自由基的ESR研究

富勒醇清除·ＯＨ自由基的ＥＳＲ研究祝严师，孙大勇，刘桂珍，刘子阳，詹瑞云，刘淑莹（中国科学院长春应用化学研究所应用谱学开放实验室，长春，１３００２２）关键词Ｃ_（６０），富勒醇，ＯＨ自由基，自旋捕捉，ＥＳＲ生物体内的许多现象均涉及到自由基反应，现已发?..     

A DFT study on structure, stability, and optical property of fullerenols

The impact of hydroxyl group adsorption on fullerene surface (namely fullerenol) has been systematically investigated in this study using the hybrid density-functional theory calculations. We find that the relative stability of fullerenol clearly depends on the distribution of hydroxyl group on the surface. The eight hydroxyl groups in C₂₀(OH)₈ structure show preference to accumulate on two adjoining five-numbered rings. Analysis of reaction energy indicates that the formation of fullerenol from the C₂₀ fullerene and hydroxyl group is energetically favorable. The highly hydroxylated fullerene is found to have high kinetic stability and low chemical reactivity, which is mostly associated with its electron distribution of HOMO and LUMO orbitals. In addition, the electronic structure of the most stable fullerenols has been analyzed by means of the total and partial density of states.     

Synthesis of Octadecahydroxylated C70

Synthesis of novel hydrophilic [70]fullerenols was described. The reaction involved an oleum-induced oxidative sulfation of the C₇₀ molecules with a product yield of 86%. The rate of fullerene sulfation was accelerated either moderately or greatly by the addition of P₂O₅ or SeO₂, respectively. Hydrolysis of the resulting polycyclosulfated C₇₀ in H₂O at 80°C afforded [70]fullerenols in a yield of more than 72%. The negative ion MALDI-TOF mass spectrum of [70]fullerenols showed a well-defined pattern of ion fragmentations with a nearly constant, consecutive weight increase in 17 mass units from the mass of C₇₀. Detection of a molecular ion at m/z 1146 was indicative for the composition of [70]fullerenols as octadecahydroxyfullerenes, containing 18 hydroxy addends per C₇₀ cage. That correlates the structure of their polycyclosulfated precursors to nonacyclosulfated [70]fullerenes, C₇₀(SO₄)₉.     

Structural and optical properties of highly hydroxylated fullerenes: stability of molecular domains on the C60 surface

The excitation spectra and the structural properties of highly hydroxylated C(60)(OH)(x) fullerenes (so-called fullerenols) are analyzed by comparing optical absorption experiments on dilute fullerenol-water solutions with semiempirical and density functional theory electronic structure calculations. The optical spectrum of fullerenol molecules with 24-28 OH attached to the carbon surface is characterized by the existence of broad bands with reduced intensities near the ultraviolet region (below approximately 500 nm) together with a complete absence of optical transitions in the visible part of the spectra, contrasting with the intense absorption observed in C(60) solutions. Our theoretical calculations of the absorption spectra, performed within the framework of the semiempirical Zerner intermediate neglect of diatomic differential overlap method [Reviews in Computational Chemistry II, edited by K. B. Lipkowitz and D. B. Boyd (VCH, Weinheim, 1991), Chap. 8, pp. 313-316] for various gas-phase-like C(60)(OH)(26) isomers, reveal that the excitation spectra of fullerenol molecules strongly depend on the degree of surface functionalization, the precise distribution of the OH groups on the carbon structure, and the presence of impurities in the samples. Interestingly, we have surprisingly found that low energy atomic configurations are obtained when the OH groups segregate on the C(60) surface forming molecular domains of different sizes. This patchy behavior for the hydroxyl molecules on the carbon surface leads in general to the formation of fullerene compounds with closed electronic shells, large highest occupied molecular orbital-lowest unoccupied molecular orbital energy gaps, and existence of an excitation spectrum that accounts for the main qualitative features observed in the experimental data.     

Isolation and characterization of unsymmetrical C(60)Me(5)O(3)H, a cage-opened bisepoxide ketone: tautomerism involving a fullerene cage bond

Bisepoxide ketone C(60)Me(5)O(3)H, possessing a nine-membered hole in the cage, has been isolated from the reaction of C(60)Cl(6) with methyllithium followed by hydrolysis. It is a tautomer of the recently isolated bisepoxide fullerenol, this tautomerism being the first example involving a cage C-C bond, and may be driven by cage strain. Like the fullerenol, the ketone gives a high C(58)(+) fragmentation ion intensity during EI mass spectrometry.     

Synergistic Effect of Phosphite with FuUerene C60 and Fullerenol C60（OH）24 as Antioxidants in Polypropylene

Polypropylene samples with fullerene C60, fullerenol C60（OH）24, 1010, C60/168, C60-OH/168 and 1010/168 as antioxidants were prepared by extrusions. MFR, YI, TGA and OIT of all the samples were tested. According to the results of MFR, during the melt extrusion, fullerene showed excellent stability effect on PP. The antioxidative ability of fullerene was comparable to the traditional antioxidant 1010. The antioxidative ability of fullerenol was not significant in the first extrusion and it accelerated the degradation of PP in the second and the third extrusions. TGA and OIT tests showed that the stability effects of fullerene and fullerenol were slightly lower than antioxidant 1010. In the first time, antioxidant 168 was reported to show great synergistic effects with fullerene and fullerenol as antioxidants, which sussested a simple way to enhance the antioxidative abilities of fullerene and fullerenol.     

A study on electron impact mass spectrometry of epoxy methylated fullerenols

Mass spectra of the epoxy methylated[60]fullerenols were obtained by EI mass spectrometry using "desorption" or "in-beam" technique. The mass spectra have an intense molecular monocation peak M(+) and a weak dication peak M(++), revealing the stability of these products under the MS (EI) conditions. The remaining peaks correspond to the successive loss of methyl groups and oxygen atoms for which the pure fullerene represents a more stable product. The distinction between the multiply charged fullerene C(60)(z+) and their fragments with equal m/z was also studied.     

Interaction Between C60 Fullerene and Alkali Metals Demonstrating Superconductivity

A discret summation method [1] has been used to calculate the van der Waals dispersion interactions between an alkali metal atom and individual C₆₀ fullerene molecules, as well as between an intercalated alkali metal atom and the face-centred-cubic lattice of solid fullerite. It is known [2, 3] that the conductivities observed in the doped C₆₀ films vary considerably for different alkali atoms. Our interest was to investigate any correlation between these conductivities and the long range potential field behaviour. In the present study, we have obtained interaction potential curves of the C₆₀ fullerene molecule including within its cage, as well the potential field topography within the overall C₆₀ fullerite solid unit cell. We have found that for all intercalated alkali metals, except Cs, there are voids within the unit-cell of fullerite where the dopant experiences attractive interactions. Whereas on the other hand, inside the fullerene cage only Li and Na experience attractive forces. Importantly, it has been shown that the localization of the crystallographic sites [4] of doped alkali metals in fullerite coincide with the potential energy minima of long range van der Waals forces.