2-乙酰基-1-甲基吡咯激发态结构动力学及溶剂效应的共振拉曼光谱和密度泛函理论计算

获取了覆盖紫外光谱中A带和B带吸收的共7个不同激发波长的共振拉曼光谱, 并结合密度泛函理论方法研究了2-乙酰基-1-甲基吡咯(2-Ac-NMP)的A带和B带电子激发和Franck-Condon区域结构动力学. 在TD-B3LYP/6-311++G(d,p)计算水平上, A带和B带吸收的跃迁主体为π→π^* . A带和B带共振拉曼光谱分别指认为13个振动模式和8个振动模式的基频、泛频和组合频, 其中C＝O伸缩振动(ν₈)、C3-C4-C5不对称伸缩振动+C2-C6伸缩振动(ν₁₄)及环上CH面内摇摆(ν₁₈)对拉曼光谱强度贡献最大, 表明2-Ac-NMP的S_π激发态结构动力学主要沿反应坐标展开. 考察了溶剂对共振拉曼光谱强度模式的影响, 结果表明, 在同一溶剂中, 随激发波长由长变短, C＝O伸缩振动模(ν₈)的强度呈现出由强变弱再变强的现象. 这种变化规律与Franck-Condon区域S_n/S_π态混合或势能面交叉相关, 并受溶剂的有效调控.     

二氧化钛系列光催化剂的拉曼光谱

采用溶胶-凝胶法制备了TiO₂粉体和薄膜光催化剂.使用FT-Raman光谱和激光共聚焦拉曼光谱研究了粉体和薄膜的拉曼光谱,探讨了热处理条件、Fe³⁺掺杂和以硅胶为载体的薄膜化所引起的TiO₂结构变化.结果表明,TiO₂在350℃存在由无定形向锐钛矿相的转变,600℃下存在锐钛矿相向金红石相的转变,750℃下完全转变为金红石相;掺杂会引起TiO₂的晶格畸变,导致拉曼谱峰宽化;以硅胶为载体的TiO₂负载薄膜的部分拉曼谱峰与粉体相比,有一定的位移和宽化.     

亮氨酸与异亮氨酸的表面增强拉曼光谱

报道了在蛋白质氨基酸中唯一一对异构体氨基酸——亮氨酸和异亮氨酸的FT-拉曼光谱和在银胶基底上的表面增强拉曼光谱(SERS). 归属了各振动、增强峰位并分析了异构体氨基酸分子内不同振动模式引起的拉曼位移及其在不同pH值下SERS的变化. 分子内不同的振动模式主要源于异构体氨基酸中一个甲基和主链的不同连接次序, 表现在拉曼光谱; 亮氨酸的甲基摇摆ρ(CH₃)和非对称变形δ_as(CH₃)在962, 945, 924和1454, 1408 cm^－1; 异亮氨酸的ρ(CH₃), δ_as(CH₃)在922和1448, 1420, 1394 cm^－1. C—CO, C—C, H—O…H及骨架晶格振动峰位基本对应. 饱和液态的拉曼光谱和SERS中, 各基团振动峰位的差异表现得更为明显. 初步推测了这对氨基酸异构体在银表面吸附状态的模型.     

乐果与氧化乐果在金/银核-壳粒子上的SERS研究

联合红外、拉曼光谱及其在金/银核-壳粒子上的表面增强拉曼散射(SERS)光谱表征了乐果和氧化乐果两种乐果类似物, 归属并分析了两乐果类似物中P＝S与P＝O的不同而引起的振动模式, 峰位变化及其酸碱影响. 振动光谱显示, ν(P＝O), ν(P＝S)分别在690, 650 cm^－1附近, 两分子结构中对应的ν(NH), ν_s(CH₂), ν(C-O), ν(O＝C-N) II, ν(S-CH₂)振动峰位中差异显著, 但ν_as(CH₃), ν(P-O-C), ν(O＝C-N) I, δ(CH₃), ν(C-C), ν(C-C＝O)则基本对应. 在金/银核-壳粒子基底上, 进一步探讨了两乐果类似物中各基团在不同浓度, pH值及酸、碱水解历程条件下的SERS变化规律, 并运用SERS机理并结合TEM初步阐述了两乐果类似物在金/银核-壳粒子表面的吸附状态.     

I2-1-己烯复合物电子转移振动重组能的共振拉曼强度分析

获得了I₂-1-己烯复合物的吸收横截面和绝对共振拉曼横截面.用约270 nm光激发导致复合物的I-I伸缩振动模和C-C伸缩振动模等拉曼基频、泛频及其组合频强度的共振增强.采用含时波包理论的简单模型定量确定I₂-1-己烯复合物的光致电子转移振动重组能和均质展宽.总振动重组能3 744 cm^-1分布于4个振动模,贡献最大是I-I伸缩振动v₁₃,其值为2 490 cm^-1,约占总振动重组能的2/3.其次为C-C伸缩振动v₄₆,其值为1 170 cm^-1,约为总振动重组能的1/3.剩余2%的振动重组能是由烷基CH₃和CH₂的扭转振动v₃₆和v₂₄贡献.     

高分辨偏正拉曼光谱对丙酸酐C=O振动模的拉曼光谱非一致效应研究

根据C=O振动的各向同性和各向异性拉曼光谱和红外光谱特点讨论研究了丙酸酐分子的局部有序排列以及振动耦合机理. 利用三级联共聚焦拉曼光谱仪测定了不同浓度丙酸酐的各向同性与各向异性拉曼光谱图, 分别采集了丙酸酐在四氯化碳和甲醇中的光谱以及不同极性溶剂中的光谱, 具体分析了丙酸酐C=O振动模的浓度效应、 溶剂效应以及拉曼光谱非一致效应(NCE). 结果表明, 丙酸酐C=O振动模的NCE效应随着浓度的降低而减小; 随着溶剂极性的减小而增加. 利用密度泛函理论的B3LYP-D3/31-311G(d,p)基组计算了丙酸酐单体和二聚体的几何稳定构型, 用聚集态理论模型解释了丙酸酐分子的NCE效应、 浓度效应与溶剂效应. 理论计算结果与实验结果相吻合.     

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.     

魔方状微纳结构BaTiO3的制备及其压电催化性能

在简单溶剂热条件下,通过控制钡、钛物质的量之比制备了魔方状微纳结构BaTiO₃粉体,并以5 mg·L^-1罗丹明B(RhB)溶液为降解对象测试其压电催化性能。采用扫描电子显微镜、X射线衍射、傅里叶变换红外光谱对所制备粉体的物化性质进行详细表征,并测试其压电、光催化活性及循环稳定性。结果表明,钡、钛物质的量之比为1∶1时,合成的粉体为由立方体组装而成的魔方状四方相结构的BaTiO₃。在40 kHz、360 W的超声条件下,180 min内的降解率达90%,5次循环后的降解率为79.7%,变化率为11.4%,优于其光催化性能,具备优异的压电催化活性及循环稳定性。     

NaNO3和NaClO4在N,N-二甲基甲酰胺中的离子溶剂化

利用红外光谱研究了NaNO₃和NaClO₄在N,N-二甲基甲酰胺(DMF)溶剂中发生离子-溶剂和离子-离子的相互作用, 分析结果表明, DMF的OC-N谱带发生了明显的变化. 定量计算了在Na⁺浓度为0.22~1.24 mol/kg范围内的溶剂化数为1~4. 对谱图中酰胺基上C-N和CO的特征峰强度随Na⁺浓度变化的对比, 推测离子溶剂化作用导致DMF的酰胺基内部形成共轭键. 利用量子化学方法进行优化及热力学性质计算, 得到C-N键伸缩振动频率及红外光谱强度变化规律. 优化结构与实验结论相符合. 由NaNO₃的ν₂谱带及NaClO₄的ν₁谱带的解析得到溶液中阴离子缔合效应的一般规律, 并通过阴离子缔合特征峰与酰胺基上的N-C-N面外振动峰(865 cm^-1)的变化情况, 讨论了溶液中的离子溶剂化作用.     

B2O3-Bi2O3-ZnO-Al2O3玻璃助烧剂对BaTiO3陶瓷烧结条件、晶体结构和介电性能的影响

通过调节B₂O₃-Bi₂O₃-ZnO-Al₂O₃(BBZA)玻璃的添加量研究其对钛酸钡(BaTiO₃)陶瓷烧结条件、晶体结构和介电性能的影响。结果表明：添加适量的BBZA玻璃能够有效地将BaTiO₃陶瓷烧结温度由1 350℃降至950℃,并使其致密化。同时,添加BBZA玻璃后,BaTiO₃的晶体结构随着烧结温度的升高而发生转变(立方相→四方相)。另外,BBZA玻璃的引入使BaTiO₃陶瓷的居里峰得到了有效的抑制和拓宽。陶瓷微观形貌显示,玻璃相均匀分布在BaTiO₃晶粒表面。优化的BaTiO₃陶瓷制备条件如下：BBZA添加量(质量分数)为2.0%,烧结温度为950℃。在该条件下制备的BaTiO₃陶瓷介电常数达到1 364,介电损耗低至1.2%。     

单层，少层和块状WS2薄膜中声子位移随温度的变化

Two-dimensional transition metal disulfides (TMDs) have recently attracted significant research attention due to their rich physical and chemical properties. Graphene has also been studied intensively due to its high electron mobility of ~200000 cm²·V⁻¹·s⁻¹. Since there is no band gap, it is difficult for a graphene-based device to achieve high current on/off ratio. For TMDs, such as MoS₂, MoSe₂, WSe₂, and WS₂, the band gaps of these materials can be adjusted according to the number of layers. Since TMD has the advantage of suppressing source-drain tunneling current in an ultra-short transistor and offering superior immunity to short-channel effects, it is also attractive for use as a channel material in Si complementary metal oxide semiconductor (CMOS) devices larger than 22 nm. Among them, MoS₂ in single-layer and multi-layer films have been intensively researched for many years. MoS₂-based field effect transistors (FETs) with excellent electrical properties have been reported. WS₂ has lower in-plane electronic mass than MoS₂, MoSe₂, and MoTe₂, and therefore has potential for higher carrier mobility or higher output current for WS₂-based FETs. Experimental research on WS₂ is limited compared to MoS₂, and more work is needed to further exploit the full potential of WS₂-based FETs. Therefore, the electron-phonon interaction and vibration properties of WS₂ used in nano-electronic applications and FETs must be investigated. To this end, mono-layer (1L), few-layer (FL), and bulk WS₂ films were prepared using mechanical exfoliation from a WS₂ crystal. 3M scotch-tape was used for transferring the WS₂ films. Detailed temperature-dependent Raman study on 1L, FL, and bulk WS₂ films has been conducted using a 514-nm excitation laser. Raman spectroscopy, as an effective and non-destructive approach for phonon vibration study, has been used to evaluate TMDs. The Raman spectra reveal much useful information on the test sample in terms of peak position and spectral shape change. With the film thickness increasing to bulk, the A_1g(Γ) and E_2g¹(Γ) modes show blue-shift and red-shift, respectively, with respect to 1L WS₂. Moreover, when the dominant Raman vibration modes swaps between E_2g¹(Γ) and A_1g(Γ), the "cross-over" temperature was identified for 1L, FL, and bulk WS₂ films. WS₂ shows smaller frequency change Δ between the E_2g¹(Γ) and A_1g(Γ) modes than MoS₂, with varying film thickness. The temperature coefficient of the Raman peak position was one magnitude lower for WS₂ than MoS₂, implying that WS₂ has better thermal stability than MoS₂. The results of this systematic study provide a physical guidance for WS₂-based device design.     

IN situ Confocal Microprobe Raman Spectroscopic Studies on Defective La-based Complex Oxides

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大黄素的电化学氧化还原机理研究

本文利用循环伏安法(CV)、红外光谱循环伏吸法(CVA)和导数循环伏吸法(DCVA)研究大黄素(Q)在乙腈溶剂中的电子转移机理.Q的还原过程中阴离子自由基Q^?-会结合中性分子Q生成二聚物Q₂^?-.Q₂^?-在更负的电位下进一步还原为Q₂^2-.当扫描范围为-0.2 ~ -2.0 V时,经过一个循环伏安过程,在扫描结束物质并没有回到反应物Q,而是Q₂^2-. Q₂^2-会继续发生电化学反应,经历两步一电子过程,分别生成Q₂^3-. 和Q₂^4-.,对应CV图中峰C₃和C₄.当扫描范围扩大至1.0~-2.0 V时,在更正的电位下,观察到两个新的氧化峰A₁和A₂,该范围内的三圈扫描结果表明,在扫描结束物质重新氧化回到Q.当扫描范围缩小至0.3 ~ -1.4 V,A2峰随着扫描圈数的增加而增大,与A2峰对应的氧化产物Q₂^?-在溶液中不断积累.A1峰对应于Q₂^?-氧化回到Q.     

Fraction of excited-state oxygen formed as b Σg in solution-phase-photosensitized reactions II. Effects of sensitizer substituent

The fraction F_Σ of excited-state oxygen formed as b ¹Σ_g⁺ was determined for a series of triplet-state photosensitizers in CCl₄ solutions. F_Σ was determined by monitoring the intensities of (a) O₂(b ¹Σ_g⁺) fluorescence at 1926 nm (O₂(b ¹Σ_g⁺)→O₂(a ¹Δ_g) and (b) O₂(a ¹ Δ_g) phosphorescence at 1270 nm (O₂(a ¹Δ_g) → O₂(X³Σ_g⁻)). Oxygen excited states were formed by energy transfer from substituted benzophenones and acetophenones. The data indicate that F_Σ depends on several variables including the orbital configuration of the lowest triplet state and the triplet-state energy. The available data indicate that the sensitizer-oxygen charge transfer (CT) state is not likely to influence F_Σ strongly by CT-mediated mixing of various sensitizer-oxygen states.     

在CdS水悬浮液中O2光吸收的pH效应

为了深入了解间接光腐蚀过程, Grätzel等人曾考察过O₂在CdS和Rh₂0₃/CdS 悬浮液(pH=9)中光吸收行为, 发现光照生成的SO₄^2-的µmol数值基本上为加入O₂的µmol数值的一半, 且反应后悬浮液的pH降低^[3]。     

Synthesis, characterization and reactivity of some novel dinuclear mixed-ligand peroxouranium(VI) complexes

Novel anionic dinuclear mixed-ligand peroxo complexes of the type [(UO₂)₂(O₂)₃L(H₂O)₂]³⁻ (L = Histidinate, aspartate, salicylate, Imidazolate and glutamate) have been synthesized from the interaction of uranyl ion (UO₂²⁺) with peroxide (O₂²⁻) in the presence of the respective coligand (L) at pH 9–10. The sparingly soluble complexes were characterized by elemental analyses, FT-IR, laser Raman (LR) and UV-vis spectroscopy and solution electrical conductance measurements. Based on these studies, a double bridged dinuclear structure involving one peroxo and the mixed ligand L (via-COO⁻) has been tentatively proposed. Infra-red coupled with LR spectra evidenced structurally different metal bound peroxides (ν² and σ:σ). An aqueous solution of the salicylate and aspartate complexes have been shown to convert triphenylphosphine (PPh₃), cyclohexene, styrene and SO₂ to the corresponding OPPh₃, 1,2 cyclohexanediol, phenylethyleneglycol and SO₄²⁻, respectively.     

L-Cysteine-assisted Synthesis of Copper Gallium Sulfide Microspheres

An effective L-cysteine-assisted synthetic route has been successfully developed to prepare copper gallium sulfide(CuGaS₂) microspheres under solvothermal conditions with CuCl₂·2H₂O, GaCl₃ and L-cysteine as source materials, in which L-cysteine was used as the sulfide source and complexing molecule. The experiments revealed that the synthesized sample was of a typical CuGaS₂ tetragonal structure. Moreover, the prepared CuGaS₂ crystals consisting of microspheres made up of nanoflakes, and the diameter of the nanoflakes was about 20 nm. Raman spectrum of the obtained CuGaS2 exhibits a high-intensity peak of the A₁ mode at 306 cm^-1. Meanwhile, a possible growth mechanism was proposed based on the investigations.     

Thermal dissociation of the protein homodimer ecotin in the gas phase

The influence of charge on the thermal dissociation of gaseous, protonated, homodimeric, protein ecotin ions produced by nanoflow electrospray ionization (nanoES) was investigated using the blackbody infrared radiative dissociation technique. Dissociation of the protonated dimer, (E₂ + nH)ⁿ⁺ E₂ⁿ⁺ where n = 14–17, into pairs of monomer ions is the dominant reaction at temperatures from 126 to 175 °C. The monomer pair corresponding to the most symmetric charge distribution is preferred, although 50–60% of the monomer product ions correspond to an asymmetric partitioning of charge. The relative abundance of the different monomer ion pairs produced from E₂¹⁴⁺, E₂¹⁵⁺, and E₂¹⁶⁺ depends on reaction time, with the more symmetric charge distribution pair dominating at longer times. The relative yield of monomer ions observed late in the reaction is independent of temperature indicating that proton transfer between the monomers does not occur during dissociation and that the different monomer ion pairs are formed from dimer ions which differ in the distribution of charge between the monomers. For E₂¹⁷⁺, the yield of monomer ions is independent of reaction time but does exhibit slight temperature dependence, with higher temperatures favoring the monomers corresponding to most symmetric charge distribution. The charge distribution in the E₂¹⁵⁺ and E₂¹⁶⁺ dimer ions influences the dissociation kinetics, with the more asymmetric distribution resulting in greater reactivity. In contrast, the charge distribution has no measurable effect on the dissociation kinetics and energetics of the E₂¹⁷⁺ dimer.     

丙烯酰胺-丙烯酸钠共聚物的键结构和光散射研究

用溶液聚合方法制备了一组单体含量相同、分子量不同的丙烯酰胺-丙烯酸钠(AM-AA)共聚物样品,用¹³CNMR和常规光散射方法进行了表征。该组样品的化学组成是均一的(AA摩尔含量16.9±1.1%),AA单体在大分子链中的序列分布为孤立、无规的,聚电解质在盐水体系中的光散射理论适用于共聚物在0.12mol/LNaCl水溶液体系。用恒化学位下的折光指数增量代替恒盐组成的折光指数增量,可从一次常规光散射实验分别求得共聚物样品的真实、第二维利系数A₂和均方旋转半径〈R²〉_z,其关系为:A₂=0.0619M_w^-0.21,〈R²〉_z^1/2=0.0210M_w^0.54.     

Synthesis of thromboxane A2 analogs—3 : (+)-Thiathromboxane A2

(+)-11a-methano-9,11-thiathiromboxane A₂(1) was synthesized from prostaglandin A₂ and prostaglandin E₂.