α-甘氨酸晶体的动态磁手性和磁电效应

利用变温直流磁化率测定,在外加磁场强度为±1T,磁场平行于晶体b轴,发现在301-302Kα-甘氨酸有动态磁手性相变.α-甘氨酸晶体的每个晶胞包含四个分子,属于具有中心对称结构的P21/n群,电荷中心对称,不导电.在晶体中,两层之间的N (3)—H(8)…O(1)和N (3)—H(8)…O(2)氢键,沿b轴相互交叉反向配对排列.在303K,用原子力显微镜可观察到α-甘氨酸晶体表面分子层与层间有规则的交叉螺旋排列.结合中子衍射确定相变机制为,在相变温度及外加磁场H=±1T时,α-甘氨酸中的N (3)—H(8),电子自旋反转为(邙).因为N (3)—H(8)…O(1)和N (3)—H(8)…O(2)两反向氢键的强度和键角不同,由动态磁手性和磁电效应,产生电荷中心不对称,导致304K附近的热电相变.     

D-和L-丙氨酸的磁手性相变

利用变温直流磁化率测定, 在外加磁场强度为1 T, 磁场平行晶体c轴, 发现在温度270 K, D-和L-丙氨酸发生磁手性相变. 结合中子衍射确定磁手性相变机制为, D-和L-丙氨酸中的(N+H)有类金属氢原子特性, 在相变点270 K, 由(N+H)释放的电子自旋有磁手性. 用变温偏振拉曼光谱进一步证明, D-丙氨酸中的(N+H)的电子自旋(↑), 而L-丙氨酸中的电子自旋(↓), 处于高低不同的能态.磁手性相变(宇称和时间反演都破缺)能差为10^-4-10^-5 eV·molecule^-1.     

“宇称-时间不对称”的实验探索: 手性丙氨酸单晶N+H…O氢键的电子自旋翻转相变的不对称拉曼散射

手性丙氨酸单晶的极性N⁺H…O氢键在~270 K的自发对称性破缺, 可用变温拉曼振动光谱在b(cc)b几何条件下在线测定. 由于其对手性的灵敏度, 可以测定D-和L-丙氨酸的N⁺H…O氢键在电子自旋翻转相变时的微小能差. 晶体定向能量的正/负, 在于电子自旋的上/下转向, 取决于原子内在磁场的方向. 变温拉曼振动光谱可以观察到: 在D-和L-丙氨酸单晶之间, 拉曼散射光子的波数位移方向相反, 散射光子的不对称度约为1/3. 由于自旋是轴矢量, 样品必须是单晶, 沿轴向测定. 多晶粉末不能观察到相变. 与次甲基(C_α－H)在260 K的自旋翻转相变, 用变温拉曼振动光谱在c(aa)c 几何条件下的相对测量结果接近一致. 本实验提供了一条证明真实手性和“宇称-时间(PT)不对称”的新线索.     

X衍射精细结构和晶体旋光角研究D-,L-,DL-缬氨酸晶格分子间N~+H…O~-氢键电子库珀对的自旋流超导相变(英文)

为了解决D-和L-缬氨酸单晶在～270 K相变的机理和分岐,以比热法测定单晶、多晶粉末及Sigma多晶产品发现,只有D-和L-缬氨酸单晶发生相变,且为吸热反应,能差0.18 J·mol-1.本文以Mo-Kα(λ=0.071073nm)为光源的X衍射精确测定表明,D-/L-缬氨酸单晶属于单斜空间点群P21,Z=4.在相变温度～270 K,其晶格常数分别为:a=0.96706(5)/0.96737(5)nm,b=0.52680(3)/0.52664(3)nm,c=1.20256(7)/1.20196(6)nm,β=90.724(2)°/90.722(3)°.在晶体结构的单元细胞中,含有两种转动异构体:A(trans)和B(gauche I).温度为293、270、223、173 K的X衍射精细结构数据表明:在～270 K,D-缬氨酸单晶分子内N―H…O氢键中,N―H、H…O的键长及键角∠N―H…O都发生波动起伏而不可测,但N―H…O总键长变化稳定可测.说明没有发生构型相变为L-缬氨酸.根据D-和L-缬氨酸单晶中,NH3→CO2顺时针和逆时针的相反走向及D-,L-和DL-缬氨酸晶体旋光角的测定,在270-290 K可以观察到晶格分子间N+H…O-氢键电子库珀对的自旋流超导相变.     

D-和L-丙氨酸晶体的突现顺磁性: 准一维N+H…O-氢键的自旋-轨道分离

研究了与磁场强度相关的手性丙氨酸晶体的电子轨道运动的磁性质. 根据丙氨酸单晶的两性离子(⁺NH₃-C(CH₃)H-CO₂^-)模型的手性和蛋白质中肽键晶格结构的螺旋性, 当外加磁场为5 T, 磁场方向平行于丙氨酸晶轴(c)的极性N⁺H…O^-氢键, 观察到D-丙氨酸晶格中, 氢原子的电子自旋翻转, 在297.6 K直接突现顺磁性. L-丙氨酸则先发生电子自旋转向, 然后在303.9 K突现顺磁性. 实验发现: 外加强磁场可以分裂手性丙氨酸晶格中氢键的简并顺磁态, 并测出能差. 本文进一步证明了准一维极性N⁺H…O^-氢键在晶格中可以发生自旋-轨道分离, 表现出一维物理的基本特征.     

CH3SH…HOO开壳型氢键复合物的结构及其电子密度拓扑性质

在DFT-B3LYP/6-311++G**水平下求得CH3SH…HOO复合物势能面上的稳定构型. 计算结果表明, 在HOO以其O8—H7作为质子供体与CH3SH分子中的S5原子为质子受体形成的氢键复合物1和2中, O8—H7明显被“拉长”, 且其伸缩振动频率发生显著的红移, 红移值分别为330.1和320.4 cm-1; 在CH3SH分子以其S5—H6作为质子供体与HOO的端基O9原子为质子受体形成的氢键复合物3和4中, 也存在类似的情况, 但S5—H6伸缩振动频率红移不大. 经MP2/6-311++G**水平计算的4种复合物含BSSE校正的相互作用能分别为-20.81, -20.10, -4.46和-4.52 kJ/mol. 自然键轨道理论(NBO)分析表明, 在CH3SH…HOO复合物1和2中, 引起H7—O8键长增加的因素包括两种电荷转移, 即孤对电子n1(S5)→σ*(H7—O8)和孤对电子n2(S5)→σ*(H7—O8), 其中后者为主要作用. 在复合物3和4中也有相似的电荷转移情况, 但轨道间的相互作用要弱一些. AIM理论分析结果表明, 4个复合物中的S5…H7间和O9…H6间都存在键鞍点, 且其Laplacian量▽2ρ(r)都是很小的正值, 说明这种相互作用介于共价键和离子键之间, 偏静电作用为主.     

不同双/多齿配体Co(Ⅱ)配合物的氧合性能

在室温水溶液体系中采用紫外-可见分光光度法和氧电极法对比研究了α-氨基酸(N/O型)、α-氨基醇(N/O型)、羟基多元羧酸(O/O型)和多胺(N/N型)这4类不同双/多齿配体的Co(Ⅱ)配合物的氧合性能及其氧合反应的可逆性.结果表明, O/O型含羟基的羧酸Co(Ⅱ)配合物无氧合性能; N/N型多胺Co(Ⅱ)配合物有强吸氧性, 但氧合反应不可逆; N/O型配体的Co(Ⅱ)配合物的氧合性能差异较大, 其中α-氨基酸Co(Ⅱ)配合物具有明显的可逆氧合性能, 而含1个—OH的α-氨基醇Co(Ⅱ)配合物没有吸氧能力, 含有2个—OH的α-氨基醇Co(Ⅱ)配合物有微弱的吸氧能力但氧合反应不可逆.分析探讨了N/O型配体中—OH和—COOH对Co(Ⅱ)配合物可逆吸氧性能影响的机理, 根据实验结果初步认为α-氨基酸配位结构是Co(Ⅱ)配合物具有可逆吸氧性能的基本配位结构单元.     

比热和直流磁化率证明N+H…O-氢键的电子自旋翻转在D-和L-丙氨酸单晶中的不对称相变

为了解决D-和L-丙氨酸在约270K相变的分岐和机理,对其单晶、多晶粉末及原料利用微分扫描量热仪测定比热.用三线法以蓝宝石作校正,并与手册的D-和L-丙氨酸标准比热值比较.在单晶中,实验观察到吸热相变峰最高处时的温度及热焓为:D-丙氨酸,Tc=272.02K,△H=1.87J·mol-1;L-丙氨酸,Tc=271.85K,△H=1.46J·mol-1;热焓差为0.41J·mol-1.参比晶体D-缬氨酸,Tc=273.59K,△H=1.75J·mol-1;L-缬氨酸,Tc=273.76K,△H=1.57J·mol-1;热焓差为0.18J·mol-1.实验发现已测量过的单晶磨成多晶粉末后再测,相变峰消失.说明相变与晶格有关.变温中子衍射排除了D→L的构型相变,但发现N+H…O-氢键沿D-和L-丙氨酸单晶的c轴反向变化.变温偏振拉曼散射反映相变机制与N+H…O-中电子的轨道磁偶极矩相关,观察到偏振光的不对称散射.在外加磁场强度H为+1T和-1T下,变温测定D-和L-丙氨酸晶体的直流磁化率,证明在270K有电子自旋翻转的相变.电子自旋的向上或向下,取决于晶格中NH+3的扭曲振动及N+H…O-氢键沿晶体c轴的方向.由于自旋的定轴性,可以解释单晶和多晶粉末比热结果的分岐.     

2-(甲苯-4-磺酰胺基)-苯甲酸的晶体结构、光谱及热性质

报道了2-(甲苯-4-磺酰胺基)-苯甲酸(I)的元素分析和红外、核磁共振光谱性质并通过单晶X射线衍射确定了其晶体结构. 晶体属单斜晶系, 空间群为C2/c,晶胞参数为, a=2.7320(3) nm, b=0.85441(8) nm, c=1.17607(11) nm, α=90°, β=98.728(3)°, γ=90°, V=2.7135(5) nm3, Z=8. 晶体中分子单体通过N—H…O 和O—H…O氢键作用形成具有中心对称的二聚体, 且进一步通过两种不同的C—H…O 氢键和π…π作用形成超分子结构. 在不同的溶剂中, 化合物I的紫外吸收表现出明显的溶剂效应, 此外, 荧光光谱与DSC-TGA热重分析表明, 该化合物是一种耐热的荧光材料.     

高压下晶体5-硝胺基-3,4-二硝基吡唑肼结构转变的周期性密度泛函理论研究

采用周期性密度泛函理论(DFT)方法研究了静水压0~160 GPa范围内5-硝胺基-3,4-二硝基吡唑肼(HNDP)的晶体结构、分子结构和电子结构.研究结果表明,晶体HNDP在静水压6,28和110 GPa时发生了3次结构转变:在6 GPa时,分子中阴离子和阳离子的相对位置发生重排,N17—H23…N13氢键断裂;在28GPa时再次形成N17—H23…N13氢键;在110 GPa时,N17—H19共价键转变为氢键,形成N20—H22…O24共价键.带隙、键布居数以及原子电荷研究结果表明,随着压强增加,晶体HNDP的金属性及离域性增强.     

Dynamical Spin Chirality and Magnetoelectric Effect of α-Glycine

Dynamical spin chirality of α-glycine crystal at 301−302 K was investigated by DC (direct current)-magnetic susceptibility measurement at temperatures ranging from 2 to 315 K under the external magnetic fields (H=±1 T) parallel to the b axis. The α-glycine crystallizes in space group P2₁/n with four molecules in a cell, which has centrosymmetric charge distribution. The bifurcated hydrogen bonds N⁺(3)−H(8)···O(1) and N⁺(3)−H(8)···O(2) are stacked along the b axis with different bond intensities and angles, which form anti-parallel double layers. Atomic force spectroscopy result at 303 K indicated that the surface molecular structures of α-glycine formed a regular flexuous framework in the b axis direction. The strong temperature dependence is related to the reorientation of NH³⁺ group and the electron spin flip-flop of (N⁺H) mode. Under the opposite external magnetic field of 1 T and −1 T, the electron spins of N⁺(3)−H(8)···O(1) and N⁺(3)−H(8)···O(2) flip-flop at 301−302 K. These results suggested a mechanism of the magnetoelectric effect based on the dynamical spin chirality of (N⁺H), which induced the electric polarization to produce the onset of pyroelectricity of α-glycine around 304 K.     

Estimation of Critical Temperature of Thermal Explosion for Energetic Materials Based on Non-isothermal Kinetic Equation dα/dt =A_0 exp(bT)[1+(T–T_0 )b]f(α)

Critical temperature(T b ) of thermal explosion for energetic materials is estimated from Semenov’s thermal explosion theory and the non-isothermal kinetic equation dα/dt=A 0 exp(bT)[1+(T–T 0 )b]f(α) deduced via reasonable hypotheses, where T 0 is the initial point of the deviation from the baseline of DSC curve. The final formula is (T b –T e0 ){1+1/[1+( T b –T 00 )b]}=1. We can easily obtain the initial temperature(T 0i ) and onset temperature(T ei ) from the non-isothermal DSC curves, the values of T 00 and T e0 from the equation T 0i or ei =T 00 or e0 +α 1 β i +α 2 β i2 +…+α L–2 β iL –2 , i=1,2,…,L, the value of b from the equation: ln[β i /(T ei –T 0i )]=ln[A 0 /G(α)]+bT ei , so as to calculate the value of T b . The result obtained with this method coincides completely with the value of T b obtained by Hu-Yang-Liang-Wu method.     

细胞毒活性二萜Wangzaozin A的晶体结构

采用单晶X射线衍射技术对对映-贝壳杉烷化合物WangzaozinA的晶体结构进行了研究.研究结果表明,在最小不对称单元中存在两个构象稍有差异(键长和键角不同)的分子,其中两者的3个六元环均为椅式构象,而五元环为扭曲信封式构象.WangzaozinA晶体结构属正交晶系,P2₁2₁2₁空间群,晶胞参数a=0.66485(8)nm,b=2.5796(4)nm,c=1.0473(2)nm,Z=4.分子通过分子内氢键O₃-H₃0…O₂和O₃'-H₃0'…O₂'以及分子间氢键O1-H10…O₃,O1'-H10'…O₃',O₂-H₂0…O₄'和O₂'-H₂0'…O₄形成网络结构,并在晶体中沿c轴排列.体外抗肿瘤实验证实,标题化合物具有显著的细胞毒活性,由SRB法测试其抗Bel-7402及HO^-8910细胞株的IC₅₀值分别为(5.32±0.79)和(4.10±1.00)μmol/L.     

过氧钒配合物的合成、结构及模拟过氧化酶催化溴化动力学

根据模拟钒卤代过氧化物酶(V-HPOs)活性中心的配位环境,设计并合成了2种新型过氧钒配合物：Na[VO(O2)2(C10H8N2)]·8H2O(1)和K3H[(VO)2(O2)4(μ2-O)]·H2O(2),通过元素分析、红外光谱和紫外光谱对其进行了表征,并通过X射线单晶衍射方法确定了其结构。 配合物1晶体属于三斜晶系,空间群：P-1,a=0.7213(2) nm,b=1.1269(4) nm,c=1.3728(4) nm,α=68.349(4)°,β=89.178(4)°,γ=88.050(4)°,V=1.0365(6) nm3。 配合物2的晶体属于单斜晶系,空间群：P21/c,a=0.67047(12) nm,b=0.99503(18) nm,c=1.5817(3) nm,α=γ=90°,β=93.739(2)°,V=1.0530(3) nm3。 配合物1和2分别是五角双锥和八面体配位构型。 通过催化溴化反应活性研究发现,2种配合物均可作为潜在的钒卤代过氧化物酶模拟物。     

Synthesis, structural characterization and properties of a 3D infinitely extended structural rare earth coordination compound of K3{[Sm(H2O)7]2Na[α-SiW11O39Sm(H2O)4]2}·14 H2O

A 3D infinitely extended structural rare earth coordination compound with a formula of K3{[Sm(H2O)7]2Na[α-SiW11O39Sm(H2O)4]2}·14H2O has been synthesized by reaction of Sm2O3, HClO4, NaOH with α-K8SiW11O39·nH2O, and characterized by IR,UV spectra, ICP, TG-DTA, cyclic voltammetry, variable-temperature magnetic susceptibility and X-ray single-crystal diffraction.X-ray single-crystal diffraction indicates that the title compound crystallizes in a triclinic lattice, Pī space group, with a=1.2462(3) nm, b=1.2652(3) nm,c=1.8420(4) nm,α=87.45(3)°,β=79.91(3)°,γ=82.57(3)°,Z=1, R1=0.0778,wR2=0.1610.Structural analysis reveals that Sm3+(1) coordination cation has incorporated into the vacant site of [α-SiW11O39]8- entity,forming the [α-SiW11O39Sm(H2O)4]5- subunit.The two adjacent [α-SiW11O39Sm(H2O)4]5- subunits are combined with each other through two Sm(1)-O-W bridges accompanying the formation of dimmer structural unit [α-SiW11O39Sm(H2O)4]210- of the title compound.The neighboring dimmer structural units [α-SiW11O39Sm(H2O)4]210- are linked to form the 1D chainlike structure by means of two Sm3+(2) and a Na+(1) coordination cations.The K+(1) cations connect the 1D packing chains constructing the 2D netlike structure, and adjacent netlike layers are also grafted by K+(2) cations to build the novel 3D infinitely extended structure.The result of TG-DTA curves manifests that the decomposition temperature of the title polyanionic framework is 554℃.The cyclic voltammetry measurements show that the title polyanion has the two-step redox processes in aqueous solution with pH=3.1.Variable temperature magnetic susceptibility indicates the title compound obeys the Cruie-Weiss Law in the higher temperature range from 110 to 300 K, while in the lower temperature range from 2 to 110 K the comparatively strong antiferromagnetism interactions can be observed.     

Metal-biradical chains from a high-spin ligand and bis(hexafluoroacetylacetonato)copper(II)

The synthesis, X-ray crystal structure, and magnetic studies of a rare example of organic/inorganic spin hybrid clusters extended in infinite ladder-type chain [Cu(C5F6HO2)2]7(C35H35N5O4)2 ([Cu(hfac)2]7(pyacbisNN)2, 2) formed by the reaction of a high spin nitronylnitroxide biradical C35H35N5O4 (pyacbisNN, 1) and bis(hexafluroacetylacetonate)copper(II) = Cu(hfac)2 are described. Single-crystal X-ray structure analysis revealed the triclinic P1 space group of 2 with the following parameters: a = 10.6191(4) A, b = 19.6384(7) A, c = 21.941(9) A, alpha = 107.111(7) degrees, beta = 95.107(8) degrees, gamma = 94.208(0) degrees , Z = 2. Each repeating unit in 2 carries a centrosymmetric cyclic six spin and a linear five spin cluster with four different copper coordination environments having octahedral and square planar geometries. These clusters are interconnected to form infinite chains which are running along the crystallographic b axis. The magnetic measurements show nearly paramagnetic behavior with very small variations over a large temperature range. The magnetic properties are thus result of complex competitions of many weak ferro- and antiferromagnetic interactions, which appear as small deviations from quite linear mu(eff) vs T dependence at low temperature. At high temperature (300-14 K), antiferromagnetic behavior dominates a little, while at very low temperature (14-2 K), a small increase of mu(eff) was observed. The magnetic susceptibility data are described by the Curie-Weiss law [chi = C/(T - theta)] with the optimal parameters C = 4.32 +/- 0.01 emuK/mol and theta = - 0.6 +/- 0.3 K, where C is the Curie constant and theta is the Weiss temperature.     

稀土配合物{La［o-C6H4(NO2)(CO2)］3·(DMF)2}2的晶体结构及其荧光性能

合成了一种新的双核倒反中心的稀土镧配合物{La［o-C6H4(NO2)(CO2)］3·(DMF)2}2. 通过元素分析、 核磁共振谱和红外光谱对配合物的组成和结构进行了表征,  用热重分析研究了该配合物的热稳定性,  用X射线单晶衍射法测定了其晶体结构. 镧配合物{La［o-C6H4(NO2)(CO2)］3·(DMF)2}2晶体属三斜晶系, 空间群P1,  晶胞参数a=1.902(2) nm, b=1.245 0(2) nm, c=1.298 7(2) nm, α=64.555(2)°, β=66.348(2)°, γ=71.920(2)°, V=1.569 5(5) nm3, Dc=1.658 Mg/m3, Z=2, μ=1.437 mm-1, F(000)=784. 配合物中有2个La(Ⅲ)被4个邻硝基苯甲酸的羧酸根的负氧离子桥联, 每个La(Ⅲ)的中心离子配位数为9,  配位原子分别来自于7个邻硝基苯甲酸的羧酸根的负氧离子和2个DMF的羰基氧原子. 化合物中的氢键和π…π堆积作用使其成为三维立体结构. 同时发现了标题化合物固体具有光致发光现象, 发光性能测试表明， 配合物具有很好的荧光性质.     

Magnetic Chirality Transitions of D- and L-Alanine

A chiral spin state of (N⁺H) in D- and L-alanine was established by monitoring the temperature dependence of dc-magnetic susceptibility (dc: direct current) under the external magnetic field of 1 T. An intrinsic spin chirality of electrons in the atomic magnetic dipole moment of (N⁺H) was also supported by polarized Raman spectroscopy. Magnetic chirality was associated with a strongly correlated electron system that was related to spin rigidity. Raman vibrational spectra were unrelated to structural chirality but could reflect spin chirality due to the reversal of motion breaking. The spin transition of (N⁺H) occured at 270 K without bond breaking but was assisted by an intermediate hydrogen bond elongation, splitting and reformation with NH₃⁺ torsion. The energy difference of spin chirality transitions between D- and L-alanine was around 10⁻⁴-10⁻⁵ eV·molecule⁻¹.