激光溅射-分子束法研究镁、铝离子与乙腈分子的气相化学反应

利用激光溅射-分子束技术研究了Mg+、 Al+与乙腈分子的气相团簇反应.根据反射式飞行时间质谱检测的结果发现, Mg+、 Al+与乙腈分子反应形成不同尺寸的团簇离子产物,其中Al+与(CHCN)n的结合数n=1～10,而Mg+与(CHCN)n的结合数n=1～5. Al+(CHCN)n、 Mg+(CHCN)n团簇离子产物的强度分布都存在明显的强度间隙现象. Al+与(CHCN)n进行缔合时,出现了两个强度间隙;而Mg+与(CHCN)n进行缔合时,则只存在一个强度间隙. Al+的第一强度间隙在n=4～5,第二强度间隙在n=6～7;而Mg+的强度间隙在n=2～3.     

激光烧蚀Al+与乙醇团簇的反应研究

利用激光烧蚀-分子束法对Al等离子体与乙醇团簇的反应进行了研究.飞行时间质谱测得的主要反应产物有Al⁺(C₂H₅OH)_n (n=3～10)与H⁺(C₂H₅OH)_n (n=1～14)团簇正离子和(C₂H₅OH)_n(H₂O)OH^- (n=0～8)团簇负离子.实验发现,烧蚀产生的Al等离子体与脉冲分子束的不同位置反应,对团簇离子的类别、大小及强度分布均产生很大影响.Al等离子体与脉冲分子束的前段反应,主要产生金属-复合物团簇离子Al⁺(C₂H₅OH)_n,且信号较强;Al等离子体与脉冲分子束的中段及后段反应,主要产生质子化团簇离子H⁺(C₂H₅OH)_n和团簇负离子(C₂H₅OH)_n(H₂O)OH^-,同时还出现强度较小的其他水合团簇离子,如H⁺(H₂O)m(C₂H₅OH)_n (m=1～2)等.     

气相过渡金属钽和钇-碳链团簇的质谱研究

Nd:YAG产生的二倍频532nm激光消融金属靶表面,同时含有3%乙炔的氦载气喷向旋转的金属靶,通过等离子体反应形成中性的气相过度金属-碳链团簇分子。经过超声膨胀,由Skimmer形成准直的分子束,进入飞行时间质谱仪的电离区,被193nm的准分子激光电离。实验发现,钽奇数碳链的过渡金属钽团簇离子信号较小,而偶数碳链的团簇离子信号较大。钇碳链观察到了YCm+(m=1～4,6)、Y2Cn+(n=2,4,6)和YCnH2+(n=2～6)的离子信号。     

甲醇团簇的多光子电离质谱及其从头算

用355 nm激光对脉冲分子束超声膨胀冷却的甲醇分子进行多光子电离, 飞行时间质谱仪观测到除甲醇碎片离子外的质子化甲醇团簇(CH3OH)nH+(n=1-16), 且离子的种类及相对强度与激光相对于脉冲分子束的延时无关, 取决于团簇离子内在结构的稳定性. 结合从头算密度泛函理论, 在B3LYP/6-31G(d)基组水平上优化得到了(CH3OH)n和(CH3OH)nH+(n=1-4)的稳定构型. 振动频谱分析显示, 团簇中最强的红外振动模主要来自氢键H伸缩振动的贡献. 团簇电离后发生于团簇内的质子转移反应也可能与激光电离引起的与氢键有关的振动模激发密切相关.     

邻羟基萘甲醛缩对二甲氨基苯甲酰腙的合成及其对锌离子的识别

设计并合成了用于识别锌离子的荧光传感分子——2-羟基-1-萘甲醛缩-4-二甲氨基苯甲酰腙(1),其结构经1H NMR,IR和MS表征。利用荧光光谱研究了在乙腈中1对过渡金属离子(Zn2+,Cd2+,Cu2+,Hg2+,Pb2+和N i2+)的识别能力。结果表明:1表现出对Zn2+的良好选择性,Zn2+的加入导致1的长波长荧光增强449倍。Job曲线确定1与Zn2+形成1∶1型配合物。     

质子转移反应质谱的建立与性能研究

报道了自行研制的质子转移反应质谱的基本结构和性能。利用水蒸气辉光放电产生了反应离子H3O ,以合成空气为反应气体,测量了H3O 与合成空气中的水反应产生的团簇离子H3O (H2O)n的质谱。实验发现,当漂移管电场与分子密度比值为144Td时,增加的离子能量可以阻止团簇离子H3O (H2O)n的形成,质谱观察到的离子主要是H3O ,其纯度可达99%以上,这时H3O 与有机物分子如甲苯的质子转移反应的产物离子也呈单一形式,团簇离子得到很好地抑制。根据离子强度和离子反应时间等参数,获得了PTR-MS目前的检出限为10-8(V/V)。利用PTR-MS对标准浓度甲苯及其稀释气体进行检测,表明PTR-MS在线定量检测准确性良好,线性动态范围跨越3个数量级,能够应用于大气中痕量挥发性有机物的实时在线测量。     

8-氨基喹啉取代苯甲酰胺衍生物对汞离子和铜离子的识别

设计合成了可识别金属离子的荧光传感分子8-氨基喹啉取代苯甲酰胺衍生物,通过核磁共振谱和质谱表征其结构;利用其光谱性质研究了该系列物质对过渡金属离子Cu2+,Hg2+,Pb2+,Zn2+,Ni2+和Cd2+的识别性质,初步探讨了其识别机理。实验表明:在乙腈中,8-氨基喹啉苯甲酰胺的吸收光谱在509nm处对Cu2+有响应,溶液由无色变成红色;而其荧光光谱对Hg2+和Cu2+有良好的选择性,荧光增强倍率分别高达368和192,与金属离子形成结合比为1:1配合物。     

应用反射式飞行时间质谱仪研究氨团簇离子解离动力学

用直射式和反射式飞行时间质谱研究了氨分子团簇体系在 355 nm激光下的多光子电离,得到一系列的质子化团簇离子 (NH3)nH+,同时还观察到超价氨团簇离子 (NH3)n H2＋。在反射式飞行时间质谱研究中观测到质子化氨团簇离子在自由飞行过程中的解离现象,表明在该实验条件下生成的质子化氨团簇离子是一些亚稳态团簇离子。对子离子产率的分析,得到质子化团簇离子解离速率常数,从而可以估计亚稳态团簇离子的寿命。团簇尺寸从 n＝3增大到 20,其寿命从 21 ms减小到 120 μs,大约小了两个数量级。解离速率在 n＝5到 6有一个阶跃式上升,这是由于 5个氨组成的质子化团簇离子(NH3)4NH4+ 的结构相对比较稳定。     

ICP-MS/MS法测定壳聚糖中的重金属元素

建立了ICP-MS/MS测定壳聚糖中重金属元素的分析方法。壳聚糖经3%的柠檬酸溶解,采用ICP-M S/M S直接进样测定样品溶液中的8个重金属元素Cr,Co,Ni,Cu,As,Cd,Hg,Pb。在M S/M S模式下,基于Cr~+,Co~+,Ni~+,Cu~+能与NH_3反应形成团簇离子,采用NH_3/He质量转移法消除了Cr,Co,Ni,Cu的质谱干扰;基于As~+能与O_2反应形成AsO~+,采用O_2质量转移法消除了As的质谱干扰;基于Cd~+的干扰离子能与O_2发生质量转移反应,而Cd~+不与O_2发生反应,采用O_2原位质量法消除了Cd的质谱干扰。元素的检出限范围0. 38～6. 20 ng/L。采用所建立的分析方法对实际样品进行分析,样品的加标回收率在94. 5%～105. 5%之间,相对标准偏差≤3. 8%,方法适用于壳聚糖中多个重金属元素测定。     

配合物[Cr3(μ3-O)(Tc)6(H2O)3]·(NO3)·4H2O的水热合成及晶体结构

通过有限个过渡金属离子如Fe,Ni,Cr,Mn与O、OH、-O或-O2CR等桥联原子或基团键合形成的具有不同尺寸的环形轮状金属离子簇合物或分子簇合物是近年来的研究热点之一[1,2].它们不仅具有独特的结构,而且在催化、非线性光学、分子自组装等方面具有潜在的应用价值[3～5].特别是具有三角型结构的过渡金属-氧轮簇化合物由于可以作为单分子磁体的磁性交换和电子耦合的研究体系,引起了研究人员的极大地兴趣[6,7].研究表明,具有[M(μ3-O)(O2CR)6L3]0/+,(M=Fe3+或Mn3+,L为水或吡啶,R为烷基或芳香基团)结构的化合物具有反铁磁作用[8,9].     

Laser ablation and secondary ion mass spectrometry of inorganic transition-metal compounds. Part I: comparison between static ToF-SIMS and LA-FTICRMS

Most of the first-row transition-metal oxides, M(A)O(B) (M = Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn) were examined by static secondary ion mass spectrometry (s-SIMS) and laser ablation/ionization Fourier transform ion cyclotron resonance mass spectrometry (LA-FTICRMS). Positive and negative ions show strong correlation between the studied oxide and the detected cluster ions. Specific M(x)O(y) (+/-) species were systematically observed with both MS techniques for each investigated M(A)O(B) transition-metal oxide. Moreover, the ion composition and ion distribution are greatly dependent on the ionization technique. Laser ablation (LA)/ionization leads to larger cluster ions (ionic species with nearly hundred atoms were in particular detected for Sc2O3 and Y2O3 oxides), whereas hydrogenated, dihydrogenated, and sometimes trihydrogenated species were observed in s-SIMS. However, the ion distribution for a given M(x)O(y) (+/-) ion series (i.e. ions including the same number of metal atoms M) generally presented important similarities in both techniques.Finally, it was demonstrated that the chemical state of metal atoms in the observed ionic species is closely dependent on the metal electronic valence shell. High valence states (+III, +IV, +V, and +VI) are favored for metals with a less-than-half full valence shell configuration, whereas for other first-row transition metals (manganese, iron, cobalt, nickel, copper and zinc) lower metal valence states (0, +I or, +II) are involved.     

CO在铜基催化剂上活化及助催剂作用本质的量子化学研究

提出了CO在助促和非助促的铜基催化剂上吸附活化的两种活性中心原子族模型Cu_5和Cu_4M~(n+)O。应用电荷自洽离散变分X_a近似计算方法对CO在这两种模型上活化本质,并对过渡金属助催剂离子M~(n+)(从ⅣA—ⅧA族中各选一个V~(3+),Ti~(3+),Fe~(3+),Mn~(2+),Mo~(4+))与合成甲醇铜基催化剂上金属铜原子相互作用的本质及其对CO活化的效应进行量子化学研究。计算表明CO是以碳端吸附在活性中心模型Cu_4M~(n+)O中的Cu(1)原子上,并向助催剂M~(n+)离子倾斜45°。从吸附态CO—Cu_5和CO—Cu_4M~(n+)O的原子簇轨道,态密度以及C—O间重选集居数的计算结果指出,CO分子受到活化。助催剂与催化剂中铜原子间相互作用影响了铜原子的价态,改变体系E_f能级,改善了前线轨道HOMO与CO 2π~*轨道的匹配,从而增加d电子的反馈,降低CO间的重选集居数,促进了CO的活化。     

Binuclear cyclopentadienylmetal cyclooctatetraene derivatives of the first row transition metals: effects of ring conformation on the bonding of an eight-membered carbocyclic ring to a pair of metal atoms

Binuclear Cp(2)M(2)(μ-C(8)H(8)) derivatives have been synthesized for M = V, Cr, Co, and Ni and have now been studied theoretically for the entire first row of transition metals from Ti to Ni. The early transition metal derivatives Cp(2)M(2)(μ-C(8)H(8)) (M = Ti, V, Cr. Mn) are predicted to form low-energy cis-Cp(2)M(2)(μ-C(8)H(8)) structures with a folded C(8)H(8) ring (dihedral angle ～130°) and short metal-metal distances suggesting multiple bonding. These predicted structures are close to the experimental structures for M = V, Cr with V≡V and Cr≡Cr bond lengths of ～2.48 and ～2.36 ?, respectively. The middle to late transition metals form trans-Cp(2)M(2)(μ-C(8)H(8)) structures (M = Mn, Fe, Co, Ni) with a twisted μ-C(8)H(8) ring and no metal-metal bonding. The hapticity of the central μ-C(8)H(8) ring in such structures ranges from five for Mn and Fe to four for Co and three for Ni and thus depend on the electronic requirements of the central metal atom. This leads to the favored 18-electron configuration for both metal atoms in the singlet Fe, Co, and Ni structures but only 17-electron metal configurations in the triplet Mn structure. In addition, the late transition metals form trans-Cp(2)M(2)(μ-C(8)H(8)) structures (M = Fe, Co, Ni), with the tub conformation of the μ-C(8)H(8) ring functioning as a tetrahapto (M = Fe, Co) or trihapto (M = Ni) ligand to each CpM group. A μ-C(8)H(8) ring in the tub conformation also bonds to two CpFe units as a bis(tetrahapto) ligand in both singlet and triplet cis-Cp(2)Fe(2)(μ-C(8)H(8)) structures.     

Reactions of first-row transition metal ions with propargyl alcohol in the gas phase

The gas-phase reactions with propargyl alcohol (PPA) of all the singly charged ions of the first-row transition metals, generated by laser ablation in an external ion source, were studied by Fourier transform ion cyclotron resonance mass spectrometry (FT-ICRMS.). The reactivities of the metal ions change irregularly across the periodic table, and the reactivity of each ion is a function of its electronic configuration and corresponding metal-oxygen (M-O) bond energies. The 10 metal ions were classified into three categories according to their reactivities: Sc(+), Ti(+) and V(+) are the most reactive ions which react with PPA to give many kinds of oxygen-rich products due to stronger M-O bonds; Fe(+), Co(+) and Ni(+) are less reactive; Cr(+), Mn(+), Cu(+) and Zn(+) are the most unreactive ions, due to the half and completely occupied valence electronic configurations. The order of reactivity is Ti(+) > V(+) > Sc(+) > Co(+) > Fe(+) approximately Ni(+) > Zn(+) > Cr(+) approximately Mn(+) approximately Cu(+).     

Spin quenching of transition metals deposited on MgO insulator and CdO semiconductor density functional calculations

We have analyzed spin quenching of first row transition metals deposited on (001) defect‐free and defect‐containing surfaces of MgO insulator and CdO semiconductor by means of density functional calculations and embedded cluster model. Clusters of moderate sizes were embedded in the simulated Coulomb fields that closely approximate the Madelung fields of the host surfaces, and relaxation of ions that surround the defect sites was taken into account. Spin states of metals deposited on the defect free surfaces were maintained as in the isolated metals except for Ti, V, and Co on MgO, and Ti, V, and Cr on CdO. On the defect containing surfaces, spin states were maintained too except for Fe on MgO, and V and Cr on CdO. The metal‐support interactions stabilize the low spin state of the adsorbed metal with respect to the isolated metal, but the effect was not in general enough to quench the spin. Spin polarization effects tend to preserve the spin states of the adsorbed metals relative to those of the isolated metals. Although charge transfer took place from the adsorbed metal to the insulator surface, it took place the other way round from the semiconductor surface to the adsorbed metal. The encountered variations in magnetic properties were attributed to the smaller band gap of the semiconductor, and the behavior of a single metal atom adsorbed on a particular surface was a result of a competition between Hund's rule for the adsorbed metal and the formation of a chemical bond at the interface. © 2010 Wiley Periodicals, Inc. Int J Quantum Chem, 2011     

Electronic structures and properties of eight-coordinate metal-polyarsenic complexes MAs8n- (M = V,Nb, Ta,Cr, Mo,W, Mn,Tc, Re)

The eight-coordinate early transition metal polyarsenic complexes, MAs(8)3- (M = V, Nb, Ta), MAs(8)2- (M = Cr, Mo, W), and MAs8- (M = Mn, Tc, Re), have been studied using density functional theory (DFT). The geometry optimizations of these complexes indicate that in the most stable structures the transition metal atoms are trapped in a crownlike cavity consisting of a zigzag eight-membered ring of As8 cluster. The scalar-relativistic effects and spin-orbit coupling effects on the electronic structures and energy levels were taken into account. The stabilities of gas-phase MAs8n- ions and bonding between the As8 ring and early transition metals are discussed on the basis of population analysis, atomization energies, and decomposition reaction energies. All these complex ions are found to be diamagnetic with notable HOMO-LUMO energy gaps. The vibrational frequencies and infrared absorption intensities of the MAs8n- series are predicted theoretically. Brief theoretical calculations of the similar MoA(8)2- pnictide ions indicate that the analogous P, Sb, and even Bi complexes are likely to be stable, whereas the crownlike MoN(8)2- is not a stable complex.     

Influence of d orbital occupation on the binding of metal ions to adenine

Threshold collision-induced dissociation of M(+)(adenine) with xenon is studied using guided ion beam mass spectrometry. M(+) includes all 10 first-row transition metal ions: Sc(+), Ti(+), V(+), Cr(+), Mn(+), Fe(+), Co(+), Ni(+), Cu(+), and Zn(+). For the systems involving the late metal ions, Cr(+) through Cu(+), the primary product corresponds to endothermic loss of the intact adenine molecule, whereas for Zn(+), this process occurs but to form Zn + adenine(+). For the complexes to the early metal ions, Sc(+), Ti(+), and V(+), intact ligand loss competes with endothermic elimination of purine and of HCN to form MNH(+) and M(+)(C(4)H(4)N(4)), respectively, as the primary ionic products. For Sc(+), loss of ammonia is also a prominent process at low energies. Several minor channels corresponding to formation of M(+)(C(x)H(x)N(x)), x = 1-3, are also observed for these three systems at elevated energies. The energy-dependent collision-induced dissociation cross sections for M(+)(adenine), where M(+) = V(+) through Zn(+), are modeled to yield thresholds that are directly related to 0 and 298 K bond dissociation energies for M(+)-adenine after accounting for the effects of multiple ion-molecule collisions, kinetic and internal energy distributions of the reactants, and dissociation lifetimes. The measured bond energies are compared to those previously studied for simple nitrogen donor ligands, NH(3) and pyrimidine, and to results for alkali metal cations bound to adenine. Trends in these results and theoretical calculations on Cu(+)(adenine) suggest distinct differences in the binding site propensities of adenine to the alkali vs transition metal ions, a consequence of s-dsigma hybridization on the latter.     

Emission of secondary ions from 3d, 4d, and 5d transition metals under chloro-trifluoro-methane CClF3 as reactant gas

Surface interactions of CClF₃ with polycrystalline samples of Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Nb, Mo, Rh, Pd, Ag, Ta, W, Re, Ir, and Pt were investigated by means of moderate dynamic SIMS. As observed with other reactant gases these transition metals in most cases appear to be discernible into “dissociative” and (partial) “molecular” adsorbents. Small signals of oxidic secondary ions which are detectable for residual gas conditions vanished under the action of CClF₃. However, due to strong polarization by either of the halogens, the emission of Me²⁺ ions is enhanced for Ti, V, and Nb.     

Electronic and geometric structure of the 3d-transition metal monocarbonyls MCO, M=Sc, Ti, V, and Cr

The electronic and geometric structure of the 3d-transition metal monocarbonyls MCO, M=Sc, Ti, V, and Cr was investigated through coupled cluster (CC) and multireference variational methods (MRCI) combined with large basis sets. For the ground and a few low-lying excited states complete potential energy profiles were constructed at the CC-level of theory. The M-CO dissociation energies of the ground states X 4Sigma-,X 5Delta,X 6Sigma+, and X 7A' are calculated to be 36, 27, 18, and 2 kcal/mol for ScCO, TiCO, VCO, and CrCO, with respect to Sc(4F),Ti(5F),V(6D),Cr(7S)+CO(X 1Sigma+). The bonding is rather complicated and could be attributed mainly to pi-conjugation effects between the M and CO pi-electrons, along with weak sigma-charge transfer from CO to M atoms. Almost in all cases the metal atoms appear to be slightly positively charged, at least according to the direction of the dipole moment vectors and the MRCI population densities.