In‐situ Raman spectroscopy of current‐carrying graphene microbridge

In‐situ Raman spectroscopy was performed on chemical vapor deposited graphene microbridge (3 μm × 80 μm) under electrical current density up to 2.58 × 10⁸ A/cm² in ambient conditions. We found that both the G and the G′ peak of the Raman spectra do not restore back to the initial values at zero current, but to slightly higher values after switching off the current through the microbridge. The up‐shift of the G peak and the G′ peak, after switching off the electrical current, is believed to be due to p‐doping by oxygen adsorption, which is confirmed by scanning photoemission microscopy. Both C–O and C=O bond components in the C1s spectra from the microbridge were found to be significantly increased after high electrical current density was flown. The C=O bond is likely the main source of the p‐doping according to our density functional theory calculation of the electronic structure. Copyright © 2014 John Wiley & Sons, Ltd.     

不同晶相结构和形貌TiO2负载Ru催化剂的CO选择甲烷化

用水热法得到的钛酸纳米纤维前体,通过不同后处理方法合成了多种纳米结构的TiO₂．采用N₂等温吸附和BET比表面、X射线衍射、透射电镜和能量分散X射线分析表征了TiO₂及负载Ru催化剂的微结构,包括比表面、晶相结构和形貌以及Ru纳米颗粒尺寸分布等．对负载Ru催化剂在富氢条件下CO选择甲烷化反应活性测试表明：金红石相TiO₂和TiO₂-B为载体负载的Ru催化剂比锐钛矿相TiO₂负载的Ru催化剂表现出更高的反应性能．其活性区别说明了不同晶相结构和形貌TiO₂载体与Ru纳米颗粒的相互作用存在差异．     

Evidences for charge‐transfer complex formation in the benzene adsorption on sulfated TiO2–a resonance Raman spectroscopy investigation

Benzene adsorbed on highly acidic sulfated TiO₂ (S‐TiO₂) shows an intriguing resonance Raman (RR) effect, with excitation in the blue‐violet region. There are very interesting spectral features: the preferential enhancement of the e_2g mode (1595 cm⁻¹) in relation to the a_1g mode (ring‐breathing mode at 995 cm⁻¹) and the appearance of bands at 1565 and 1514 cm⁻¹. The band at 1565 cm⁻¹ is probably one of the components of the e_2g split band, originally a doubly degenerate mode (8a, 8b) in neat benzene, and the band at 1514 cm⁻¹ is assigned to the 19a mode, an inactive mode in neat benzene. These facts indicate a lowering of symmetry in adsorbed benzene, which may be caused by a strong interaction between S‐TiO₂ and the benzene molecule with formation of a benzene to Ti (IV) charge transfer (CT) complex or by the formation of a benzene radical cation species. However, the RR spectra of the adsorbed benzene cannot be assigned to the benzene radical cation because the observed wavenumber of the ring‐breathing mode does not have the value expected for this species. Moreover, it was found by ESR measurements that the amount of radicals was very low, and so it was concluded that a CT complex is the species that originates the RR spectra. The most favorable intensification of the band at 1595 cm⁻¹ in the RR spectra of benzene/S‐TiO₂ at higher excitation energy corroborates this hypothesis, as an absorption band in this energy range, assigned to a CT transition, is observed. Copyright © 2008 John Wiley & Sons, Ltd.     

Detection of small amounts of H2O in CO2‐rich fluid inclusions using Raman spectroscopy

Raman spectroscopic analysis at low (−100 °C) or high (100–200 °C) temperature is shown to be effective for detecting small amounts of H₂O in CO₂‐rich fluid inclusions from the deep lithosphere, which have previously been thought to be water‐free. Copyright © 2009 John Wiley & Sons, Ltd.     

Adsorption study of 4‐MBA on TiO2 nanoparticles by surface‐enhanced Raman spectroscopy

In this paper, the adsorption of 4‐mercaptobenzoic acid (4‐MBA) on TiO₂ nanoparticles was studied mostly by surface‐enhanced Raman spectroscopy (SERS) and UV‐vis spectroscopy, at different pH values as well as under different temperatures and concentrations. The results show that the 4‐MBA molecules are bonded to the TiO₂ surface both through the sulfur atoms and COO⁻ groups at neutral or alkaline pH, but only through the sulfur atom at acidic pH. Furthermore, the 4‐MBA molecules possess high adsorptive stability on TiO₂ at a comparatively high temperature (150 °C). Concentration‐dependent SERS experiments show that the saturation concentration for 4‐MBA adsorbed on TiO₂ is about 10⁻³ M in natural case (pH = 6). Copyright © 2009 John Wiley & Sons, Ltd.     

Experimental assessment of the phonon confinement in TiO2 anatase nanocrystallites by Raman spectroscopy

TiO₂ aerogels prepared by sol‐gel method and followed by supercritical drying have been annealed at temperatures ranging between 400 and 550 °C. The obtained TiO₂ anatase crystallites with the mean size between 6.4 and 13.9 nm, as obtained from transmission electron microscopy measurements, have been further investigated by Raman spectroscopy. It was found that the peak position and full width at half maximum (FWHM) of the TiO₂ anatase Raman bands located around 144, 398, and 638 cm⁻¹ are influenced by crystallite dimension. These spectral changes can be assigned to the combined action of several nanosize effects such as phonon confinement, phonon coupling, strain, and stoichiometry defects. Surprisingly, the best discrimination of the FWHM change with the nanocrystallite mean size was achieved for the 638 cm⁻¹ band, whereas the best discrimination for the peak position was found for the 398 cm⁻¹ band. The critical size values obtained from the peak position and FWHM evaluation were between 12.7 and 13.1 nm. Taking into consideration that only the phonon confinement and inhomogeneous strain can induce an asymmetric broadening of the Raman signal, the bands asymmetry was evaluated, and the critical size values of the nanocrystallites were determined to be between 10 and 11 nm. For a symmetric size distribution of TiO₂ anatase crystallites with dimensions between 6.4 and 13.9 nm, the obtained result indicates that the phonon confinement contribution to the overall size effects is more than 75%. No evidence about the influence of the phonon coupling and vacancies on the Raman features was observed. The comparison of the data derived from the experimental analysis with those obtained by applying the theoretical phonon confinement model indicates the necessity of developing an improved phonon confinement model. The asymmetry approach can be applied for a great variety of nanostructures, as a measure of the confinement effect. Copyright © 2011 John Wiley & Sons, Ltd.     

低温拉曼光谱研究二氧化钛纳米晶的相变

本文通过对二氧化钛纳米晶在-190℃温度的低温拉曼光谱的研究,得到了在二氧化钛纳米晶聚集体中,可以发生锐钛矿到板钛矿然后到金红石和/或直接到金红石的相变;也可发生板钛矿到锐钛矿然后到金红石和/或直接到金红石的相变。     

TiO_2/石墨烯/Ag复合结构SERS实验

基于氧化物半导体的光催化特性,能够降解有机物分子,使表面增强拉曼散射基底得以重复使用。提出了银纳米颗粒有效修饰覆盖有石墨烯的二氧化钛纳米棒阵列(TiO_2/石墨烯/Ag)复合结构作为表面增强拉曼散射基底,并对其进行了实验研究。利用水热法制备了二氧化钛纳米棒阵列;采用湿法转移石墨烯和光照还原方法制备了TiO_2/石墨烯/Ag复合结构。用罗丹明6G(R6G)分子作为探测分子,结果表明:随着紫外光照沉积时间增加,探针分子的拉曼信号先增强后减弱;计算得到最大增强因子值约为2.6×106。此外,还对TiO_2/石墨烯/Ag复合结构的紫外自清洁特性进行了初步实验,结果表明,紫外光照射20min后,其拉曼强度下降到42.3%,具有一定的紫外清洁效果。     

CO在MoS2/K2CO3/TiO2上的加H2反应

根据“盐类及氧化物等在高比表面载体上有自发分散倾向”的原理，制备了一种新型的用于由合成气（H2／CO）合成甲醇的催化剂MoS2/K2CO/TiO2(DSA),该催化剂具有较好的耐硫性和对甲醇有较高的选择性，通过对反应条件的教察得出结论：高压、低温、高空速有利于提高醇的选择性。     

TiO_2对α-Fe_2O_3纳米微粒拉曼散射效应的影响

选取α Fe2O3和TiO2研究一种氧化物对另一种氧化物的拉曼散射效应。采用Sol gel方法制备纳米α Fe2O3/TiO2复合微粒,α Fe2O3粒径及含量分别为20nm、150nm和3%、6%、12%。制备过程中调节水解时的pH值和热处理温度,得到掺杂α Fe2O3粒子的不同晶型的TiO2纳米颗粒。Raman测量结果显示,α Fe2O3粒径越小、含量越高,TiO2对其散射效应的影响越大。不同的TiO2晶型对α Fe2O3纳米粒子的拉曼增强效应也不同。锐钛矿型及金红石型TiO2对α Fe2O3有一定的拉曼增强作用,当水解pH值较小时,得到板钛矿型TiO2,由于部分板钛矿型TiO2振动声子模的峰位与α Fe2O3的重叠,所以尚难观察它对α Fe2O3的拉曼增强效应。     

Probing reoxidation sites by in situ Raman spectroscopy: differences between reduced CeO2 and Pt/CeO2

Raman spectroscopy is a powerful technique for detecting peroxo (O₂)^2– and superoxo (O₂)^– species adsorbed on defect sites of ceria. These sites are probed by reducing CeO₂ at high temperature and then chemisorbing oxygen species at low temperature. In the present study, it is shown for the first time that such Raman characterization has to be achieved at very low laser power to avoid formation of oxygen species by photolysis and analyze only the chemisorbed species. Respecting this requirement, the (O₂)^2– and (O₂)^– species formed on 0.7% Pt/CeO₂ compound, and the CeO₂ support used to prepare it were compared after reduction for various times and at various temperatures. Superoxo species were more stabilized on reduced 0.7% Pt/CeO₂ after short reduction at 773 K than on reduced CeO₂. Additionally, the distributions of peroxo species adsorbed on defect sites of Pt/CeO₂ and CeO₂ were significantly different after long reduction at 773 K in spite of similar amounts. Indeed, less stable species were formed during the reduction of 0.7% Pt/CeO_2. These two features revealed that new sites were created during the preparation and reduction of Pt/CeO₂ compared to its bare support. Copyright © 2012 John Wiley & Sons, Ltd.     

纳米颗粒DBS/TiO_2的拉曼光谱

采用水热法制得表面包覆有十二烷基苯磺酸的二氧化钛纳米粒子 ,并应用拉曼光谱对其进行了检测。结果表明 :样品为表面包覆有十二烷基苯磺酸的二氧化钛纳米粒子的集合体。其拉曼峰与未包裹的二氧化钛拉曼峰相比 ,出现了蓝移现象 ,从纳米粒子的表面结构及包裹层的压力出发对此现象进行了定性解释和讨论     

CO2连续激光蒸发制备单壁碳纳米管及其Raman光谱的研究

讨论了在室温下用波长10.6μm的CO2连续激光制备单壁碳纳米管的工艺条件和生长机理.用大功率CO2连续激光蒸发制备单壁碳纳米管,所用激光功率400—900W,高分辨透射电镜观察表明单壁碳纳米管直径1.1—16nm,随着激光功率的增加稍微增加.本文还分别用波长为514.5nm和632.8nm激发光测量了CO2红外激光制备的单壁碳纳米管的一级和二级Raman光谱,发现在Raman特征峰的位置、强度上都存在差异.还将用CO2红外激光制备的单壁碳纳米管的Raman光谱与用YAG激光制备的单壁碳纳米管的Raman光谱进行了比较. 关键词： 单壁碳纳米管 CO2连续激光 Raman光谱     

PATP在Ag/TiO_2纳米管基底上的表面增强拉曼散射和光催化过程研究

表面增强拉曼散射(SERS)是一种超灵敏、高选择性的分析方法,越来越受到人们的关注。对巯基苯胺(PATP)由于其易吸附在大多数SERS基底表面,并可以产生极强的SERS信号,因此常被用作SERS的探针分子。二氧化钛(TiO_2)是一种目前常用的光催化剂,但是其催化效率仍有待提高。将贵金属与TiO_2复合是提高其催化效率的有效手段。本文采用电化学阳极氧化法制备了二氧化钛纳米管(TiO_2NTs),并采用光化学还原方法在表面沉积了贵金属银,制备了一种同时具有SERS和催化性能的双功能基底,即银纳米粒子修饰的二氧化钛纳米管(Ag/TiO_2NTs),研究了PATP分子在该基底上的光催化过程,并与在银镜基底上的光催化过程进行了比较。我们发现,Ag/TiO_2NTs基底上的PATP在催化过程中峰强度逐渐减弱,但没有新峰的出现;而在银镜基底上PATP的峰强度随光照时间却几乎没有变化,证明了PATP分子在Ag/TiO_2 NTs上的光催化降解过程。本文还对Ag/TiO_2NTs上PATP的催化过程进行了动力学分析,结果表明PATP在该基底表面的催化反应为一级反应。     

Enhancing the efficiency of TiO2–perovskite heterojunction solar cell via evaporating Cs2CO3 on TiO2

In a TiO₂–perovskite heterojunction solar cell (TiO₂–PHSC), besides the perovskite CH₃NH₃PbX₃, TiO₂ as one side of the TiO₂/CH₃NH₃PbX₃ heterojunction also plays an important role in the photovoltaic effect. In order to improve the performance of the TiO₂–PHSC with the structure of glass/FTO/compact TiO₂/mesoporous TiO₂/CH₃NH₃PbI_3–xCl_x /poly‐TPD (poly(N,N ′‐bis(4‐butylphenyl)‐N,N ′‐bis(phenyl)benzidine))/Au, a 2 nanometer thick Cs₂CO₃ layer is thermally evaporated on the mesoporous TiO₂ layer. The short‐circuit current density (J_sc) raises from 17.7 mA cm^–2 to 18.9 mA cm^–2, the open‐circuit voltage (V_oc) from 0.81 V to 0.87 V, and the fill factor (FF) from 55.2% to 67.3%; as a result, the power conservation efficiency (PCE) increases from 8.0% to 11.1% under AM 1.5G solar illumination (100 mW cm^–2). Moreover, in a TiO₂–PHSC free of mesoporous TiO₂, where Cs₂CO₃ is evaporated on the compact TiO₂ layer, the J_sc, V_oc, FF and PCE values increase from 16.0 mA cm^–2, 0.83 V, 50.8% and 6.7% to 17.9 mA cm^–2, 0.90 V, 59.3%, and 9.5%, respectively. The reasons of the PCE increase for either the first kind of TiO₂–PHSC or the mesoporous‐TiO₂‐free TiO₂–PHSC with a nanometer‐thick Cs₂CO₃ layer on mesoporous TiO₂ or compact TiO₂ are discussed. (© 2014 WILEY‐VCH Verlag GmbH &Co. KGaA, Weinheim)     

Monitoring of the microstructure of ion‐irradiated nuclear ceramics by in situ Raman spectroscopy

Raman spectroscopy is an efficient technique for studying the evolution of microstructure of materials under irradiation. For that purpose, a Raman spectrometer has been recently installed at the JANNUS‐Saclay platform. In this paper, we describe the new setup for in situ experiments. These in situ experiments allowed following the microstructural evolution of different materials (SiC, ZrO₂ and B₄C) as a function of ion fluence on a single sample (either single crystal or polycrystalline ceramics) under the same irradiation conditions. Our results show that Raman spectroscopy is a versatile non‐contact technique for studying on‐line crystalline phase changes or amorphization of irradiated iono‐covalent solids. A detailed analysis of Raman spectra is provided for the three materials (SiC, ZrO₂ and B₄C) investigated in this study, revealing quite different behaviors upon irradiation. Basically, Raman spectroscopy gives insight on these evolutions at the level of bonds given by specific phonon modes, in good agreement with Rutherford backscattering channeling (RBS/C), X‐ray diffraction (XRD) or transmission electron microscopy (TEM) data, which provide information at a long‐range scale. Copyright © 2015 John Wiley & Sons, Ltd.     

掺磷TiO_2优化TiO_2/MBA/Ag三明治结构的SERS性能

本文以磷酸为磷源,通过溶胶水热法制备磷掺杂TiO_2,利用Lee和Meisel的方法制备银溶胶,以4-巯基苯甲酸(MBA)为探针分子,通过构建TiO_2/MBA/Ag三明治结构,研究磷掺杂二氧化钛对该基底表面增强拉曼(SERS)性能的提升。通过TEM、XRD、XPS、DRS和拉曼光谱图表征二氧化钛的形貌结构、化学组成、光学和拉曼性能,结果表明,制备出的磷掺杂二氧化钛为锐钛矿型纳米颗粒,粒径范围6~12nm,XPS显示磷以P~(5+)替代了Ti~(4+),形成O-P-O键掺入TiO_2的晶格中,当磷的掺杂量在1.77%时,TiO_2/MBA/Ag三明治体系具有最佳的SERS信号,这是因为适量的磷掺杂降低了TiO_2的能带间隙,丰富TiO_2的表面态,这能促进TiO_2向MBA分子的电荷转移。     

微区Raman光谱在TiO_2高压结构相变研究中的应用

本文以金红石单晶TiO2和锐钛矿多晶TiO2为研究对象,应用金刚石小压机和原位拉曼光谱测量技术,系统研究了室温高压下TiO2的结构相变。原位拉曼测量表明,金红石单晶TiO2在压力达到12.91GPa时开始发生由金红石结构向斜锆石结构(MI)的相变,当压力达到14.16 GPa时,相变完成;继续加压到21.65 GPa,没有发现进一步的相变;卸压时由斜锆石结构转变为PbO2结构,相变发生在大约7.11 GPa处。锐钛矿多晶TiO2在压力达到4.26 GPa时开始向PbO2结构转变,当压力达到8.34 GPa时相变完成;继续加压到12.94 GPa,样品开始发生由PbO2结构向斜锆石结构的相变,当压力达到18.74 GPa时相变完成;继续加压到21.39 GPa,没有发现进一步的相变;卸压时也由斜锆石结构转变为PbO2结构,起始相变压力点应高于8 GPa。     

Time‐resolved investigation of the ν1 ro‐vibrational Raman band of H2CO with fs‐CARS

The technique of femtosecond time‐resolved coherent anti‐Stokes scattering (fs‐CARS) is used to investigate the strongly perturbed ν₁ ro‐vibrational Raman band of formaldehyde (H₂CO). The time‐dependent signal is simulated using a ‘Watson‐’Hamiltonian in A‐type reduction and Raman theory for asymmetric rotors. The results are compared with the experimental data. The fs‐CARS method measures the evolution of the polarization in a molecular ensemble via superposition of many states and is sensitive to spectral irregularities or line shifts of the involved transitions. ‘Coriolis’ interactions play a major role in the analysis of the ν₁ band of formaldehyde. We successfully simulate the fs‐CARS transient signal from the ν₁ band of formaldehyde including a model for multiple ‘Coriolis’ interactions, without the necessity of describing the complete interaction between all the vibrational levels. ‘Coriolis’ coupling coefficients and energy shifts are derived from the experiment by a least‐square fit. The results are discussed and compared to literature values. Copyright © 2006 John Wiley & Sons, Ltd.     

Electrochemical in situ surface enhanced Raman spectroscopic characterization of a trinuclear ruthenium complex,Ru‐red

To study the fate of a molecular di‐μ‐oxo‐bridged trinuclear ruthenium complex, [(NH₃)₅Ru–O–Ru(NH₃)₄–O–Ru(NH₃)₅]⁶⁺, also known as Ru‐red, during the electro‐driven water oxidation reaction, electrochemical in situ surface enhanced Raman spectroscopy (SERS) investigations have been conducted on an electrochemically roughened gold surface in acidic condition. It was previously described that on a basal plane pyrolitic graphite electrode in 0.1 M H₂SO₄ aqueous solution, Ru‐red undergoes one electron oxidative conversion into a stable higher oxidation state ruthenium complex, Ru‐brown, at <1.0 V (vs normal hydrogen electrode (NHE)), and this leads to water oxidation and dioxygen release, but the fate of Ru‐red during electrochemistry was not studied in much detail. In this investigation, Ru‐red dispersed in acid electrolyte and immobilized on a roughened gold electrode without Ru‐red in solution has been subjected to anodic controlled potential experiments, and in situ SERS was carried out at various potentials in succession. The electrochemical SERS data obtained for Ru‐red are also compared with in situ SERS results of an electrodeposited ruthenium oxide thin film on the Au disk. Our study suggests that on a gold electrode in sulfuric acid solution containing Ru‐red, one electron oxidative conversion of Ru‐red to a higher oxidation state ruthenium compound, Ru‐brown, occurs at ca. 0.74 V (vs NHE), as supported by the electrochemical in situ SERS experiments. Moreover, at higher potentials and on Au disk, the Ru‐red / Ru‐brown are not stable and slowly decompose or electro‐oxidize leading to deactivation of the tri‐ruthenium catalytic system in acidic medium. Copyright © 2013 John Wiley & Sons, Ltd.