1-亚甲基苯并咪唑-1,4,7-三氮环壬烷配体及其铜配合物[Cu(C14H21N5)Br]2•[CuBr4]的合成与晶体结构

采用新的方法合成了1-亚甲基苯并咪唑-1,4,7-三氮环壬烷配体, 利用该配体合成了一个新的铜配合物[Cu(C₁₄H₂₁N₅)Br]₂•[CuBr₄] ([Cu(C₁₄H₂₁N₅)Br]^＋•[CuBr₄]^2－•[Cu(C₁₄H₂₁N₅)Br]^＋), 并测定了它的晶体结构, 结果表明: 该配合物的晶体属于单斜晶系的C2/c空间群, 晶胞参数a＝1.96209(15) nm, b＝0.82319(5) nm, c＝2.39249(15) nm, α＝90.00°, β＝102.996(2)°, γ＝90.00°, V＝3.7653(4) nm³, Z＝4, μ(Mo Kα)＝8.083 mm^－1, D_c＝2.097 Mg/m³, F(000)＝2308, R＝0.0417, wR＝0.0945, GOF＝0.933. 该配合物由两个1-亚甲基苯并咪唑-1,4,7-三氮环壬烷一溴合铜配阳离子和一个四溴合铜配阴离子组成. 在两个配阳离子中, 每个Cu(II)离子与五个配位原子配位(四个氮原子和一个溴阴离子), 位于一个变形四方锥的中心. 在配阴离子中, Cu(II)离子与四个溴阴离子配位, 位于一个稍变形四面体的中心.     

N-皮考林酰肼及其双核钯配合物的晶体结构和荧光性质

合成了配体N-皮考林酰肼(简写为Hphz)及其双核钯配合物[Pd₂(phz)₂Cl₂]. X射线衍射实验结果表明, 配体和配合物晶体均属于单斜晶系, 空间群分别为C 2/c和P 2₁/c, 分子式分别为C₆H₇N₃O和C₁₂H₁₂Cl₂N₆O₂Pd₂. 晶体学参数, Hphz, a＝1.9245(2) nm, b＝0.38927(2) nm, c＝1.8073(2) nm, b＝107.255(2)°, V＝1.2931(2) nm³, Z＝8, D_c＝1.409 Mg/m³, F(000)＝576, μ(Mo Kα)＝0.102 mm^－1, R＝0.0541, wR＝0.1762; [Pd₂(phz)₂Cl₂], a＝1.48274(9) nm, b＝1.44797(9) nm, c＝0.73951(5) nm, b＝92.719(3)°, V＝1.5860(2) nm³, Z＝4, D_c＝2.329 Mg/m³, F(000)＝1072, μ(Mo Kα)＝2.62 mm^－1, R＝0.0262, wR＝0.0555. 在配合物[Pd₂(phz)₂Cl₂]分子内, 两个钯(II)原子, 均呈畸变的N₃Cl平面正方形配位构型, 晶体内通过分子间氢键N—H…Cl 作用形成一维链状结构, 分子间吡啶环存在相互作用. 量子化学从头算方法计算结果表明, 分子内及分子间的金属钯之间也存在相互作用. 红外光谱表明, 配体在形成配合物后, ν(C＝O)和ν(C＝N)红移, ν(C—N)蓝移, 荧光光谱表明, 配合物金属对配体n-π*激发(310 nm)引起的发射峰有较大的影响.     

Eu(C10H9N2O4)(C10H8N2O4)(H2O)3]•0.5bipy•3H2O配合物的合成、晶体结构及荧光性质

在水-乙醇混合体系中, 以2-羰基丙酸水杨酰腙(C₁₀H₁₀N₂O₄)、2,2-联吡啶(C₁₀H₈N₂, 简写bipy)与Eu(NO₃)₃•4H₂O反应, 首次培养出黄色单晶[Eu(C₁₀H₉N₂O₄)(C₁₀H₈N₂O₄)(H₂O)₃]•0.5bipy•3H₂O. 该晶体属三斜晶系, 空间群为P-1, 晶胞参数a＝0.93392(16) nm, b＝1.3100(2) nm, c＝1.3895(2) nm, α＝97.205(3)°, β＝105.411(2)°, γ＝106.364(2)°, V＝15.35(2) nm³, Z＝2, μ＝2.118 mm^－1, D_c＝1.686 Mg/m³, F(000)＝786, R＝0.0116, wR＝0.0507, GOF＝0.995. 晶体测试结果表明, 该单晶结构为铕的9配位配合物, 两个2-羰基丙酸水杨酰腙分别以负一价和负二价酮式和三个水分子同时参与配位; 每个2-羰基丙酸水杨酰腙中的羧基氧、酰胺基中的羰基氧和C＝N中的氮与Eu^3＋配位, 形成两个共边的稳定五元环, 另三个配位原子则分别来自三个水分子中的氧原子, 该配合物在空间呈扭曲的单帽四方反棱柱, 而在不对称单位中还有游离的一个2,2-联吡啶分子和三个水分子, 这些游离分子与配位分子之间存在大量分子内和分子间氢键, 整个分子在空间呈三维网状结构. 发光性能测试表明该配合物具有很好的荧光性质.     

基态N2O－的势能函数研究

以6-311＋＋G(3df, 3pd)为基函数, 采用密度泛函理论的B3LYP方法对N₂O^－分子体系的结构进行了优化计算. 结果表明N₂O^－分子最稳态为C_s构型, 电子组态为²A', 平衡核间距R_N—N＝0.11873 nm, R_N—O＝0.13012 nm, 键角∠NNO＝133.94448°, 离解能D_e＝10.3857 eV, 基态简正振动频率: 弯曲振动频率ν₁＝656.7488 cm^－1, 对称伸缩振动频率ν₂＝998.1562 cm^－1, 反对称伸缩振动频率ν₃＝1684.3093 cm^－1. 并用多体展式理论方法推导出了基态N₂O^－分子的分析势能函数, 其等值势能图准确地再现了N₂O^－分子的结构特征和离解能.     

[1-芳基甲羰基-2-(1,2,4-三唑-1-基)]乙基-N,N-二烷基二硫代氨基甲酸酯衍生物的合成、结构表征及生物活性研究

以芳香基三唑类杀菌剂三唑酮为先导物设计并合成了5个含N,N-二烷基二硫代氨基甲酸酯的芳香三唑类化合物, 通过元素分析、红外光谱、核磁共振氢谱和质谱对其结构进行了表征. 用X射线单晶衍射测定了[α-(4-甲氧基苯甲酰基)-2-(1,2,4-三唑-1-基)]乙基-N,N-二甲基二硫代氨基甲酸酯的晶体结构, 晶体属于三斜晶系, 空间群, 晶胞参数为: a＝0.73482(15) nm, b＝1.1051(2) nm, c＝1.1209(2) nm, α＝90.32(3)°, β＝101.97(3)°, γ＝105.13(3)°, V＝0.8578(3) nm³, Z＝2, D_c＝1.357 g/cm³, F(000)＝368, µ＝0.324 mm^－1. 生物测试结果显示这5种有机化合物都具有杀菌性和植物生长调节活性     

配合物[Ni(EDTB)]•2Cl•CH3OH•C2H5OH的合成、晶体结构及SOD模拟活性的研究

报道六齿配体N,N,N',N'-四(2-苯并咪唑亚甲基)-1,2-乙二胺(EDTB)及单核镍(II)配合物[Ni(EDTB)]•2Cl• CH₃OH•C₂H₅OH的合成、晶体结构和SOD模拟活性. 该配合物为三斜晶系, P1空间群, a＝1.0931(2) nm, b＝1.1693(2) nm, c＝1.6756(4) nm, α＝76.042(3)°, β＝88.787(3)°, γ＝72.044(3)°, V＝1.9740(7) nm³, D_c＝1.321 g/cm³, Z＝2, F(000)＝824, μ＝0.670 mm^－1. 最终因子R[I＞2σ(I)]: R₁＝0.0611, wR₂＝0.1497; R(全部数据): R₁＝0.0870, wR₂＝0.1604. 结构分析表明, 镍(II)分别与配体中的四个苯并咪唑氮和两个亚胺基氮配位形成扭曲的八面体构型. 改良的邻苯三酚自氧化活性测定表明, 该配合物具有较高的SOD模拟活性.     

三维异核Mn-Na配合物[MnNa(N3)4(C5H5N)4]的合成与表征

Azide-containing coordination polymers have received considerable attention for the construction of new molecule-based magnets. A three dimensional heteronuclear Mn-Na compound [MnNa(N₃)₄(C₅H₅N)₄] was obtained by reaction of [Mn₃O(O₂CCH₃)₆(py)₃]ClO₄ and NaN₃ in pyridine solvents. The title compound crystallizes in monoclinic space group C2/c, a=1.536 6(2), b=1.045 3(2), c=1.576 3(2) nm, β=90.309(3)°, V=2.531 8(6) nm³, Z=4. In the structure, each Mn³⁺ and Na⁺ ion coordinated with four N atoms from four N₃^- and two N atoms from two pyridine molecules. Each pair of Mn³⁺ and Na⁺ ion are linked by N₃^- bridges into a 3D polymer with PtS topology. CCDC: 706250.     

2,4,4'-三羟基脱氧安息香-3'-磺酸钴的合成、晶体结构表征及性质研究

合成了未见文献报道的水溶性很好的2,4,4'-三羟基脱氧安息香-3'-磺酸钴, 采用IR, UV, ¹H NMR和元素分析对其进行了表征, 并利用X射线单晶衍射仪测定了该化合物的晶体结构. 使用荧光光谱法检测了化合物对羟基自由基的清除作用, 紫外光谱法检测其对超氧自由基的清除作用. 实验结果表明, 2,4,4'-三羟基脱氧安息香-3'-磺酸钴[C₂₈H₄₆CoO₂₆S₂]属于单斜晶系, 空间群C2/c, a＝3.3937(3) nm, b＝0.85180(7) nm, c＝1.37455(11) nm, α＝90°, β＝97.8200(10)°, γ＝90°, Z＝4, V＝3.9365(5) nm³, D_c＝1.555 g/cm³, F(000)＝1924, R₁＝0.0329, wR₂＝0.0852, 具有较好的清除羟基自由基和超氧自由基的作用.     

稀土配合物[Pr(C3H7NO2)2(C3H4N2)(H2O)](ClO4)3的标准生成焓及热分解动力学研究

合成了高氯酸镨和咪唑(C₃H₄N₂), DL-α-丙氨酸(C₃H₇NO₂)混配配合物晶体. 经傅立叶变换红外光谱、化学分析和元素分析确定其组成为[Pr(C₃H₇NO₂)₂(C₃H₄N₂)(H₂O)](ClO₄)₃. 使用具有恒温环境的溶解-反应量热计, 以2.0 mol•L^－1 HCl为量热溶剂, 在T＝(298.150±0.001) K时测定出化学反应PrCl₃•6H₂O(s)＋2C₃H₇NO₂(s)＋C₃H₄N₂(s)＋3NaClO₄(s)＝[Pr(C₃H₇NO₂)₂(C₃H₄N₂)(H₂O)](ClO₄)₃(s)＋3NaCl(s)＋5H₂O(1)的标准摩尔反应焓为Δ_rH_m^ө＝(39.26±0.11) kJ•mol^－1. 根据盖斯定律, 计算出配合物的标准摩尔生成焓为Δ_fH_m^ө{[Pr(C₃H₇NO₂)₂(C₃H₄N₂)(H₂O)](ClO₄)₃(s), 298.150 K}＝(－2424.2±3.3) kJ•mol^－1. 采用TG-DTG技术研究了配合物在流动高纯氮气(99.99%)气氛中的非等温热分解动力学, 运用微分法(Achar-Brindley-sharp和Kissinger法)和积分法(Satava-Sestak和Coats-Redfern法)对非等温动力学数据进行分析, 求得分解反应的表观活化能E＝108.9 kJ•mol^－1, 动力学方程式为dα/dt＝2(5.90×10⁸/3)(1－α)[－ln(1－α)]^－1exp(－108.9×10³/RT).     

β-环糊精与水杨酸包合物的合成与结构

合成了β-环糊精与水杨酸的包合物b-cyclodextrin-salicylic acid (β-CD-sal) [(C₄₂H₇₀O₃₅)₂•(C₇H₆O₃)₂•(H₂O)₂₄], 用X射线单晶衍射、元素分析和核磁共振对其分子结构进行了表征. X射线单晶衍射结果表明: 包合物的晶体属于单斜晶系, 空间群为C₂, a＝1.9269(5) nm, b＝2.4395(7) nm, c＝1.6095(4) nm, β＝107.816(5)°, V＝7.203(3) nm³, Z＝4, D_c＝1.373 g•cm^－3, F(000)＝3176, R[I＞2σ(I)]＝0.0971. 在形成的2∶2包合物中, β-环糊精通过羟基间的氢键形成头对头的二聚体, 两个水杨酸分子以不同的形式与环糊精形成包合物, 其中一个水杨酸分子寄居于环糊精的空腔中, 而另一个水杨酸则位于由两个环糊精形成二聚体的空隙中.     

Cluster-assistant generation of multiply charged atomic ions in nanosecond laser ionization of seeded methyl iodide beam

The photoionization of methyl iodide beam seeded in argon and helium is studied by time-of-flight mass spectrometry using a 25 ns, 532 nm Nd-YAG laser with intensities in the range of 2 × 10¹⁰–2 × 10¹¹ W/cm². Multiply charged ions of I^q+ (q = 2–3) and C²⁺ with tens of eV kinetic energies have been observed when laser interacts with the middle part of the pulsed molecular beam, whose peak profiles are independent on the laser polarization directions. Strong evidences show that these ions are coming from the Coulomb explosion of multiply charged CH₃I clusters, and laser induced inverse bremsstrahlung absorption of caged electrons plays a key role in the formation of multiply charged ions.     

Measurement of collision-induced dissociation rates for tantalum oxide ions in a quadrupole ion trap

A study of factors influencing the collision-induced dissociation (CID) rate of strongly bound diatomic ions effected via resonance excitation in a quadrupole ion trap is presented. From these studies, an approach to measuring the CID rates is described wherein product ion recovery is optimized and the effect of competitive processes (e.g., parent ion ejection and product ion reactions) on rate measurements are prevented from influencing rate measurements. Tantalum oxide ions (dissociation ENERGY = 8.2 eV), used as a model system, were formed via reactions of glow discharge generated Ta⁺ ions with residual gases in the ion trap. Neon (0.5 mtorr) was found to be a more favorable target gas for the dissociation of TaO⁺ than He and Ar, but collisional activation of TaO⁺ ions in neon during ion isolation by mass selective instability necessitated ion cooling prior to dissociation. A 25 ms delay time at q_z = 0.2 allowed for kinetic cooling of stored TaO⁺ ions and enabled precise dissociation rate measurements to be made. CID of TaO⁺ was determined to be most efficient at q_z = 0.67 (226 kHz for m/z 197). Suitable resonance excitation voltages and times ranged from 0.56 to 1.2 V_p-p and 1 to 68 ms, respectively. Under these conditions, measurement of rates approaching 80 s⁻¹ for the dissociation of TaO⁺ could be made without significant complications associated with competing processes, such as ion ejection.     

On the extremum property of electron density functions in position and momentum spaces

For statistically uncorrelated wave functions, the electron density ρ(r) is known to be an extremum function of the generalized electron-pair density g(q;a,b), which smoothly connects ρ(r), the electron-pair intracule (relative motion) density h(u), and the electron-pair extracule (center-of-mass motion) density d(R). The present systematic examination of the numerical Hartree–Fock results of moments rⁿ, uⁿ, Rⁿ and density values at the origin ρ(0), h(0), d(0) for 102 neutral atoms and 96 singly charged ions suggests that ρ(r) is local maximum for a small q and is local minimum for a large q of the function g(q;a,b). Analogous results are obtained for the momentum-space counterparts Π(p) and .     

激光解吸电离飞行时间质谱下的银簇行为

近年来,对金属簇的研究已成为化学与物理学中最活跃的研究领域之一［１］．金属簇被认为是介于单个原子与固体之间的中间相［２］．深入地研究其结构、形成机理及物理与化学行为,对于寻找新的催化剂［３］,重新认识气相化学与凝聚相化学的关系［４］,都有非常重要的意...     

Rates of the reactions CN + H2CO and NCO + H2CO in the temperature range 294–769 K

The rate coefficients of the reactions: (1) CN + H₂CO → products and (2) NCO + H₂CO → products in the temperature range 294–769 K have been determined by means of the laser photolysis-laser induced fluorescence technique. Our measurements show that reaction (1) is rapid: k₁(294 K) = (1.64 ± 0.25) x 10⁻¹¹ cm³ molecule⁻¹ s⁻¹; the Arrhenius relation was determined as k₁ = (6.7 ± 1.0) x 10⁻¹¹ exp[(−412 ± 20)/T] cm³ molecule⁻¹ s⁻¹. Reaction (2) is approximately a tenth as rapid as reaction (1) and the temperature dependence of k₂ does not conform to the Arrhenius form: k₂ = 4.62 x 10⁻¹⁷T^1.71 exp(198/T) cm³ molecule⁻¹ s⁻¹. Our values are in reasonable agreement with the only reported measurement of k₁; the rate coefficients for reaction (2) have not been previously reported.     

Determination of calcium, iron and zinc in milk powder by reaction cell inductively coupled plasma mass spectrometry

An inductively coupled plasma mass spectrometer (ICP-MS) equipped with a dynamic reaction cell™ (DRC) was used for the determination of Ca, Fe and Zn in milk powder samples. The effect of the operating conditions of the DRC system was studied to get the best signal-to-noise (S/N) ratio. The potentially interfering ⁴⁰Ar⁺, ⁴⁰Ar¹⁶O⁺, ⁴⁰Ca¹⁶O⁺, ⁴⁸Ca¹⁶O⁺ and ³²S¹⁶O¹⁶O⁺ at the masses m/z 40, 56 and 64 were reduced in intensity significantly by using CH₄ as the reaction cell gas in the DRC while a q-value of 0.7 was used. The limits of detection for ⁴⁰Ca, ⁵⁶Fe and ⁶⁴Zn estimated from the external calibration graphs were 1, 0.01 and 0.001 ng ml⁻¹, respectively, which correspond to 1000, 10 and 1 ng g⁻¹ in the original powder sample. This method was applied to the determination of Ca, Fe and Zn in NIST SRM 1549 non-fat milk powder and two milk powder samples purchased locally. The results for the reference sample agreed satisfactorily with the reference values; the accuracy of the determination was better than 3.8, 18 and 2.2% for Ca, Fe and Zn, respectively. The results for which no reference value was available were also found to be in good agreement between different isotopes. Precision (R.S.D.) between sample replicates was better than 10% for all the determinations.     

乙烯自由基A2A''(v'=0)←X2A'(v''=0)带的转动分析

通过193 nm光解丁烯酮分子产生乙烯基自由基(C₂H₃). 经射流冷却后, 用另一束激光光解C₂H₃, 生成的氢原子碎片经共振增强多光子电离(REMPI)过程, 记录氢离子信号随光解波长变化, 得到20020～20070 cm_-1范围内乙烯基激发的转动分辨光谱. 该谱对应于A²A'(v'=0)←X²A'(v'=0)跃迁的转动结构. 结合量子化学理论计算、光谱拟合以及前人的研究结果, 对该段光谱进行了完整的转动识别, 确定了40条转动谱线的位置. 由光谱拟合还得到A²A'(v'= 0 )能级的预解离寿命为3.3 ps, 且不依赖于转动量子数.     

共掺稀土离子对Er~(3+)激活中红外激光晶体光谱性能的影响

Er3+掺杂的晶体能够产生2.7~3.0μm波段中红外激光,在激光医疗、光通讯、环境探测和光电对抗等领域具有重要的应用。基于本课题组近年来开展的Er3+激活中红外激光晶体的相关工作,本文综述了共掺稀土离子对Er3+激活晶体光谱性能的影响:包括敏化离子Cr3+、Yb3+等的敏化作用增强了Er3+的特征吸收峰;退激活离子Pr3+、Ho3+等的退激活效应抑制了自终态瓶颈效应;以及共掺Nd3+所起的敏化和退激活双重作用,并对中红外激光的研究趋势和前景进行了展望。