Bi_2MoO_6/BiVO_4异质结的水热合成和可见光催化活性(英文)

采用一步水热法制备Bi2MoO6/BiVO4复合光催化剂.利用X射线衍射(XRD)、场发射扫描电子显微镜(FESEM)、高分辨透射电子显微镜(HRTEM)等手段对其晶体结构和微观结构进行了表征.结果表明,Bi2MoO6纳米粒子沉积在BiVO4纳米片表面从而形成异质结结构.紫外-可见漫反射光谱(UV-Vis DRS)表明所制备的Bi2MoO6/BiVO4异质结较纯相Bi2MoO6和BiVO4对可见光吸收更强.由于形成异质结结构及其光吸收性能使Bi2MoO6/BiVO4光催化活性有较大提高.可见光下(λ420 nm)光催化降解罗丹明B(RhB)实验结果表明,Bi2MoO6/BiVO4光催化活性较纯相Bi2MoO6和BiVO4高.Bi2MoO6/BiVO4样品光催化性能提高的原因是Bi2MoO6和BiVO4形成异质结,从而有效抑制光生电子-空穴对的复合,增大了可见光吸收范围及比表面积.     

网状钼酸铋的可见光催化活性

采用无助剂、无模板的水热法成功合成网状Bi2MoO6. pH值对这一形貌的形成起重要作用. 所制备的网状Bi2MoO6样品表现出优异的可见光催化活性,其光催化活性比固相法合成的块状Bi2MoO6样品高得多.     

原位稀土修饰Bi2MoO6高效可见光催化剂

采用原位法制备了系列稀土离子修饰的Bi₂MoO₆可见光催化剂并应用于罗丹明B的光催化降解,HPLC-MS显示该反应经脱除乙基的过程形成5个中间产物,最后完全矿化。研究表明,Gd³⁺修饰效果最佳,且原位法优于浸渍法,主要归因于Gd³⁺进入Bi₂MoO₆晶格,形成施主能级,导致能级带隙变窄,不仅有利于可见光活化光催化剂,而且阻碍电子-空穴复合并抑制修饰剂流失,从而提高光催化活性和稳定性。     

镂空Bi2MoO6微球的制备及其对氧氟沙星抗生素的降解性能

以钼酸钠以及五水合硝酸铋为原料,采用醇热法及高温退火制备了镂空Bi2MoO6微球光催化剂。采用X射线衍射(XRD)、红外光谱(FTIR)、场发射扫描电子显微镜(FESEM)、高分辨透射电镜(HRTEM)、物理吸附分析仪、紫外-可见漫反射(UV-Vis DRS)、荧光光谱分析(PL)以及电化学测试等分析方法分别对制备材料的晶体结构、微观形貌、比表面积和光学特性进行表征。以氧氟沙星(OFX)水溶液作为目标降解物,在可见光照射的条件下,探究了Bi2MoO6对OFX的光催化降解性能。实验结果表明:醇热法合成的球状钼酸铋的平均直径为500 nm,镂空结构使得球状Bi2MoO6的比表面积提高到片状Bi2MoO6的5倍。更大的比表面积为光催化提供了大量的吸附位点,在120 min的可见光辐射下,投放量为1 g·L^-1的Bi2MoO6对p H=7、浓度为10 mg·L^-1OFX水溶液的降解效率可达64%,而片状Bi2MoO6仅为31%。镂空球状的Bi2MoO6在强碱性环境具有优异的光催化效果,对OFX的降解率达到79%,在强碱性环境中,具有更优的光催化降解性能。     

增强可见光催化活性的Z型MoO3/Bi2O4复合光催化剂的制备（英文）

全球工业化进程的加快使人们饱受环境污染问题的困扰.半导体光催化技术作为一种高效、绿色、有潜力的新技术,在环境净化方面有着广阔的应用前景.Bi2O4是近年来新开发出的一种铋基光催化剂,在环境净化方面已有一些研究.但是,单体光催化剂通常存在光响应范围窄、光生载流子复合率高等问题,这些不足限制了Bi2O4的进一步应用.因此,需要通过适当的改性来拓宽其光响应范围和提高其载流子的分离效率,从而提高其光催化活性.构建Z型异质结被认为是提高光催化剂光生载流子分离效率并进一步提高光催化活性的有效方法.MoO3是一种宽禁带的n型半导体,具有独特的能带结构、光学特性和表面效应,是一种非常有前景的半导体光催化剂.虽然MoO3材料的光生载流子复合率高,带隙(2.7-3.2 eV)大,不利于其参与光催化反应,但MoO3与其他合适的半导体配位形成复合材料后能够有效提高其光生载流子的分离效率,从而提高其光催化活性.本研究采用简单的水热法制备了一种新型Z型MoO3/Bi2O4复合光催化剂,SEM和TEM分析结果表明,MoO3和Bi2O4紧密结合在一起.X射线光电子能谱分析表明,MoO3和Bi2O4之间存在很强的界面相互作用,这有助于电荷转移和光生载流子的分离.光致发光光谱、电阻抗和光电流测试也证明了MoO3/Bi2O4复合光催化剂的光生载流子分离效率更高,形成了更强的光电流.通过在可见光下降解RhB溶液评价了所合成光催化剂的光催化性能.15%MoO3/Bi2O4(15-MB)复合光催化剂表现出了最佳的可见光催化活性,在40 min内对10 mg/L RhB溶液的降解率达到了99.6%,其降解速率是Bi2O4的2倍.此外,15-MB复合光催化剂在经过五次循环降解RhB溶液后仍保持良好的光催化活性和稳定性,表明MoO3/Bi2O4复合光催化剂具有较强的应用潜力.通过自由基捕获实验确定了光催化反应中主要的活性自由基为 O2-和h+.通过莫特-肖特基测试和带隙计算得到MoO3和Bi2O4的价带和导带位置.最后,根据实验和分析结果提出了Z型MoO3/Bi2O4复合光催化剂在可见光下降解RhB溶液的机理.本研究为设计铋基Z型异质结光催化剂用于高效去除环境污染物提供了一种有前景的策略.     

探究超薄Bi2MoO6纳米片高效光催化CO2还原活性

铋系层状半导体材料凭借其独特的表面特性在光催化领域得到广泛的研究及应用,然而在光催化反应过程中光生电荷迁移及其表界面动态变化却鲜见报道。本文中,我们利用准原位X射线光电子能谱仪（QIS-XPS）系统研究超薄Bi2MoO6纳米片光催化CO2还原过程中光生电荷迁移及其表界面演变过程。研究结果表明：在暗态条件下CO2分子吸附于（010）暴露面Bi活性位,由于CO2分子强的拉电子能力,导致内层出现高价态Mo(6 x) 。当光照射至样品表面上时,*CO2峰显著降低,*CO峰明显升高,表明CO2分子在Bi活性位发生活化断键,并与光生电子反应形成*CO,使得高价态Mo(6 x) 含量增大。活性测试表明超薄Bi2MoO6纳米片的CO产量活性为41.8 ?mol g-1 h-1,其比块体Bi2MoO6活性高4.2倍,并且展现出优异的光催化稳定性。该工作为二维层状材料高效光催化CO2还原机理研究提供了一种全新的研究思路。     

β-Bi_2O_3/BiOI异质结的制备及其有效去除有机染料的光催化作用（英文）

窄带半导体氧化铋(Bi2O3,带宽介于2.1-2.8 e V)因其强的可见光吸收和无毒性等特性而一直被认为是潜在的可见光催化材料.通常,Bi2O3具有α,β,γ,δ,ε和ω等六种晶型,其中,α,β和δ-Bi2O3具有催化可见光降解有机物的活性.可是,由于其光生电子-空穴复合较快,Bi2O3的光催化活性还很低,远不够实际应用.将半导体与另一种物质如贵金属或其他半导体复合形成异质结是一种有效控制光生电子-空穴复合,提高光催化活性的方法.目前已成功开发了许多Bi2O3基的异质结光催化材料.尤其是通过用卤化氢酸与α-Bi2O3直接作用原位形成的α-Bi2O3与铋的卤氧化合物Bi OX(X=Cl,Br或I)的异质结在提高光催化活性和制备方面显示了优越性.然而,具有更强可见光吸收的β-Bi2O3(带宽约2.3 e V)与卤氧化合物的异质结光催化性能却鲜有报道.本文通过用HI原位处理β-Bi2O3形成β-Bi2O3/Bi OI异质结.该异质结表现较纯β-Bi2O3和Bi OI更高的降解甲基橙(MO)可见光催化活性.通过多晶X射线衍射(XRD)、紫外漫散射(UV-DRS)、扫描电镜、透射电镜(TEM)、X光电子能谱(XPS)和荧光(PL)等手段研究了β-Bi2O3/Bi OI异质结,并提出其高催化活性的机理.XRD结果显示,用HI原位处理β-Bi2O3可形成Bi OI相,并且随着HI使用量增加,混合物中的Bi OI相逐渐增多.HRTEM结果进一步表明,在混合物中的β-Bi2O3和Bi OI都是高度结晶态,且两相之间有很好的接触,从而有利于两相之间的电荷移动.根据UV-DRS和αhv=A(hv–Eg)n/2等公式,计算出了β-Bi2O3和Bi OI带隙分别为2.28和1.77 e V,以及两种半导体的导带和价带位置.β-Bi2O3的导带和价带位置分别为0.31和2.59 e V,而Bi OI的导带和价带位置分别为0.56和2.33 e V.这样两种半导体能带结构呈蜂窝状,显然不适合光生电子-空穴的分离.然而,XPS测定结果显示,β-Bi2O3和Bi OI相互接触形成异质结后,β-Bi2O3相的电子向Bi OI相发生了明显的移动.根据文献报道,当两种费米能级不同的半导体接触时,电子会从费米能级高的半导体移向费米能级低的半导体,直至建立新的费米能级.β-Bi2O3被报道是典型的n型半导体,其费米能级在上靠近其导带位置;而Bi OI是典型的p型半导体,其费米能级在下靠近其价带位置.基于此,我们提出了β-Bi2O3/Bi OI异质结高催化活性的机理.当β-Bi2O3与Bi OI形成异质结时,由于β-Bi2O3的费米能级较Bi OI的高,因而电子从β-Bi2O3转向Bi OI,直至新的费米能级形成.因此电子在两相之间移动导致了β-Bi2O3能带结构整体下移,以及Bi OI能带结构整体上移,使得新形成的Bi OI导带和价带位置高于β-Bi2O3的.当该异质结在可见光的照射下,光生电子将移至β-Bi2O3的导带,而空穴会移至Bi OI的价带,最终达到了光生电子-空穴分离的效果,产生高的光催化活性.PL测试也证实了β-Bi2O3/Bi OI异质结具有更长的光生电子-空穴寿命.     

离子交换法制备高光催化活性Bi2WO6@Bi2S3异质结纳米片

社会经济快速发展的同时, 也带来了日益严峻的环境污染问题. 半导体光催化氧化技术因节能环保而在环境领域有广阔的应用前景. 作为最具有代表性的半导体光催化材料, TiO2因为其禁带宽度(3.2 eV)比较大, 只能被紫外光激发, 因而对太阳能的利用率较低. 作为一种最简单的含铋层状氧化物, Bi2WO6的禁带宽度(2.7 eV)相对较小, 可以部分利用太阳光中的可见光, 因而受到广大研究者的青睐. 但是, Bi2WO6光催化材料的可见光响应范围较窄, 仅能被波长小于450 nm的光激发, 且激发后的光生载流子容易复合, 导致光催化效率不高. 因此, 迫切需要对Bi2WO6光催化材料进行结构修饰与改性,采用拓展其光响应范围和抑制载流子复合, 来提高其光催化活性.本文采用离子交换法原位合成了具有核-壳结构的Bi2S3@Bi2WO6纳米片, 充分利用Bi2S3优良的可见光响应性能和半导体异质结光催化剂的构建, 来提高Bi2WO6的光催化活性. 结果表明, 随着Na2S·9H2O用量从0增加到1.5 g, 所得催化剂的光活性不断提高, X3B的降解速率常数由0.40×10-3min-1增加到6.6×10-3min-1, 催化剂活性提高了16.5倍. 当进一步增加Na2S·9H2O的用量时(1.5-3.0 g), 复合催化剂的光活性下降. 这是由于过多Na2S·9H2O的引入导致在催化剂表面生成了没有光活性的NaBiS2层(Bi2S3+ Na2S = 2NaBiS2), 占据了催化剂的活性位点, 阻碍了染料分子与催化剂的直接接触. Bi2WO6@Bi2S3异质结纳米片光活性的提高, 可归因于Bi2S3的敏化作用极大拓展了复合催化剂的光响应范围; 另一方面, Bi2WO6和Bi2S3两者之间的半导体异质结效应有效促进了光生载流子在空间的有效分离, 抑制了光生电子-空穴的复合, 从而提高了复合催化剂的催化效率. 本研究为其他半导体复合材料的原位生长制备提供了新的思路.     

Fe~(3+)掺杂三维分级纳米Bi_2WO_6的合成及其光催化活性增强机理(英文)

利用水热法合成了Fe3+掺杂的三维分级纳米Bi2WO6,借助X射线衍射(XRD)、场发射扫描电镜(FE-SEM)、透射电镜(HRTEM)、能谱(EDS)、紫外可见漫反射(UV-Vis-DRS)等测试手段对所得样品的相组成、形貌和谱学特征进行了表征。选择罗丹明B为模型污染物研究所得样品在可见光下的催化活性。结果表明,Fe3+掺杂Bi2WO6为新颖的分级纳米结构,且Fe3+掺杂能有效提高Bi2WO6的光催化活性,Fe3+掺杂量对Bi2WO6活性的影响显著;实验结果还表明,所得Fe3+掺杂Bi2WO6催化剂的稳定性较好,易于回收。此外,还对Fe3+掺杂Bi2WO6的光催化活性增强机理进行了研究,缺电子的Fe3+作为电子捕获中心有利于促进光生电子-空穴对的分离,从而提高Bi2WO6的光催化活性。     

三元Ho3+-TiO2/Bi等离子体复合纤维制备及其可见光催化产氢性能

以电纺Ho³⁺-TiO₂纳米纤维为基质,葡萄糖酸钠为还原剂,采用水热法制备Ho³⁺-TiO₂/Bi等离子体复合纤维光催化剂。 利用X射线衍射(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、X射线光电子能谱(XPS)、紫外可见漫反射光谱(UV-Vis DRS)和瞬时光电流(IP)等分析测试手段对样品的物相、形貌和光电性能等进行表征。 以三乙醇胺为电子给体,研究了Ho³⁺-TiO₂/Bi光催化分解水产氢的反应过程。 结果表明:在水热过程中,Bi³⁺被葡萄糖酸钠还原成单质Bi纳米颗粒,复合在Ho³⁺-TiO₂纳米纤维表面形成肖特基结。 金属Bi通过局域表面等离子体共振效应结合稀土元素丰富的能级结构和4f电子跃迁特性,对TiO₂进行双重修饰改性,有效提高了TiO₂的光催化活性和稳定性,可见光下产氢速率最大为43.6 μmol/(g·h)。     

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.     

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.     

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.     

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.     

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.     

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。     

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。     

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.