NMR研究溶液中正十四烷基硫酸钠/正十四烷基聚氧乙烯醚(3)表面活性剂之间的相互作用

采用¹HNMR弛豫、自扩散系数和二维相敏(2DNOESY)实验研究了正十四烷基硫酸钠[n-CH₃(CH₂)₁₃OSO₃Na(STS)]和正十四烷基聚氧乙烯醚(3)[n-CH₃(CH₂)₁₃O(C₂H₄O)₃H(C₁₄E₃)]在溶液中的自聚集以及二者混合后的相互作用.结果表明,STS与C₁₄E₃混合后存在相互作用,并形成混合胶束;弛豫实验表明,混合胶束中STS疏水链质子运动更加受阻,C₁₄E₃的α-(4″)和β-CH₂(3″)处链堆积紧密.C₁₄E₃的亲水端(CH₂CH₂0)₃链卷曲紧贴在疏水壳表面外链堆积较紧密处.自扩散系数测量表明,混合胶束比单一阴离子表面活性剂形成的胶束大.单一非离子型胶束和混合胶束的亲水端(CH₂CH₂0)₃(5″)链构成相应较软和松散的外壳.单一C₁₄E₃在极性溶剂氯仿溶液中,质子运动比在水中自由度大,但2DNOESY谱中出现了少量分子间的交叉峰,也可能形成了一些小的聚集体.     

弛豫铁电体结构起伏与弛豫性研究

制备了铅基弛豫铁电体0.9Pb(Mg_1/3Nb_2/3)O₃-0.1PbTiO₃和Pb(Zn_1/3Nb_2/3)O₃基陶瓷. 铅基弛豫铁电体PMNT, PZN基陶瓷弛豫过程可用局域冻结模型描述. 在微畴-宏畴转变过程中, 弛豫铁电体产生结构起伏; 在相同的频率条件下, 弛豫铁电体的结构起伏程度越大, 弛豫程度越低. 在微畴-宏畴转变过程中, 随微畴的增大, 弛豫铁电体的弛豫特性减弱或消失.     

γ-Al2O3催化合成聚甲基膦酸乙二醇酯的适宜活化温度的确定

聚甲基膦酸乙二醇酯(PEMP)作为一种良好的阻燃剂,具有无毒、低烟、含磷量高、阻燃效果好的优点。 γ-Al₂O₃是催化乙二醇(EG)和甲基磷酸二甲酯(DMMP)缩合生成PEMP的良好催化剂。 但是由于γ-Al₂O₃容易吸附CO₂和水分,降低其催化活性,所以使用前需要活化。 活化温度影响着γ-Al₂O₃的催化活性。 本文分别在300、400、500、600、700和800 ℃不同温度下对γ-Al₂O₃进行活化,用X射线粉末衍射(XRD)分析了γ-Al₂O₃晶型变化、用低温氮吸附比表面积测试法(BET法)测量了γ-Al₂O₃比表面积、孔径和孔容积,用傅里叶变换红外光谱(FTIR)分析了红外吸收变化,用吡啶吸附-FTIR测定了γ-Al₂O₃的Brønsted酸位点与Lewis酸位点相对含量。 比较了不同温度下活化的γ-Al₂O₃催化合成PEMP产品的纯度和粘度,找到了γ-Al₂O₃催化合成PEMP的适宜活化温度为400~600 ℃。 此时,γ-Al₂O₃属于典型的γ-Al₂O₃晶型,比表面积较大,孔径较小,所得PEMP产品纯度最高。     

α-氨基酸各官能团对其Co(Ⅱ)配合物可逆氧合性能的影响

选择氧合性能良好的组氨酸(His)-Co(Ⅱ)作为研究对象, 分别掩蔽—NH₂、 取代—O^-和去除—COO^-, 得到短肽、 伪肽和多胺等类组氨酸结构. 采用UV-Vis光谱法研究了α-氨基酸中的3个官能团对其Co(Ⅱ)配合物氧合性能的影响. 对比研究表明: α-氨基酸中—NH₂对其Co(Ⅱ)配合物的吸氧性具有决定作用; —COO^-对其Co(Ⅱ)配合物氧合作用的可逆性起关键作用; 而—O^-对其Co(Ⅱ)配合物的吸氧性影响不大. 在前期研究结果的基础上, 对α-氨基酸-Co(Ⅱ)配合物可逆吸收和释放O₂的机理进行了探讨.     

四核钬配合物的结构、慢磁驰豫行为及CO2催化转化性质

使用多齿希夫碱配体通过溶剂热的方法合成了一例新的Ho4配合物,即[Ho₄(NO₃)₂(acac)₄(L)₂(CH₃OH)₂]·2CH₃CN,其中H4L=(E)-2-(羟甲基)-2-(((2-羟基萘-1-基)亚甲基)氨基)丙烷-1,3-二醇,acac=乙酰丙酮。X射线衍射分析表明,配合物呈中心对称的四核结构,中心的Ho1(Ⅲ)和Ho2(Ⅲ)均为八配位的三角十二面体几何构型。配合物1具有良好的溶剂稳定性。磁性研究表明配合物1具有慢磁弛豫行为。据我们所知,配合物1是一例少有的在零直流场下具有慢磁驰豫行为的Ho₄配合物。值得一提的是,配合物1在催化CO₂与环氧化合物的环加成反应中表现出较高的催化活性。     

基于二茂铁的两个查尔酮衍生物的合成及超快三阶非线性光学响应

二茂铁是合成新颖有机功能材料的基本单元之一。 本文设计并合成了两个基于二茂铁的同分异构查尔酮衍生物:1-二茂铁基-3-(噻吩-2-基)丙烯酮(a)和1-二茂铁基-3-(噻吩-3-基)丙烯酮(b)。 采用超快激光Z-扫描技术(脉宽180 fs,波长532 nm)测定了化合物a和b的三阶非线性光学性质。 结果表明,化合物a吸收系数β=-2.1×10^-12 m/W,折射率n₂=1.9×10^-19 m²/W,分子超极化率γ=5.37×10^-32 esu;化合物b:β=-1.2×10^-13 m/W,n₂=2.0×10^-19 m²/W,γ=4.48×10^-32 esu。 说明在飞秒激光激发下,电荷转移能够在化合物a和b分子内部快速进行,二者均具有优异的超快三阶非线性光学响应。 在B3LYP/6-311+G(d,p)理论水平下,计算了化合物a和b分子轨道能量、极化率和各基团在前线分子轨道中的占有率。 理论计算结果显示,二茂铁基团在化合物a和b前线分子轨道中占有率分别为97%和98%,对两化合物的非线性光学性能起主导作用。     

三嗪-吡唑钌配合物的合成、结构及光催化活性

光催化具有无污染、安全高效等优点,已成为环保领域的研究热点。 本文选择2,4-二(3,5-二甲基吡唑)-6-二乙基胺-1,3,5-三嗪(L₁)和2, 6-二[3-(5-甲基吡唑基)]吡啶(L₂)为配体、以RuCl₃为金属源,合成了3种配合物[Ru(L₁)Cl₃](1)、[Ru(L₂)₂]·Cl₃(2)和[Ru(L₂)₂]·(H₂BTC)·(HBTC)·H₂O(3),同时进行了IR、UV-Vis、TG及X射线衍射等表征,并对配合物在光催化降解罗丹明B方面进行了探讨,结果表明,配合物13均具有一定程度的光降解效果,降解效果分别为46.8%、44.7%和40.4%。 相同条件下,加入H₂O₂后的配合物13的降解效果比金属盐、配体及H₂O₂单独存在时的降解效果好。     

γ-巴豆酰内酯激发态动力学的共振拉曼光谱和完全活性空间自洽场(CASSCF)计算研究

采用共振拉曼光谱和完全活性空间自洽场(CASSCF)方法研究了γ-巴豆酰内酯的光吸收S₂态的结构动力学和衰变机制. 采用含时密度泛函理论方法结合光谱实验确认了紫外光谱和振动光谱. 获得了涵盖A-带吸收的4个激发波长下的共振拉曼光谱. 用CASSCF计算得到了S_1,min, S_2,min, T_1,min, T_2,min和T_3,min及其相关势能面交叉点的结构与能量. 研究了A-带共振拉曼光谱强度模式与S_2,min和CI(S₂/S₁)交叉点结构的关系. 借助El-Sayed规则分析了各系间窜跃路径的效率, 提出了γ-巴豆酰内酯从S_2,FC弛豫到基态S₀的2条主要路径: 内转换路径和系间窜跃路径.     

γ-AlOOH纳米棒的水热合成与形貌调控

γ-AlOOH作为液相法合成γ-Al₂O₃的前驱体,其形貌与最终产物的性能密切相关。 本文采用水热法合成γ-AlOOH纳米棒,通过改变Al³⁺浓度和沉淀剂的种类调控γ-AlOOH纳米棒的长径比,利用X射线衍射仪(XRD)和透射电子显微镜(TEM)表征产物的晶体结构和形貌。 结果表明,随Al³⁺浓度增大可得到长径比在5.9~8.0的γ-AlOOH纳米棒,而改变沉淀剂的种类可进一步将长径比增大到8.0~10.0。 通过对产物结晶过程的分析,发现增大Al³⁺浓度和增强沉淀剂碱性均可以促进铝离子与羟基的配合。 提高反应体系中Al(OH)₃浓度,有利于γ-AlOOH晶粒的成核,促进了晶核之间的定向接触,从而提高了纳米棒的长径比。 长径比为10.0的γ-AlOOH纳米棒烧结所得纳米γ-Al₂O₃改性变压器油(体积分数为0.1%)的正冲击击穿强度较纯油提高9.9%.     

非绝热分子动力学模拟A位阳离子对钙钛矿热载流子弛豫的影响

钙钛矿具有优异的光学和电学性质, 近年来成为太阳能电池领域的研究热点. 大量实验报道钙钛矿热载流子弛豫时间变化顺序为CsPbBr₃>MAPbBr₃(MA=CH₃NH₃)>FAPbBr₃[FA=HC(NH₂)₂], 但A位阳离子(Cs ⁺, MA ⁺, FA ⁺)对弛豫快慢的影响机制仍不明确. 采用基于含时密度泛函理论的非绝热动力学方法研究了上述3种钙钛矿热电子和热空穴的能量弛豫动力学, 计算得到的热载流子弛豫时间与实验结果吻合. 结果表明, A位阳离子通过静电和氢键作用影响其与无机Pb—Br骨架的电子-振动耦合, 使非绝热耦合强度遵从FAPbBr₃>MAPbBr₃>CsPbBr₃的变化趋势, 进而使热载流子弛豫时间尺度变化趋势与之相同, 表明合理选择A位阳离子可以优化钙钛矿太阳能电池的性能.     

Vacancy spectroscopy of radiation cross-linked and degraded polytetrafluoroethylenes

Polytetrafluoroethylene samples having different morphology were prepared by radiation induced cross-linking and degradation, and positron annihilation lifetimes were measured to extract information about the vacancy structure from the orth-positronium (o-Ps) component. The o-Ps intensity I₃ was inversely correlated with the crystallinity confirming that this component is associated with the amorphous part. The o-Ps lifetime τ₃ was distinctly different depending on the phase of the polymer. Below the γ relaxation temperature, the vacancies produced by degradation could be seen from an increase in the τ₃ value, but at temperatures between the γ and β relaxations such vacancies became invisible due to the activated segment motion. And above the β relaxation temperature vacancies in the interface between crystalline and amorphous parts appear to affect τ₃. The o-Ps intensity did not show stable reproducible results. Accumulation of positive charge can be responsible for it. The results, not only unveiling the not yet well understood behavior of the o-Ps component, demonstrate the uniqueness of the vacancy spectroscopy using o-Ps as a probe.     

REACTIVITY OF CHLOROPHYLL a/b-PROTEINS AND MICELLAR TRITON X-100 COMPLEXES OF CHLOROPHYLLS a OR b WITH BOROHYDRIDE

The reaction of several plant chlorophyll-protein complexes with NaBH₄ has been studied by absorption spectroscopy. In all the complexes studied, chlorophyll b is more reactive than Chi a, due to preferential reaction of its formyl substituent at C-7. The complexes also show large variations in reactivity towards NaBH₄ and the order of reactivity is: LHCI > PSII complex > LHCII > PSI > P700 (investigated as a component of PSI). Differential pools of the same type of chlorophyll have been observed in several complexes.
Parallel work was undertaken on the reactivity of micellar complexes of chlorophyll a and of chlorophyll b with NaBH₄ to study the effect of aggregation state on this reactivity. In these complexes, both chlorophyll a and b show large variations in reactivity in the order monomer > oligomer > polymer with chlorophyll b generally being more reactive than chlorophyll a. It is concluded that aggregation decreases the reactivity of chlorophylls towards NaBH₄ in vitro, and may similarly decrease reactivity in naturally-occurring chlorophyll-protein complexes.     

LASER PHOTOLYSIS OF 3-METHYLLUMIFLAVIN

Abstract— Using high-intensity actinic light, the chlorophyll a fluorescence transient from HCO^-₃-depleted chloroplasts shows a rapid initial rise (O → I) followed by a slow phase (I → P). In the presence of HCO^-₃, the O → I rise is delayed but the I → P phase is much more rapid. Using low-intensity actinic light, the chlorophyll a fluorescence transient from 3-(3,4-dichlorophenyl)-1,1 dimethylurea (DCMU)-treated chloroplasts is delayed in the presence of HCO^-₃. Bicarbonate increases the amount of delayed light emission from chloroplasts given 10 s illumination with weak blue light (0·4 W/m²). DCMU greatly increases the amount of delayed light seen in the presence of HCO^-₃ under these conditions but decreases the amount seen in the absence of HCO^-₃. It is suggested that HCO^-₃ may somehow form or stabilize, in the dark, a number of reaction centers corresponding to the S₁ state in the model of B. Forbush, B. Kok and M. McGloin ( Photochem. Photobiol. 14, 307–321, 1971).     

Dielectric spectroscopy of an antiferroelectric liquid crystal showing an antiferroelectric-ferrielectric transition

We report the dielectric relaxation behaviour in the antiferroelectric SmC_A* and ferrielectric SmC_γ* phases of the antiferroelectric liquid crystal 4-[5-(4-octloxyphenyl)-2-pyrimidinyl]phenyl 4,4,4-trifluoro-3-(methoxyphenyl)butanoate which shows an antiferroelectric transition at around 88±0.1°C. In the SmC_A* phase, two dielectric relaxation modes have been found, namely the usual antiferroelectric Goldstone mode and another arising from molecular rotation around its short axis. In the SmC_γ* phase, one dielectric relaxation mode has been observed due to the ferrielectric Goldstone mode. Dielectric increments and relaxation frequencies of the antiferroelectric and ferrielectric phases are estimated from the fits of the Cole-Cole function of the dielectric spectrum. The dependence of the bias field in the ferrielectric phase is also discussed.     

Study of the NaBr–DyBr3 phase diagram by differential thermal analysis

The phase diagram of the quasi binary NaBr–DyBr₃ system was determined by differential thermal analysis (DTA) applied to 27 samples covering the complete composition range of the system. The 3NaBr*DyBr₃(s) compound is present in the solid-phase in addition to the pure component halides NaBr(s) and DyBr₃(s). The DyBr₃(s) and 3NaBr*DyBr₃(s) phases showed a polymorphic transition at 1112 and at 733 K, respectively. The {DyBr₃(s) + 3NaBr*DyBr₃(s)} eutectic mixture melts at 709 K giving a liquid of the molar composition x(NaBr) = 0.62. The 3NaBr*DyBr₃(s) phase melts peritectically at 765 K. The phase diagram obtained in the present study virtually agrees with the calculated one available in literature.     

减色法彩色胶片中吡唑酮氮甲川染料有害吸收的研究

本文合成了3-甲基、3-氨基、3-苯胺基、3-苯甲酰氨基、3-苯脲基吡唑酮化合物所衍生的氮甲川染料,并以醋酸正丁酯为溶剂组成模拟系统。测得ε值并定义R_E=ε_y/ε_x作为实测的有害吸收度量值。同时编制了改进的PPP-CI程序,进行分子结构的模型计算,取得了电子跃迁强度f,定义R_T=f_y/f_x作为理论的有害吸收值,并获得R_E～R_T的良好线性关系(相关系数r=0.99)。得到的有害吸收的理论计算公式: R=0.349(f_y/f_x)+0.051。     

The effect of biasing electric field on the soft mode in the vicinity of the ferroelectric phase transition in liquid crystals

The complex permittivity of a room-temperature ferroelectric liquid crystal 4-n-octyloxy benzoic acid 4'-[(2-methylbutyloxy)carbonyl]phenyl ester, has been measured in the vicinity of the phase transition in the frequency range 40 Hz-300 kHz. In the para-electric phase the contribution ε_s of the soft mode to the permittivity and the soft-mode relaxation frequency f_s satisfy the Curie-Weiss law. Under a biasing field E, the helicoidal structure is unwound, and ε_s and f_s can then be measured even in the ferroelectric phase. On the other hand, the phase transition is smeared under the influence of E. This smearing results in deviations from the Curie-Weiss law for both ε_s and f_s in the vicinity of the transition. On increasing E, the maximum of the permittivity, ε_max, is lowered and shifted to higher temperatures. Both the shift and ε^-1_max are proportional to E^2/3. From experimentally found dependences, some constants in the free energy are determined.     

Enhanced conductivity and dielectric absorption in discotic liquid crystalline columnar phases of a vanadyl complex

A liquid crystalline vanadyl complex has been studied by DSC, polarizing optical microscopy, the reversal current technique, X-ray diffraction and frequency domain dielectric spectroscopy. The compound exhibits three columnar phases: rectangular ordered (Col_ro), rectangular disordered (Col_rd), and hexagonal disordered (Col_hd), all of which show a dielectric relaxation process at low frequencies. In the Col_ro low temperature phase this process seems to be connected with a slow relaxation of polarized polymeric chains inside the columns (mHz frequency range). However, in the Col_hd high temperature disordered phase this relaxation is faster (Hz range). It is interesting that the liquid crystalline phases studied show enhanced conductivity which changes by four orders of magnitude from 10^-9 S m^-1 in the orientationally disordered crystal (an ODIC phase) to 10^-5 S m^-1 in the Col_hd high temperature phase. Such a value of the conductivity is typical for semiconducting materials.     

Raman and Brillouin scattering from electrolytic solutions

A number of spectroscopic investigations are reported on aqueous solutions of CdCl₂ and molten Ca(NO₃)₂·4H₂)0 and its mixture with KNO₃. The Raman probe gives evidence of the existence of two different local structures in the solutions of CdCl₂: one is dominated by the solvent, the other by the solute. A competition between them exists whose equilibrium changes with concentration. Hypersonic and ultrasonic velocity data and hypersonic absorption results on the same system, as a function of concentration and of temperature, give evidence of a structural relaxation connected to the local variation of the structural arrangement induced by the solute. Extended X-ray absorption fine structure (EXAFS) measurements on Ca(NO₃)₂·4H₂O and its mixture with KNO₃ reveal an inner shell of water complexation for the Ca²⁺ and K⁺ ions that produces a close-packed structure in which hydration forces are mainly responsible for the local arrangement. Mandelstamm-Brillouin scattering results give evidence for a relaxation phenomenon to which both structural and shear mechanisms contribute. The mean relaxation time τ_r, and the relaxation modulus M_r show a non-Arrhenius behaviour, supporting the idea that our systems can be regarded as fragile liquids.     

热处理时间对锂电池正极材料Cr8O21的影响

本文以CrO₃为原料,采用高温固相法制备锂电池用正极材料Cr₈O₂₁,系统研究了热处理时间对Cr₈O₂₁结构、电化学性能的影响。采用TGA、XRD、SEM、EDS、ICP、EIS和恒流放电技术对制备的铬氧化物的物相及电化学性能进行研究。结果表明,延长热处理时间有利于提升材料的电化学性能。且不同的热处理时间对材料的电化学性能有重要影响。热处理时间为48 h得到的材料性能优异,在恒放电电流0.05 mA下,材料克比容量达到383.26 mAh·g^-1,克比能量达到1153.83 mWh·g^-1,平均放电电压3.01 V。