三氧化钼溶胶凝胶光致变色的研究

通过金属钼粉与过氧化氢溶液反应制备三氧化钼溶胶和凝胶,在高压汞灯的照射下,溶胶和凝胶由浅黄色变成蓝色。Raman光谱研究表明：通过紫外光照,MoO3凝胶结构进行了重整,呈有序排布。乙醇相的MoO3溶胶在紫外光照或长期自然光照下,均表现出光致变色特性。电子自旋共振(ESR)和X射线电子能谱(XPS)研究表明：空气中的MoO3经光照同时接受质子和电子后,生成了蓝色的钼青铜,其中Mo^6^+被还原成了Mo^5^+离子。     

ABO3型钙钛矿结构的可见光光催化剂LaCo0.5Ti0.5O3的设计与合成

采用溶胶-凝胶法在较低温度条件下设计合成了新型的具有ABO3型钙钛矿结构的三元金属复合氧化物LaCo0.5Ti0.5O3. 通过TG-DTA, XRD, XPS, UV-Vis DRS等测试技术和可见光光催化活性测试对其进行了表征. 结果表明, 与LaCoO3和La2Ti2O7相比, LaCo0.5Ti0.5O3样品表现出相对较高的可见光光催化活性, 并且合成温度较低. 这是由于原料中的Co2+和Ti4+离子通过电荷补偿作用使产物B位的两种金属均以+3价氧化态分布所致.     

掺Eu及Ag微粒的SiO2凝胶在多孔阳极氧化铝中的荧光增强

近年来,将稀土配合物掺杂于溶胶－凝胶（Sol-gel)基质中及在溶胶－凝胶制备过程中原位（In stitu)合成稀土配合物已有报道^[1]。溶胶－凝胶基质使掺杂分子和外界隔绝,形成一种很好的保护基质,而渗杂的光活性物质,由于受到笼效应的影响,掺杂分子之间相互孤立,减小了聚集体的生成和浓度猝灭^[2]。在溶胶－凝胶中掺杂镧系离子,尤其掺杂Eu^2 和Sm^2 等二价离子已成为研究热点,它们在光学存储^[3]、固态激光^[4]、绿光发光材料、药物学上的X射线无机发光材料等方面具有潜在应用前景。二价镧系离子（如Eu^2 ）通常是由三价离子（Eu^3 ）在加热条件下,经短波光还原或电化学还原产生的,而在溶胶－凝胶中既可有效地还原Eu^3 ,也可将Eu^2 固定在光学透明凝胶中^[5]。国内有关凝胶中掺杂稀土离子的荧光现象虽报道很多^[6],但将凝胶固定在多孔基底上却未见报道。多孔阳极氧化铝具有规则的六边形孔状结构,还可以根据需要制成不同的形状,在其为模板制备金纳米线^[7],由于溶胶可渗入几个至十个纳米深的孔道中,在多孔基底上用溶胶－凝胶法制作的薄膜能增强荧光现象并没有较好的重现性。     

甲基三乙氧基硅烷修饰的Ti3+/SiO2复合薄膜的发光性能

采用溶胶-凝胶(Sol-Gel)法, 以正硅酸乙酯(TEOS)和甲基三乙氧基硅烷(MTES)为先驱物, 盐酸为催化剂, 用二步水解法制备了Ti3+/SiO2薄膜和甲基三乙氧基硅烷修饰的Ti3+/SiO2复合薄膜. 采用红外光谱仪、X射线衍射仪、椭偏仪、荧光光谱仪等对膜层性质进行了分析. 结果表明, 掺杂Ti3+的SiO2薄膜分别在250 nm附近有一弱的激发峰, 294 nm附近有一强的激发峰, 在393 nm附近出现一强的发射峰. IR光谱发现, MTES修饰的Ti3+/SiO2复合薄膜的Si—OH的吸收峰强度比Ti3+/SiO2薄膜的略减小, Si—O—Si的吸收峰明显增强, 表明复合薄膜硅氧网络结构更规则, 有利于Ti3+的均匀分散. Ti3+/SiO2薄膜与复合薄膜的孔隙率分别为13.64%和6.66%, 表明MTES的加入使薄膜更致密. 在空气中陈放30 d后, Ti3+/SiO2薄膜已经检测不到荧光发射峰, 而MTES修饰的Ti3+/SiO2复合薄膜荧光强度只下降了18%. 在氮气中陈放30 d后, 普通薄膜与复合薄膜的荧光强度均仅下降了10%. 表明Ti3+的荧光猝灭的主要原因是由于Ti3+被氧化造成的. 溶胶中加入MTES后, 薄膜表面结构得到改善, 有效地防止了Ti3+的氧化, 荧光强度更稳定.     

氮掺杂二氧化钛薄膜的光催化性能研究

采用溶胶-凝胶法制备了氮掺杂Ti O2薄膜;利用X射线光电子能谱仪、紫外-可见光谱仪表征了所制备的薄膜的化学状态和光吸收性能;并考察了可见光照射下薄膜的亲水性能和光催化性能.结果表明:N通过取代部分O的方式进入到Ti O2薄膜中,且掺杂后在可见光区的光吸收增强;最优条件下,Ti O2-xNx薄膜的接触角由31°降到12°,亲水化速度常数为0.018,可见光照射3 h,亚甲基蓝的降解率达到45%.     

新型荧光粉Ca2Zn4Ti16O38∶Pr3+，Na+的合成和红色长余辉性质

采用溶胶-凝胶法合成了Ca2Zn4Ti16O38:Pr3+,Na+荧光粉.通过X-射线衍射和荧光光谱表征样品的物相组成和发光性质.X射线衍射(XRD)分析表明添加适量的H3BO3作助熔剂有利于形成良好的Ca2Zn4Ti16O38晶体结构.荧光光谱表明Ca2Zn4Ti16O38:Pr3+,Na+在可见光区(450～495 nm)呈现Pr3+离子的4f→4f厂特征激发光谱以及613 nm(1D2→3H4)和644 nm(3P0→3F2)特征发射.Ca2Zn4Ti16O38:Pr3+,Na+被可见光(475 nm)激发产生的(3P0→3F2)(644 nm)红色发射呈现出极慢的衰减特性.Ca2Zn4Ti16O38:Pr3+,Na+是一种新型的可见光激发红色长余辉荧光粉.     

NiO在γ-Al2O3及 TiO2/γ-Al2O3载体上的表面存在状态

本文采用LRS,XRD,UV－DRS考查了γ－Al2O3上TiO2的分散容量,分散态Ti^4 离子的配位环境;NiO在经TiO2改性后的γ－Al2O3载体上的分散容量,结果表明,（1)TiO2在γ－Al2O3表面的分散容量约为0．65mmol/100m^2γ－Al2O3,当TiO2含量低于该分散容量时Ti^4 在γ－Al2O3载体表面以嵌入形式呈离子态分布,而含量离于分散容量时还有结晶态的TiO2出现,（2）NiO在TiO2/γ－Al2O3载体表面的分散容量约为1．1mmol/100m^2γ－Al2O3,比之在γ－A2O3载体表面的分散容量（1．5mmol/100m^2γ－Al2O3）要低,这是由于γ-AlO3表面上部分空位被Ti^4 离子占据,用表面相互作用的“嵌入模型”（Incorporation Model)讨论的这些结果。     

Er3+和Yb3+共掺杂La2Ti2O7纳米晶的上转换发光

采用溶胶-凝胶法制备了 Er3+单掺杂A2 Ti2O7(A=La,Y,Gd)和Er3+,Yb3+共掺杂的La2 Ti2O7纳米晶样品.用X射线衍射仪、扫描电子显微镜和紫外-可见-近红外光谱仪分别对样品的结构、形貌和光吸收性质进行了表征;测试了样品在980 nm激光激发下的室温上转换光谱.结果发现,样品都发出了很强的绿光(大约在525和549 nm)和红光(大约660 nm).通过研究这些基质的晶体结构对上转换发光的影响,发现La2 Ti2O7基质中Er3+离子的上转换发射最强.对La2 Ti2O7纳米晶的上转换发光研究表明,Yb3离子能够有效地敏化Er3离子的上转换发射.对上转换发光强度与泵浦功率的依赖分析,发现红光和绿光的发射均属于双光子吸收过程,最后讨论了Er3+和Yb3的上转换发光机制.     

Ti~(3+)自掺杂的纳米TiO_2的制备及其可见光催化性能

以TiH2为Ti源,H2O2为氧化剂,首先通过表面氧化得到不同状态的前驱体凝胶,然后采用后续水热处理制备Ti3+自掺杂的纳米Ti O2.考察了前驱体凝胶状态及水热处理时间对材料结构和性能的影响.利用X射线衍射、透射电子显微镜、X射线光电子能谱、电子顺磁共振波谱和紫外-可见漫反射光谱手段对样品进行表征.以次甲基蓝溶液为模拟废水评价样品的可见光催化降解性能.结果表明,与纯Ti O2相比,Ti3+的自掺杂使材料在可见光区有明显的吸收,并具有良好的可见光催化降解性能和循环使用性能.当采用黄色凝胶为前驱体时,在160°C下水热处理24 h所得样品在可见光下光催化降解次甲基蓝的反应速率常数(0.0439 min-1)是纯Ti O2的18.3倍.     

不同制备方法对BiOCl材料的形貌、结构与光催化性能的影响研究

对比采用溶剂热合成、传统固相合成与溶胶-凝胶合成技术,制备了四方相BiOC1和Nd3+掺杂BiOCl光催化材料.运用X射线粉末衍射(XRD)、扫描电子显微镜(SEM)及紫外-可见吸收光谱(UV-Vis),研究了不同合成方法所制备BiOCl材料的相结构、形貌和紫外-可见光吸收性能;并以甲基橙溶液为模拟废水,研究了不同方法所制备的BiOCl材料的光催化性能.结果表明:溶剂热合成的BiOCl是由纳米片组装成粒径小于1μm微球,紫外-可见吸收边为335 nm;固相合成所得BiOCl结晶度较高,其片状颗粒粒径约为6μm,紫外-可见吸收边为430n m;溶胶-凝胶合成法制得BiOCl片状颗粒粒径约为3～4 μm,紫外-可见吸收边为430 nm.进一步地对比研究了稀土离子Nd3+掺杂前后BiOCl样品的结构、紫外-可见光吸收特性,可以发现,Nd3+掺杂后样品的相结构及形貌均无变化,但吸收边均发生不同程度的红移,以溶胶-凝胶法制得的样品效果最为明显,并具有最优的光催化性能.     

Visible light photo-oxidation of model pollutants using CaCu3Ti4O12: an experimental and theoretical study of optical properties, electronic structure, and selectivity

Charge transfer between metal ions occupying distinct crystallographic sublattices in an ordered material is a strategy to confer visible light absorption on complex oxides to generate potentially catalytically active electron and hole charge carriers. CaCu3Ti4O12 has distinct octahedral Ti4+ and square planar Cu2+ sites and is thus a candidate material for this approach. The sol?gel synthesis of high surface area CaCu3Ti4O12 and investigation of its optical absorption and photocatalytic reactivity with model pollutants are reported. Two gaps of 2.21 and 1.39 eV are observed in the visible region. These absorptions are explained by LSDA+U electronic structure calculations, including electron correlation on the Cu sites, as arising from transitions from a Cu-hybridized O 2p-derived valence band to localized empty states on Cu (attributed to the isolation of CuO4 units within the structure of CaCu3Ti4O12) and to a Ti-based conduction band. The resulting charge carriers produce selective visible light photodegradation of 4-chlorophenol (monitored by mass spectrometry) by Pt-loaded CaCu3Ti4O12 which is attributed to the chemical nature of the photogenerated charge carriers and has a quantum yield comparable with commercial visible light photocatalysts.     

Experimental and computational study of the electronic structural changes in LiTi2O4 spinel compounds upon electrochemical Li insertion reactions

Electronic structural changes in LiTi(2)O(4) spinel compounds upon electrochemical lithium insertions were investigated by X-ray absorption spectroscopy (XAS) measurements and first principles calculations based on spin-polarized density functional theory. Ti K-edge, O K-edge XAS spectra and theoretical calculations indicate that oxide ions as well as titanium ions are involved in electronic structural changes caused by electrochemical lithium ion insertions. The considerable effect of the oxide ions in the early 3d transition metal (titanium) oxide system is discussed in this article.     

CCl4的光解微观机制研究

利用激光光解瞬态吸收光谱技术,研究有氧和无氧条件下CCl4的激光光解.结果表明,在248 nm激光作用下, CCl4发生了单光子吸收,反应生成{CCl4－Cl}σ电荷转移复合物、(CCl3＋…Cl－)离子对、CCl3O2过氧自由基等瞬态物种,它们的衰减过程是表观一级反应. {CCl4－Cl}σ电荷转移复合物在有氧/无氧条件下的拟合衰减速率常数分别是3.38×106 s－1和3.65×106 s－1,它的形成不受氧气含量影响. (CCl3＋…Cl－)离子对在有氧/无氧条件下的拟合衰减速率分别为3.73×107 s－1和3.02×107 s－1,它的形成也不受氧气含量影响, CCl3O2过氧自由基需在有氧条件下形成,拟合衰减速率是2.32×104 s－1.     

新戊基钛在MCM-41表面的接枝反应及产物性质

采用原位红外光谱法在真空系统中考察了MCM-41分子筛表面与四新戊基钛Ti(CH2CMe3)4的反应,发现这个反应可在室温下定量进行,得到表面新戊基钛(≡Si－O)2Ti(CH2CMe3)2. 这种表面新戊基钛很容易与CH3OH、H2O和O2进一步发生反应分别得到(≡Si－O)2Ti(OCH3)2、(≡Si－O)2Ti(OH)2和(≡Si－O)2Ti(OCH2CMe3)2等表面化合物.在氧气中焙烧由(≡Si－O)2Ti(CH2CMe3)2水解所得的(≡Si－O)2Ti(OH)2可制得表面含钛MCM-41介孔分子筛（Ti-MCM-41）.元素分析、低温N2吸附-脱附、紫外可见漫反射光谱、X射线粉末衍射和FTIR等表征结果表明,接枝反应和后续的处理不破坏分子筛的介孔结构; Ti-MCM-41的比表面积和孔直径较MCM-41略有降低; Ti原子在Ti-MCM-41表面以TiO4四面体配位状态分散,并对乙烯氧化有较明显的光催化活性.论文还通过对Ti-MCM-41与水热合成骨架含钛[Ti]-MCM-41结构和光催化活性的比较,对分子筛类材料光催化作用机制进行了分析探讨.     

TiO2纳米薄膜的溶胶-凝胶工艺制备和表征

通过ｓｏｌ－ｇｅｌ工艺在普通钠钙玻璃表面制备了均匀透明的锐钛矿型ＴｉＯ２纳米薄膜,ＴｉＯ２薄膜的Ｘ射线衍射分析表明,当薄膜的厚度小于０．４６μ时,薄中未出现锐钛矿的衍射峰,随着镀膜次数或薄膜厚度的增加,薄膜中ＴｉＯ２纳米微晶的平均晶粒大小逐渐增大,ＴｉＯ２薄膜的透光率略有减小,其吸收阈值发生了明显的红移,ＸＰＳ实验结果表明：薄膜中除含有Ｔｉ、Ｏ元素外,还有一定量来自有机前驱物中未完全燃烧的碳和少量     

间接电氧化法合成甘油醛

通过电化学合成前驱体和溶胶-凝胶法在Ti表面修饰一层纳米TiO2膜,在纳米Ti02膜上电沉积分散的Pt微粒制成钛基纳米TiO2-Pt(Ti/nano-TiO2-pt)修饰电极。采用循环伏安法、间接电氧化法研究了纳米Ti02-Pt修饰电极的电催化活性以及Mn^3 ／Mn^2 媒质氧化甘油为甘油醛的过程。结果表明,纳米Ti02-Pt修饰电极对Mn^2 的电氧化具有高催化活性,电流效率可达90％以上,非均相电解得到的Mn^3 可一步氧化甘油为甘油醛,收率为91％。     

Effect of Processing Parameters on the Optical Properties of TiO<Subscript>2</Subscript>/Ormosil Planar Waveguide

Hybrid TiO₂/ormosil waveguiding films have been prepared by the sol-gel method at low thermal treatment temperature of 150C. The influence of processing parameters including the molar ratios of titanium butoxide (Ti(OBu)₄)/3-glycidoxypropyltrimethoxysilane (GLYMO) and H₂O/Ti(OBu)₄ (expressed as R), especially aging of sol on the optical properties was investigated. The optical properties of films were measured with scanning electron microscope (SEM), UV/VIS/NIR spectrophotometer (UV-Vis), m-line and the scattering-detection method. The results indicate that the film thickness increases with the increase of sol aging time, but the variation of refractive index as a function of sol aging time depends on the relative ratios of GLYMO to Ti(OBu)₄. Higher transmittance and lower attenuation of the planar waveguide can be obtained in the sol with lower Ti(OBu)₄ contents and shorter aging time.     

掺Tb-硅基发光材料制备过程中结构及发光性能

采用溶胶 凝胶技术,制备了不同退火温度下掺Tb3＋的SiO2玻璃,掺Tb3＋的凝胶玻璃在448,544,585,620 nm显示Tb3＋的5D4 7FJ(J=3,4,5,6)的特征发光光谱.通过不同退火温度下样品的激发光谱、发射光谱、红外光谱、远红外光谱及差热 热重谱研究了掺Tb3＋的硅基材料由凝胶向玻璃转变过程中的结构变化及对Tb3＋发光性能的影响.结果显示,在50～100 ℃退火温度下,凝胶大部分吸附水分子被除去,在150～500 ℃退火温度区,是凝胶向玻璃转变的主要结构变化区,并且其发光强度也明显增加,到800 ℃时趋于稳定.这些现象得出一个结论,Tb3＋的发光跃迁被O－H基强烈猝灭而随退火温度的升高而加强.     

Pre-edge features of Ti K-edge X-ray absorption near-edge structure for the local structure of sol-gel titanium oxides.

Titanium K-edge X-ray absorption near-edge structure (XANES) spectroscopy is used to examine the local Ti environments in the sol, gel, and xerogels of titanium oxide prepared by a sol-gel method. The xerogels were prepared by heat treatment at 200, 300, 400, 500, and 600 degrees C (denoted xero-200, xero-300, xero-400, xero-500, and xero-600), and the xerogels were doped with Fe(II), Ni(II), and Cu(II) ions (xero-Fe, xero-Ni, and xero-Cu). The local structures of the samples are compared using the pre- and post-edge features of the XANES spectra. Further analysis of the pre-edge features using Gaussian functions provides the energy and height of each peak, and the intensity ratios between peaks. Based on the resulting data, the samples can be classified into three groups: a weak Ti-Ti interaction group, an anatase-like structure group, and an anatase group. The sol, gel, xerogel, and xero-Ni are in the weak Ti-Ti interaction group, and the xero-200, xero-Fe, and xero-Cu are in the anatase-like structure group. The remaining samples are in the anatase group.     

Gas phase synthesis of Au clusters deposited on titanium oxide clusters and their reactivity with CO molecules

Titanium oxide clusters were formed in the gas phase by the laser ablation of a Ti rod in the presence of oxygen in a He gas. Not only stoichiometric but also nonstoichiometric titanium oxide clusters, Ti(n)O(2n+x)(+) (n = 1-22 and x = -1-3), were formed. The content of oxygen atoms depends strongly on a partial pressure of oxygen. Gold clusters, Au(m) (m = 1-4), were generated by the laser ablation, which were then deposited on Ti(n)O(2n+x) clusters. The formation of Au(m)Ti(n)O(2n+x)(+) follows electron transfer from Au(m) to Ti(n)O(2n+x)(+). The reactivity of Au(m)Ti(n)O(2n+x)(+) cluster ions with CO was examined for different m, n, and x by the mass spectrometry. It was found that Au(m) on Ti(n)O(2n-1)(+) are less reactive than those on the other Ti(n)O(2n+x)(+) (x = 0 and 1). In addition, the reactivity is highest when Au(m) (m = 1 and 3) is on the stoichiometric titanium oxide (x = 0), whereas the reactivity is also high when Au(2) is on the oxygen-rich titanium oxide (x = 1). The reactivity was found to relate to geometrical structures of Au(m)Ti(n)O(2n+x)(+), which were studied by density functional calculations.