相转移有机前驱体BiOAc0.6Br0.2I0.2固溶体合成表面富有氧空位的棒状S型 Bi4O5I2/Bi4O5Br2异质结

近年来,卤氧铋(BiOX,X=Cl,Br,I)作为多功能半导体光催化材料,因其具有独特的层状结构和电子结构,吸引了广泛关注.然而,相对低的导带(CB)和高的价带(VB)位置导致其氧化还原能力弱,从而限制了其实际应用.研究表明,通过富铋策略调控BiOX中元素化学计量比,可以实现对其能带结构的可控调控.尽管富铋半导体材料被视为有效的可见光光催化剂的候选材料之一,但是单一组分的富铋光催化剂不利于光生载流子的分离和迁移.具有匹配能带结构的富铋基复合光催化剂的构建已被证实可以加速光生电子-空穴对的分离和迁移.与传统的Ⅱ型异质结构相比,S型异质结既可以有效地分离光生载流子,又可以增强其氧化还原能力.如果双富铋基半导体之间能形成S型异质结,不仅可以拓展可见光响应,而且还可以增强光生电荷的氧化还原能力.基于Bi₄O₅I₂/Bi₄O₅Br₂的匹配能带,制备具有强氧化还原能力的S型Bi₄O₅I₂/Bi₄O₅Br₂异质结是可行的.除了电子结构外,表面缺陷的引入也对改善光催化性能起到了重要作用.氧空位(OVs)作为一种典型的缺陷,可以捕获电子来抑制光诱导载流子的复合,并加速这些捕获载流子向吸附剂的转移.此外,它们还可以充当有机污染物和分子氧的吸附位点,促进吸附和降解效率.目前,光催化材料中OVs的形成通常需要复杂、苛刻的条件,如高温、高压、惰性或还原气氛处理等,因此寻找简便有效的方法生成OVs仍然具有挑战性.此外,在无惰性或还原气氛下对有机前驱体进行热处理被认为是形成OVs的有效方法.鉴于此,本文通过低温煅烧二维纳米片有机前驱体BiOAc_0.6Br_0.2I_0.2(Ac-=CH3COO-)固溶体,成功合成了表面富有氧空位的一维纳米棒状的S型Bi₄O₅I₂/Bi₄O₅Br₂异质结(Bi₄O₅I₂/Bi₄O₅Br₂-OV).X射线衍射、高分辨率透射电子显微镜电子顺磁共振以及X射线光电子能谱分析(XPS)等结果均证实了表面氧空位的存在.同时,根据吸收光谱图和肖特基曲线计算出Bi₄O₅I₂和Bi₄O₅Br₂的能带结构,而且通过XPS价带谱进一步证实了所计算的价带的可靠性.根据捕获剂实验、氯化硝基四氮唑蓝(NBT)转移以及对苯二甲酸荧光均证实了h+、·OH和·O2-是参与光催化降解的主要活性物种.再结合上述能带结构以及活性物种的类型推断出光生载流子的迁移方式将遵循S型机制,而不是传统的II型异质结.而且,通过光电流、阻抗和稳态荧光均证实了表面OVs和S型异质结的协同效应,有利于提高Bi₄O₅I₂/Bi₄O₅Br₂-OV的光生电子空穴对的分离效率,并延长其寿命,从而有效地提高其光催化性能.在可见光照射下,OVs和S型异质结的协同效应赋予Bi₄O₅I₂/Bi₄O₅Br₂-OV显著的可见光光催化性能,对抗生素四环素和染料罗丹明B的去除率分别高达90.2%和97.0%,均高于Bi₄O₅I₂(56.8%和71.8%)、Bi₄O₅Br₂(47.4%和68.4%)、固溶体BiOAc_0.6Br_0.2I_0.2(67.0%和84.0%)以及表面具有低氧空位浓度的Bi₄O₅I₂/Bi₄O₅Br₂-P(30.6%和40.4%).此外,在实际废水或电解质存在下,S型Bi₄O₅I₂/Bi₄O₅Br₂-OV异质结仍呈现出优异的光催化性能.本文不仅为OVs修饰的富铋基异质结的设计提供了有效策略,也为界面载流子的分离和迁移提供了切实可行的途径.     

双酚A敏化Bi5O7I纳米片增强可见光自降解活性

以BiOIO₃为前驱体,通过高温煅烧法制备了一系列铋(Bi)基材料,并系统地研究了不同样品的物相组成、微观形貌、光学性能及光催化活性。实验结果表明,Bi₅O₇I纳米片在可见光(λ>420 nm)照射60 min后,对双酚A(BPA)的降解率可达99.3%,5次循环使用后仍能去除97%的BPA,表现出良好的光催化活性与稳定性。研究表明,BPA可以作为表面配体,与Bi₅O₇I发生表面配位,通过配体-金属电荷转移(LMCT)的光敏化机制作用实现太阳光的高效利用并促进其自降解。     

固溶体内电场调控增强Bi24O31ClxBr10-x体相电荷流动和光催化活性

光催化是一种在能源和环境领域有着重要应用前景的绿色技术,在光照射下可将有机污染物彻底降解为二氧化碳和水,但因缺乏精确调控电荷流动的方法,导致大多数光催化剂活性不高.因此,促进光生电荷的高效分离一直是光催化研究的重要方向.目前多数电荷分离调控研究集中于表面修饰、表面缺陷设计、异质结构建等表面电荷分离改善策略,而对于体相电荷分离调控研究相对较少.卤氧化铋固溶体光催化材料由于独特的层状晶体结构、可调节的带隙结构和优化的电荷分离效率,近年来受到广泛关注.目前对固溶体的体相电荷分离机理尚不清楚.内电场作为一种新的增强光催化反应活性的有效调控途径,通过定向促进体相电荷的分离和转移,使光生载流子快速参与氧化还原反应.然而,通过调控内电场来增强卤氧化铋固溶体光催化活性的报道较少,且缺乏从理论和实验的角度对固溶体内电场大小以及电荷分离机理的分析.本文构建了具有相同形貌和晶体结构的Bi₂₄O₃₁Cl_xBr_10-x固溶体光催化剂,并考察了其催化性能.密度泛函理论计算、开尔文探针力显微镜(KPFM)和Zeta电位测试结果表明,通过改变卤素类型和比例可增加晶体结构单元的不对称性,从而调节[Bi₂₄O₃₁]和[X]层之间的电势差,增强光催化材料的内电场强度,促进体相电荷分离和转移效率,进而提高酚类有机污染物的降解活性.光电化学测试发现,相较于Bi₂₄O₃₁Cl₁₀和Bi₂₄O₃₁Br₁₀,Bi₂₄O₃₁Cl₄Br₆固溶体体相电荷分离效率显著提高,表面和界面上的电荷转移效率以及载流子密度增加.Bi₂₄O₃₁Cl₄Br₆的载流子密度分别是Bi₂₄O₃₁Cl₁₀和Bi₂₄O₃₁Br₁₀的33.1倍和4.7倍,Bi₂₄O₃₁Cl₄Br₆固溶体降解双酚A活性分别是Bi₂₄O₃₁Cl₁₀和Bi₂₄O₃₁Br₁₀的6.21倍和2.71倍.此外,其它酚类的降解实验也证明了光催化活性和内电场强度以及电荷分离效率成正相关.综上所述,本文从内电场的角度揭示了固溶体策略对光催化性能增强的内在机理,这些发现将进一步加深对体相电荷运动行为的理解,为设计高活性光催化剂提供一条新的途径.     

表面活性剂修饰碳酸氧铋的制备及光催化性能

采用水热法,以阳离子表面活性剂十六烷基三甲基溴化铵(CTAB)、非离子型表面活性剂聚乙二醇8000(PEG8000)、阴离子表面活性剂十二烷基硫酸钠(SDS)及SDS与CTAB耦合修饰Bi₂O₂CO₃。 系统地研究了表面活性剂种类及用量对Bi₂O₂CO₃晶面、形貌、光吸收特性及光催化降解效率的影响。 以紫外光下降解罗丹明B(RhB),考察样品的光催化性能。 结果表明,当Bi盐投加量为6 mmol(2.9106 g)时,SDS对Bi₂O₂CO₃的修饰对其光催化活性有所抑制;0.6 g CTAB修饰Bi₂O₂CO₃能有效提高其光催化活性;0.3 g SDS与CTAB耦合修饰Bi₂O₂CO₃就能有效提高其光催化活性;0.3 g PEG8000修饰Bi₂O₂CO₃也能使其光催化活性有所提高。     

TiO2/Bi2O3纳米复合体的制备及可见光催化产氢性能

首先采用相分离的水解-溶剂热法制备了Bi₂O₃纳米粒子,然后利用简单的湿化学法在Bi₂O₃表面负载不同比例的TiO₂纳米颗粒,进而得到TiO₂/Bi₂O₃纳米复合体。通过气氛调控的表面光电压谱(SPS)等测试表明,表面负载适量的TiO₂后能够提高Bi₂O₃光生电荷分离。可见光催化产氢和降解污染物测试结果进一步证明,表面负载适量的TiO₂后可显著提高其可见光催化活性,其中Ti/Bi摩尔比为7%时具有最高的光催化活性。这主要归因于TiO₂具有较为合适的导带能级位置,可以接收Bi₂O₃在可见光激发下所产生的高能级电子,从而抑制光生电子-空穴对复合,并且维持了高能级电子较高的还原能力。     

沉淀法制备Bi2O3的晶相转变过程及其光催化性能

以硝酸铋为原料,氨水为沉淀剂,通过液相沉淀法制得前驱体Bi(OH)₃,并将Bi(OH)₃分别在不同温度和时间下焙烧。利用X射线衍射(XRD)、拉曼光谱、热重(TG)、扫描电子显微镜(SEM)、X射线光电子能谱(XPS)及紫外-可见漫反射光谱(UV-Vis DRS)详细研究了Bi(OH)₃转变为Bi₂O₃的过程及相变过程中粒子形貌、大小、光吸收性质等。结果表明,前驱体Bi(OH)₃经过焙烧之后,发生了如下的转变过程:Bi(OH)₃→Bi₅O₇NO₃→β-Bi₂O₃/Bi₅O₇NO₃→β-Bi₂O₃/Bi₅O₇NO₃/α-Bi₂O₃→α-Bi₂O₃,而且转变过程伴随着粒子长大。在上述转变过程中,与Bi₅O₇NO₃向β-Bi₂O₃转变的过程相比,从β-Bi₂O₃到α-Bi₂O₃相变过程更为迅速。此外,以光催化降解罗丹明B(RhB)为模型反应,考察了不同晶相的Bi₂O₃光催化活性,结果表明Bi₅O₇NO₃和β-Bi₂O₃材料具有优异的光催化性能,而α-Bi₂O₃具有较低的光催化活性。     

Bi4V2O11/石墨烯异质结光催化剂的制备及其在降解抗体污染物中应用

发展和设计高效、廉价和稳定的光催化剂用于抗生素污染物降解仍然存在巨大的挑战。 本文通过一种便捷的水热方法制备了Bi₄V₂O₁₁/石墨烯复合材料并用于可见光下抗生素污染物光催化降解。 通过自由基追踪实验,确认了光催化降解过程中活性物质为h⁺和·OH基团。 根据实验结果,提出了相应的反应机理。 石墨烯的引入可以有效地促进光生电子-空穴对的分离,从而增强光催化活性。 该复合催化剂展现出良好的活性和稳定性。 该方法以石墨烯为载体制备了光催化降解材料,为高性能光催化剂的制备提供了参考。     

p区金属氧化物Ga2O3和Sb2O3光催化降解盐酸四环素性能差异

对沉淀法合成的p区金属氧化物Ga₂O₃和Sb₂O₃紫外光光催化降解盐酸四环素的性能进行了研究,讨论了制备条件对光催化性能的影响。最佳制备条件下得到的Ga₂O₃-900和Sb₂O₃-500样品光催化性能存在巨大差异,通过X射线粉末衍射、傅里叶红外光谱、N2吸附-脱附测试、荧光光谱、拉曼光谱、电化学分析及活性物种捕获实验等对样品进行分析,研究二者光催化降解盐酸四环素的机理,揭示影响光催化性能差异的本质因素。结果表明,Ga₂O₃和Sb₂O₃光催化性能差异主要归结于二者不同的电子和晶体结构、表面所含羟基数量及光催化降解机理。     

锌掺杂OV-β-Bi2O3可见光催化活性的提高:能带结构的调节和电荷分离的促进

采用溶胶-凝胶-原位碳热还原处理的方法,制备了一种含有氧空位(OV)的新型Zn掺杂β-Bi₂O₃纳米材料(OV-Zn∶Bi₂O₃),氧空位的浓度可以通过改变Zn²⁺的掺杂量进行调节。作为参照,只有氧空位没有Zn²⁺的新型β-Bi₂O₃(OV-β-Bi₂O₃)也通过类似的方法制得。通过紫外可见漫反射光谱、X射线光电子能谱、电子顺磁共振、光致发光光谱和光电化学测试,系统研究了氧空位和Zn²⁺掺杂对OV-Zn∶Bi₂O₃降解亚甲基蓝(MB)和2,4,6-三氯苯酚(2,4,6-TCP)可见光催化活性的综合影响。结果表明,氧空位的引入不仅可以使光吸收向长波方向拓展,而且可以促进光生载流子的分离。因此,与传统的β-Bi₂O₃相比,OV-β-Bi₂O₃对亚甲基蓝(MB)和2,4,6-三氯苯酚(2,4,6-TCP)的降解活性显著增强。对于OV-Zn∶Bi₂O₃催化剂,Zn²⁺掺杂可使光催化剂的价带边缘向下移动,增强了光激发空穴的氧化能力,并且适量的锌掺杂也能提高光生载流子的分离效率。因此,OV-Zn∶Bi₂O₃的可见光活性优于OV-β-Bi₂O₃,而且当Zn与Bi物质的量之比为0.3时,OV-Zn∶Bi₂O₃-0.3对MB和2,4,6-TCP的降解活性最高。     

β-Bi2O3修饰Bi2WO6光催化降解苯酚及其可能机理

采用简单混合法制备了一系列Bi₂O₃/Bi₂WO₆复合光催化剂. 在紫外光降解水中苯酚的过程中, Bi₂O₃/Bi₂WO₆的光催化活性随Bi₂O₃含量的增加呈现先增大后减小的趋势. 当Bi₂O₃最佳负载量等于12.5% (质量分数, w)时, 该复合光催化剂的活性大约是单一Bi₂WO₆的4 倍. 固体样品表征表明, Bi₂O₃主要以β-Bi₂O₃存在, 复合光催化剂是Bi₂O₃和Bi₂WO₆的简单混合物. 此外, 在电催化氧化水的过程中, β-Bi₂O₃/Bi₂WO₆薄膜电极的光电流远大于β-Bi₂O₃和Bi₂WO₆薄膜电极的光电流之和. Bi₂O₃对Bi₂WO₆光催化的促进作用是由于前者接受后者的光生空穴, 提高Bi₂WO₆光生载流子的分离效率, 从而加快了O₂的还原和苯酚的降解.     

Sol-gel synthesis of K3InF6 and structural characterization of K2InC10O10H6F9, K3InC12O14H4F18 and K3InC12O12F18

K₃InF₆ is synthesized by a sol-gel route starting from indium and potassium acetates dissolved in isopropanol in the stoichiometry 1:3, with trifluoroacetic acid as fluorinating agent. The crystal structures of the organic precursors were solved by X-ray diffraction methods on single crystals. Three organic compounds were isolated and identified: K₂InC₁₀O₁₀H₆F₉, K₃InC₁₂O₁₄H₄F₁₈ and K₃InC₁₂O₁₂F₁₈. The first one, deficient in potassium in comparison with the initial stoichiometry, is unstable. In its crystal structure, acetate as well as trifluoroacetate anions are coordinated to the indium atom. The two other precursors are obtained, respectively, by quick and slow evaporation of the solution. They correspond to the final organic compounds, which give K₃InF₆ by decomposition at high temperature. The crystal structure of K₃InC₁₂O₁₄H₄F₁₈ is characterized by complex anions [In(CF₃COO)₄(OH_x)₂]^(5−2x)− and isolated [CF₃COOH_2−x]^(x−1)− molecules with x=2 or 1, surrounded by K⁺ cations. The crystal structure of K₃InC₁₂O₁₂F₁₈ is only constituted by complex anions [In(CF₃COO)₆]³⁻ and K⁺ cations. For all these compounds, potassium cations ensure only the electroneutrality of the structure. IR spectra of K₂InC₁₀O₁₀H₆F₉ and K₃InC₁₂O₁₂F₁₈ were also performed at room temperature on pulverized crystals.     

Li2O-TiO2-SiO2-P2O5和Li2O-TiO2-Al2O3-P2O5体系锂离子固体电解质的制备及性能研究

一些具有NASICON型网格结构的固体电解质具有高的电导率和好的稳定性,NASICON的意思是Na Super Ionic Conductor[1]。当NaZr2(PO4)3中P5 被Si4 部分取代时便可以得到具有NASICON结构的Na1 xZr2SixP3-xO12体系,其具有高的钠离子电导率。然而有相同结构的Li1 xZr2SixP3-xO12体系的离子电导率却很低,这是因为Li 半径太小,而NASICON三维网格结构的离子通道太大,两者不匹配而使电导率下降[2]。但当LiZr2(PO4)3中Zr4 被离子半径小些的Ti4 取代,所得LiTi2(PO4)3的通道就与Li 半径相匹配,适合于锂离子的迁移,从而使其电导率…     

Non-centrosymmetric Ba3Ti3O6(BO3)2

The compound previously reported as Ba₂Ti₂B₂O₉ has been reformulated as Ba₃Ti₃B₂O₁₂, or Ba₃Ti₃O₆(BO₃)₂, a new barium titanium oxoborate. Small single crystals have been recovered from a melt with a composition of BaTiO₃:BaTiB₂O₆ (molar ratio) cooled between 1100°C and 850°C. The crystal structure has been determined by X-ray diffraction: hexagonal system, non-centrosymmetric space group, a=8.7377(11) Å, c=3.9147(8) Å, Z=1, wR(F²)=0.039 for 504 unique reflections. Ba₃Ti₃O₆(BO₃)₂ is isostructural with K₃Ta₃O₆(BO₃)₂. Preliminary measurements of nonlinear optical properties on microcrystalline samples show that the second harmonic generation efficiency of Ba₃Ti₃O₆(BO₃)₂ is equal to 95% of that of LiNbO₃.     

Synthesis, crystal structure, infrared and Raman spectra of Sr4Cu3(AsO4)2(AsO3OH)4·3H2O and Ba2Cu4(AsO4)2(AsO3OH)3

The two new compounds, Sr₄Cu₃(AsO₄)₂(AsO₃OH)₄·3H₂O (1) and Ba₂Cu₄(AsO₄)₂(AsO₃OH)₃(2), were synthesized under hydrothermal conditions. They represent previously unknown structure types and are the first compounds synthesized in the systems SrO/BaO-CuO-As₂O₅-H₂O. Their crystal structures were determined by single-crystal X-ray diffraction [space group C2/c, a=18.536(4) Å, b=5.179(1) Å, c=24.898(5) Å, β=93.67(3)°, V=2344.0(8) Å³, Z=4 for 1; space group P4₂/n, a=7.775(1) Å, c=13.698(3) Å, V=828.1(2) Å³, Z=2 for 2]. The crystal structure of 1 is related to a group of compounds formed by Cu²⁺-(XO₄)³⁻ layers (X=P⁵⁺, As⁵⁺) linked by M cations (M=alkali, alkaline earth, Pb²⁺, or Ag⁺) and partly by hydrogen bonds. In 1, worth mentioning is the very short hydrogen bond length, D···A=2.477(3) Å. It is one of the examples of extremely short hydrogen bonds, where the donor and acceptor are crystallographically different. Compound 2 represents a layered structure consisting of Cu₂O₈ centrosymmetric dimers crosslinked by As1φ₄ tetrahedra, where φ is O or OH, which are interconnected by Ba, As2 and hydrogen bonds to form a three-dimensional network. The layers are formed by Cu₂O₈ centrosymmetric dimers of CuO₅ edge-sharing polyhedra, crosslinked by As1O₄ tetrahedra. Vibrational spectra (FTIR and Raman) of both compounds are described. The spectroscopic manifestation of the very short hydrogen bond in 1, and ABC-like spectra in 2 were discussed.     

A new 2212-type stair like structure: Bi14Sr21Fe12O61, m=5 member of the generic [Bi2Sr3Fe2O9]m[Bi4Sr6Fe2O16] family

A new oxide, Bi₁₄Sr₂₁Fe₁₂O_61, with a layered structure derived from the 2212 modulated type structure Bi₂Sr₃Fe₂O₉, was isolated. It crystallizes in the I2 space group, with the following parameters: a=16.58(3) Å, b=5.496(1) Å, c=35.27(2) Å and β=90.62°. The single crystal X-ray structure determination, coupled with electron microscopy, shows that this ferrite is the m=5 member of the [Bi₂Sr₃Fe₂O₉]_m[Bi₄Sr₆Fe₂O₁₆] collapsed family. This new collapsed structure can be described as slices of 2212 structure of five bismuth polyhedra thick along , shifted with respect to each other and interconnected by means of [Bi₄Sr₆Fe₂O₁₆] slices. The latter are the place of numerous defects like iron or strontium for bismuth substitution; they can be correlated to intergrowth defects with other members of the family.     

Ion-beam irradiation of lanthanum compounds in the systems La2O3-Al2O3 and La2O3-TiO2

Thin crystals of La₂O₃, LaAlO₃, La_2/3TiO₃, La₂TiO₅, and La₂Ti₂O₇ have been irradiated in situ using 1 MeV Kr²⁺ ions at the Intermediate Voltage Electron Microscope-Tandem User Facility (IVEM-Tandem), Argonne National Laboratory (ANL). We observed that La₂O₃ remained crystalline to a fluence greater than 3.1×10¹⁶ ions cm⁻² at a temperature of 50 K. The four binary oxide compounds in the two systems were observed through the crystalline-amorphous transition as a function of ion fluence and temperature. Results from the ion irradiations give critical temperatures for amorphisation (T_c) of 647 K for LaAlO₃, 840 K for La₂Ti₂O₇, 865 K for La_2/3TiO₃, and 1027 K for La₂TiO₅. The T_c values observed in this study, together with previous data for Al₂O₃ and TiO₂, are discussed with reference to the melting points for the La₂O₃-Al₂O₃ and La₂O₃-TiO₂ systems and the different local environments within the four crystal structures. Results suggest that there is an observable inverse correlation between T_c and melting temperature (T_m) in the two systems. More complex relationships exist between T_c and crystal structure, with the stoichiometric perovskite LaAlO₃ being the most resistant to amorphisation.     

Raman scattering investigations on lanthanum-doped Bi4Ti3O12-SrBi4Ti4O15 intergrowth ferroelectrics

The ferroelectric ceramics of Bi₄Ti₃O₁₂, SrBi₄Ti₄O₁₅, and lanthanum-doped Bi₄Ti₃O₁₂-SrBi₄Ti₄O₁₅ were synthesized, and their Raman spectra were investigated. La-doping resulted in the enlargement of remnant polarization of Bi₄Ti₃O₁₂-SrBi₄Ti₄O₁₅. The structure of the Bi₂O₂ layers and TiO₆ octahedra of the intergrowth was found to be different from those of Bi₄Ti₃O₁₂ and SrBi₄Ti₄O₁₅. La³⁺ ions exhibit pronounced selectivity for the occupation of A site as La content is lower than 0.50, and tend to be incorporated into Bi₂O₂ layers when the La content is higher than 0.50. Lanthanum substitution brings about the structural phase transition in Bi₄Ti₃O₁₂-SrBi₄Ti₄O₁₅. The variation of ferroelectric property may be attributed to combined contribution from the decreasing of the oxygen vacancies, the relaxation of the lattice distortion, the destroying of the insulation and the space charge compensation effects of the Bi₂O₂ slabs.     

g-C_3N_4/CaTi_2O_5复合材料制备及其光催化性能

利用类石墨氮化碳(g-C_3N_4)和亚稳相钙钛氧化物(CaTi_2O_5)固相法制备C_3N_4/CaTi_2O_5复合材料。利用X射线衍射(XRD)、金相显微镜、扫描电子显微镜(SEM)及附带能谱分析仪(EDS)和N2吸附-脱附对样品的显微结构和比表面积进行检测分析,并用紫外-可见吸收光度计(UV-Vis)测试了样品的光吸收性能,研究C_3N_4与CaTi_2O_5物质的量之比(nC_3N_4/nCaTi_2O_5)对C_3N_4/CaTi_2O_5复合样品的物相结构和微观形貌的影响,同时考察C_3N_4/CaTi_2O_5复合样品在可见光照射下光催化降解罗丹明染料效果。实验结果表明:相比纯C_3N_4和CaTi_2O_5样品,C_3N_4/CaTi_2O_5复合样品在可见光下具有较高的光催化性能,随着nC_3N_4/nCaTi_2O_5增加,样品的光催化降解率随之增加而后降低,当nC_3N_4/nCaTi_2O_5=1∶1时,样品的光催化降解率达到最大值99.5%,并且循环重复利用5次后,样品的光催化剂降解率仍几乎保持不变。复合样品光催化性能提高主要归因于复合能级结构有效地抑制了电子和空穴复合所致。     

g-C3N4/CaTi2O5复合材料制备及其光催化性能

利用类石墨氮化碳（g-C₃N₄）和亚稳相钙钛氧化物（CaTi₂O₅）固相法制备C₃N₄/CaTi₂O₅复合材料。利用X射线衍射（XRD）、金相显微镜、扫描电子显微镜（SEM）及附带能谱分析仪（EDS）和N₂吸附-脱附对样品的显微结构和比表面积进行检测分析,并用紫外-可见吸收光度计（UV-Vis）测试了样品的光吸收性能,研究C₃N₄与CaTi₂O₅物质的量之比（n_C3N4/nCaTi₂O₅）对C₃N₄/CaTi₂O₅复合样品的物相结构和微观形貌的影响,同时考察C₃N₄/CaTi₂O₅复合样品在可见光照射下光催化降解罗丹明染料效果。实验结果表明：相比纯C₃N₄和CaTi₂O₅样品,C₃N₄/CaTi₂O₅复合样品在可见光下具有较高的光催化性能,随着n_C3N4/nCaTi₂O₅增加,样品的光催化降解率随之增加而后降低,当n_C3N4/nCaTi₂O₅=1：1时,样品的光催化降解率达到最大值99.5%,并且循环重复利用5次后,样品的光催化剂降解率仍几乎保持不变。复合样品光催化性能提高主要归因于复合能级结构有效地抑制了电子和空穴复合所致。     

Magnetic diphase nanostructure of ZnFe2O4/γ-Fe2O3

Magnetic diphase nanostructures of ZnFe₂O₄/γ-Fe₂O₃ were synthesized by a solvothermal method. The formation reactions were optimized by tuning the initial molar ratios of Fe/Zn. All samples were characterized by X-ray diffraction, thermogravimetric analysis, infrared spectroscopy, and Raman spectra. It is found that when the initial molar ratio of Fe/Zn is larger than 2, a diphase magnetic nanostructure of ZnFe₂O₄/γ-Fe₂O₃ was formed, in which the presence of ZnFe₂O₄ enhanced the thermal stability of γ-Fe₂O₃. Further increasing the initial molar ratio of Fe/Zn larger than 6 destabilized the diphase nanostructure and yielded traces of secondary phase α-Fe₂O₃. The grain surfaces of diphase nanostructure exhibited a spin-glass-like structure. At room temperature, all diphase nanostructures are superparamagnetic with saturation magnetization being increased with γ-Fe₂O₃ content.