氨基酸DLH及其稀土镧配合物的高压红外和拉曼光谱研究

测定了DL-2-氨基-4-磺酸基-丁酸 [DLH, DL-Homocysteic acid, (NH+₃)-CH(COOH)-(CH₂)₂-SO-₃] 及其稀土La配合物[La(DLH)₂Cl₃·H₂O=LaL₂]在不同压力下的红外和拉曼光谱。DLH 在50 kbar左右压力以下存在两个压力诱导相转变区,它们分别在17和37 kbar左右,两者均为二级相转变,认为分子间氢键的存在是出现两个压力诱导相转变区的原因。在红外光谱中,SO-₃的对称伸缩振动的压力灵敏度(dν/dp)表现出与其他振动模式不同的变化趋势,它们在低压相区的平均压力灵敏度为0.30 cm-1·(kbar)-1、中压相区为0.32 cm-1·(kbar)-1、高压相区为0.41 cm-1·(kbar)-1,低压相区与高压相区的比值为0.72, 而其他振动模式刚好相反,低压相区与高压相区的比值为4.8。稀土La配合物LaL₂的生成,改变了分子间的氢键,在50 kbar左右压力以下只观察到1个压力诱导相转变区(27 kbar附近)。在红外光谱中,配合物LaL₂中SO-₃的反对称伸缩振动的压力灵敏度(dν/dp)也表现出与其他振动模式不同的变化趋势,它们在低压相区的平均压力灵敏度与高压相区的平均压力灵敏度的比值为0.43, 而其他振动模式的比值为2.5。     

金属钨三键多核金属有机配合物高压拉曼及红外光谱研究

研究了金属钨三键多核金属有机配合物 [Cl(CO) 2 (DPPE)WCC6 H4CCC6 H4NC]2 ReCl(CO) 3(DPPE =bis(diphenylphosphino)ethane,(Ph) 2 PCH2 CH2 P(Ph) 2 )不同压力下的拉曼和红外光谱 (最高压力约 5 0kbar)。配合物在 3 0kbar存在一压力诱导二级相变。金属钨三键伸缩振动ν(WC)压力相关 (dν/dp)在低压相区 ( 0 5 9cm-1·(kbar) -1)与高压相区 ( 0 0 4cm-1·(kbar) -1)差别很大 (约 15倍 )。在高压下 ,从基团Cl(CO) 2 (DPPE)WC中的金属钨W向COπ 轨道的π 反馈明显增强 ,WC的键强度减弱 ,力常数减小和ν(WC)降低 ;此效应与压力缩短WC键 ,增大力常数和增加ν(WC)的效应互相竞争。     

异多核金属三键(W≡C)有机化合物的红外和拉曼光谱研究

五种 (Ⅰ ,Ⅱ ,Ⅲ ,Ⅳ ,Ⅴ )异多核金属钨三键W≡C金属有机化合物的红外和拉曼光谱研究表明 ,由于N和P原子为强的σ 给予体和弱的π 接受体 ,在金属原子上分别引入含N或P的功能基团 (TMEDA或DPPE)将降低金属三键 (W≡C)的键强度 ,W≡C伸缩振动νW≡C 波数下降。化合物Ⅲ的压力调制红外和拉曼光谱显示 ,在 2 0kbar压力附近存在一压力诱导相变。低压相区高的压力灵敏度dv/dp(0 75cm-1·kbar-1)和高压相区很低的压力灵敏度 (0 0 8cm-1·kbar-1)指出 ,对W≡C键存在两种压力效应 ,一种是正常的 ,W≡C键强度随压力增加而增强 ,伸缩振动 νW≡C 波数增加 ;另一种是随着压力增加 ,从W到COπ 轨道反馈增加 ,导致W≡C键强度减弱 ,伸缩振动νW≡C 波数下降。     

二正丁基锡三齿酰腙Schiff碱配合物的合成和红外光谱研究

合成了 4种三齿酰腙Schiff碱配体H2 L [H2 L1 :C6 H5C(O)NHN =CHC6 H4OH 2 ,H2 L2 :C6 H5C(O)NHN =CHC6 H3(OH) 2 2 ,4,H2 L3:NC5H4C(O)NHN =CHC6 H4OH 2 ,H2 L4:NC5H4C(O)NHN =CHC6 H3(OH) 2 2 ,4]和它们的二正丁基锡新型配合物 (n Bu) 2 SnL ,通过元素分析确定了这些配合物的组成 ,并对配合物在 4 0 0 0～ 40 0cm- 1范围内的主要红外光谱吸收峰进行了归属和讨论 ,推测出配合物可能的分子结构。     

金属-糖胺配合物的合成,光谱表征及催化酯类水解的动力学研究

合成了4种新的糖胺 金属配合物,分别为[Ni(HL) (H2 O) 2 ]2 Cl2 ·CH3OH·2H2 O ,[Cu(HL) ]2 Cl2 ·CH3CH2 OH·3H2 O ,[Zn(HL) ]2 Cl2 ·H2 O ,[Co(HL) (H2 O) (OH) ]2 Cl2 ·CH3OH·2H2 O (HLN ,N′ 二βD 葡萄糖基乙二胺) ,并用元素分析、红外、紫外、核磁共振氢谱对其结构进行了表征。结果表明,Ni(Ⅱ) ,Co(Ⅲ)配合物为八面体构型,而Cu(Ⅱ) ,Zn(Ⅱ)配合物为四面体构型。最后研究了其对对硝基苯吡啶甲酸酯(PNPP)催化水解的催化速率常数。     

2-噻吩乙醛酸-邻菲罗啉-铕配合物的合成、结构表征及荧光性能的研究

合成了铕与 2 噻吩乙醛酸 (HL)和邻菲罗啉 (phen)的配合物 ,用元素分析、电导率、红外光谱和核磁共振谱测定了配合物的分子式为 [EuL2 phen·(H2 O) 3 ]NO3 ;配合物中的Eu(Ⅲ )离子与 2 噻吩乙醛酸和水分子中的O原子以及邻菲罗啉中的N原子配位。在室温下测定了配合物的激发和发射光谱 ,配合物中Eu(Ⅲ )离子的5D0 7F1和5D0 7F2 跃迁分别位于 5 92和 6 18nm。该固体配合物于室温下被紫外光激发可以发出强的特征红色荧光。IR光谱中 ,2 噻吩乙醛酸的特征吸收峰νCO (1719cm-1) ,νC—O(12 32cm-1) ,δO—H(90 9cm-1)在形成配合物后消失。在配合物中出现—COO-的反对称νas(16 4 2cm-1)和对称νs(14 0 8cm-1)伸缩振动吸收峰。在1HNMR谱图中 ,2 噻吩乙醛酸环上的 3个氢原子的化学位移形成配合物后移向高场 ,邻菲罗啉环上 4种不同环境的质子峰的化学位移形成配合物后向低场移动。从TG曲线可以看出 ,此配合物在常温至 2 5 0℃以下是稳定的。     

Nd和Sb掺杂SnO2导电粉体的红外光谱研究

本文以 Sn Cl4· 5 H2 O、Sb Cl3 和 Nd2 O3 为原料制备了 Nd和 Sb掺杂 Sn O2 导电粉体 ,用红外光谱法测定了该粉体的光谱。在 730— 6 2 0 cm-1范围 ,有个宽的吸收峰 ,在 4 0 0 0— 2 80 0 cm-1范围有强吸收。     

耐高温型4-卤代(氟、氯)苯甲酸铽配合物的合成及荧光性能研究

以4-氟苯甲酸(4-FBA)、4-氯苯甲酸(4-ClBA)为配体制备了具有良好热稳定性的稀土配合物Tb(4-FBA)3·2H2O和Tb(4-ClBA)3·2H2O,与前期工作中合成的Tb(4-BrBA)3的紫外及荧光光谱进行了分析比较。紫外-可见光吸收光谱表明,相同浓度下,3种配合物的紫外吸收能力以Tb(4-FBA)3·2H2O、Tb(4-ClBA)3·2H2O、Tb(4-BrBA)3顺序依次增大。液体荧光光谱表明,Tb(4-ClBA)3·2H2O的荧光发射强度最强。从配体的能级、配合物的紫外吸收能力及能量传递过程中的热振动损耗等方面对实验结果进行了讨论分析。热重分析表明,Tb(4-FBA)3·2H2O和Tb(4-ClBA)3·2H2O在450℃出现快速分解。将2种配合物放置于马弗炉中350℃加热1 h后,发现Tb(4-FBA)3·2H2O的荧光发射强度降低了24%,Tb(4-ClBA)3·2H2O荧光发射强度仅降低了13%左右,表明2种配合物高温条件下分子结构保持稳定,加热后2种配合物的红外光谱也表明2种配合物在高温条件下未发生分解。     

羧酸类钕(Ⅲ)配合物的合成、热稳定性和荧光性能研究

为了开发稀土有机配合物作为激光工作物质,分别以均苯三甲酸(H3BTC)、苯六甲酸(H6MTA)和1,2,3,4,5,6-环己六甲酸(H6CCA)为配体合成了三种Nd(Ⅲ)的二元发光配合物。通过元素分析、等离子体原子发射光谱和红外光谱对其化学组成进行了结构表征,确定其化学结构依次为Nd(BTC)·4H2O,Nd2(MTA)·6H2O和Nd2(CCA)·4H2O,并对其热稳定性和荧光性能进行了分析测试。三种配合物的发射谱均有三个带状谱带,位于近红外区,其对应于Nd(Ⅲ)离子的特征跃迁4F3/2→4I9/2,4F3/2→4I11/2和4F3/2→4I13/2。结果表明,羧酸类钕(Ⅲ)配合物在近红外区具有明显的特征发射,具有良好的热稳定性和较好的发光性能,可以作为潜在的激光介质。     

光诱导下系列钴配合物的表面电子行为对比研究

通过水热方法合成了6种Co(Ⅱ/Ⅲ)配合物Co(H2O)6·H2btec(1);{[Co2(HCOO)6]·CH3OH}n(2);([Co(4,4'-bipy)2(H2O)4]·suc·4H2O}n(3);Co(NA)2(H2O)4(4);[Co(mal)(4,4'-bipy)H2O]n(5);[Co(HCOO)4Co(H2O)4]n(6)(H4btec=均苯四甲酸,H2suc=丁二酸,HNA=娴酸,H2mal=丙二酸,bipy=联吡啶)},测试了配合物的UV-Vis吸收光游和表面光电压光谱(SPS),并通过X-ray单晶衍射确定了配合物的结构.它们的表面光电压光谱在300～800 nm范围内均表现出正的光伏响应,并将其与UV-Vis吸收光谱进行了分析和对比,发现SPS中表面光伏响应带与UV-Vis吸收光谱的吸收峰具有良好的对应关系.通过对比6种配合物的SPS可以看出,中心金属离子的价态、配位模式及配位微环境均对SPS响应带的位置和形状有一定影响.     

High pressure equation of state of rubidium

The pressure-volume relation of rubidium metal is studied by high-pressure x-ray diffraction up to 110 kbar at room temperature. In addition, pressure scans of the near-infrared reflectivity are recorded up to 250 kbar. Rubidium undergoes a bcc to fcc structural transition (Rb I → Rb II) at 70 ± 2 kbar. Other phase transitions occur at 128 ± 3, 160 ± 5 and 190 ± 5 kbar on the ruby pressure scale. The pressure-volume relation and the near-infrared reflectivity provide evidence for a pressure-induced 5s → 4d electronic transition similar to the well-known 6s → 5d transition in cesium metal.     

High-resolution FTIR study of the para-terphenyl phase transition at high pressure

High-resolution infrared (IR) spectroscopy has been used to investigate the pressure-induced (0-11 kbar) polymorphic phase transition of crystalline para-terphenyl at low temperature (25 K). A number of doublet bands observed in low-pressure triclinic p-terphenyl were observed to coalesce in the high-pressure monoclinic phase. The coalescing of doublet bands was attributed to changes in factor group (Davydov) splittings associated with the transition from a low-pressure triclinic phase to a high-pressure monoclinic phase. The bands that ‘disappear’ also do not correlate with frequency changes associated with changes in molecular symmetry. Molecular dynamics (MD) simulations at low temperature (20 K) yield a non-planar average molecular structure for the high-pressure monoclinic phase, in contrast to the high-temperature monoclinic phase. The MD simulations also reveal a broadening of the distribution of ring torsion angles near the triclinic-monoclinic phase transition pressure.     

Pressure-induced structural transitions in PbI2: A high-pressure Raman and optical absorption study

The effect of pressure on the 2H and 4H polytype of PbI₂ has been investigated by Raman and optical absorption spectroscopy, using the diamond anvil cell. The 2H-polytype undergoes pressure-induced phase transitions at 5 kbar and near 30 kbar. The 4H-polytype exhibits phase transitions near 8 kbar and above 30 kbar. The Raman modes abruptly change at these pressures. The optical absorption edge shifts red at the rate of 15±1 MeV/kbar in the 2H-PbI₂ and at the rate of 7 MeV/kbar in phase II. The latter phase is most likely to possess a 3d-structure and not a layer type. The possible structures for the high pressure phases are discussed.     

Pressure-induced phase transition in LiLuF4:Pr3+ investigated by an optical technique

The luminescence and luminescence kinetics of LiLuF(4) doped with 1.5 at.% of Pr(3+) obtained at high hydrostatic pressure changing from ambient to 220 kbar applied in a diamond anvil cell are presented. It has been shown that pressure causes shift of the emission lines toward the red with rates of the order of single cm(-1) kbar(-1). The pressure-induced phase transition from tetragonal to fergusonite structure for pressure above 100 kbar was observed. The crystal field calculations performed showed that this phase transition reduces the point symmetry of the Pr(3+) site from the S(4) to the C(2) point group.     

Pressure-tuned collapse of the Mott-like state in Ca(n+1)Ru(n)O(3n+1) (n=1,2): Raman spectroscopic studies

We report a Raman scattering study of the pressure-induced collapse of the Mott-like phases of Ca3Ru2O7 (T(N)=56 K) and Ca2RuO4 (T(N)=110 K). The pressure dependence of the phonon and two-magnon excitations in these materials indicate (i) a T approximately 0 pressure-induced collapse of the antiferromagnetic (AF) insulating phase above P(*) approximately 55 kbar in Ca3Ru2O7 and P(*) approximately 5-10 kbar in Ca2RuO4, (ii) a remarkable insensitivity of the exchange interaction to pressure in both systems, and (iii) evidence for persistent AF correlations above the critical pressure of Ca2RuO4, suggestive of phase separation involving AF insulator and ferromagnetic metal phases.     

High-frequency and -field EPR and FDMRS study of the [Fe(H2O)6]2+ ion in ferrous fluorosilicate

The complex [Fe(H2O)6]SiF6 is one of the most stable and best characterized high-spin Fe(II) salts and as such, is a paradigm for the study of this important transition metal ion. We describe high-frequency and -field electron paramagnetic resonance studies of both pure [Fe(H2O)6]SiF6 and [Zn(H2O)6]SiF6 doped with 8% of Fe(II). In addition, frequency domain magnetic resonance spectroscopy was applied to these samples. High signal-to-noise, high resolution spectra were recorded which allowed an accurate determination of spin Hamiltonian parameters for Fe(II) in each of these two, related, environments. For pure [Fe(H2O)6]SiF6, the following parameters were obtained: D=+11.95(1) cm(-1), E=0.658(4) cm(-1), g=[2.099(4),2.151(5),1.997(3)], along with fourth-order zero-field splitting parameters: B4(0)=17(1)×10(-4) cm(-1) and B4(4)=18(4)×10(-4) cm(-1), which are rarely obtainable by any technique. For the doped complex, D=+13.42(1) cm(-1), E=0.05(1) cm(-1), g=[2.25(1),2.22(1),2.23(1)]. These parameters are in good agreement with those obtained using other techniques. Ligand-field theory was used to analyze the electronic absorption data for [Fe(H2O)6]SiF6 and suggests that the ground state is 5A1, which allows successful use of a spin Hamiltonian model. Density functional theory and unrestricted Hartree-Fock calculations were performed which, in the case of latter, reproduced the spin Hamiltonian parameters very well for the doped complex.     

Phase behavior of four homologous compounds of 4-n-alkyl-4′-isothiocyanatobiphenyl (nBT) under pressure

The phase behavior of four homologous compounds of 4-n-nonyl-, 4-n-decyl-, 4-n-undecyl-, and 4-n-dodecyl-4′-isothiocyanatobiphenyl (9BT, 10BT, 11BT, and 12BT) was re-investigated to characterize their high-pressure mesophases under pressures up to 150 MPa using a polarizing optical microscope equipped with a high-pressure optical cell and a wide-angle X-ray diffractometer equipped with a high-pressure sample vessel. The pressure-induced mesophases of 9BT and 10BT appearing under pressures above about 60 and 100 MPa, respectively, were identified as nematic (N) and SmA phases, which indicate the reversible Cr–CrE–N–I and Cr–CrE–SmA–I phase transitions under elevated pressure. 11BT and 12BT exhibited the reversible transition of Cr–CrE–SmA–I in the low-pressure regions below about 5 and 23 MPa, respectively. Both the stable CrE phases changed into the monotropic (and metastable) one under higher pressures, in which the Cr–SmA–I and I–SmA–CrE–Cr phase transitions on heating and cooling processes, respectively, were recognized.     

Phase behavior of four homologous compounds of 4-n-alkyl-4′-isothiocyanatobiphenyl (nBT) under pressure

The phase behavior of four homologous compounds of 4-n-nonyl-, 4-n-decyl-, 4-n-undecyl-, and 4-n-dodecyl-4′-isothiocyanatobiphenyl (9BT, 10BT, 11BT, and 12BT) was reinvestigated to characterize their high-pressure mesophases under pressures up to 150 MPa using a polarizing optical microscope equipped with a high-pressure optical cell and a wide-angle X-ray diffractometer equipped with a high-pressure sample vessel. The pressure-induced mesophases of 9BT and 10BT appearing under pressures above about 60 and 100 MPa, respectively, were identified as nematic (N) and smectic A (SmA) phases, which indicate the reversible Cr–CrE–N–I and Cr–CrE–SmA–I phase transitions under elevated pressure. Both the 11BT and 12BT exhibited the reversible transition of Cr–CrE–SmA–I in the low-pressure regions below about 5 and 23 MPa, respectively. Both the stable CrE phases changed into the monotropic (and metastable) one under higher pressures, which the Cr–SmA–I and I–SmA–CrE–Cr phase transitions on heating and cooling processes were recognized, respectively.