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1.
以P123为模板,以钛酸四正丁酯、硝酸银和硫脲为原料采用模板法制备了一系列硫和银共掺杂介孔TiO2光催化材料.利用SEM、XRD、BET和紫外-可见光谱等技术对其形貌、晶体结构及表面结构、光吸收特性等进行了表征.以甲基橙溶液的光催化降解为模型反应,考察了不同掺杂量的样品在紫外和可见光下的光催化性能.结果表明,用模板法制备的共掺杂介孔TiO2光催化材料在紫外和可见光条件下较纯介孔TiO2和单掺杂介孔TiO2对甲基橙溶液具有更好的光催化降解效果, 且硫和银的掺杂量及样品焙烧温度显著影响该材料的催化性能.当硫掺杂量为2mol%和银掺杂量为1mol%,在500 oC 焙烧2 h所得光催化材料的催化性能最佳,4 h即可使甲基橙的降解率达98.8%,重复使用4次仍可使甲基橙的降解率保持在87.5%以上  相似文献   

2.
以棉花纤维为模板,以钛酸四正丁酯、硝酸铈铵和磷钨酸为原料采用模板法制备了一系列铈和磷钨酸共掺杂的、具有中空纤维结构的TiO2光催化材料, 利用扫描电子显微镜、X射线衍射、BET和紫外-可见光谱等技术对其形貌、晶体结构及表面结构、光吸收特性等进行了表征. 以苯酚溶液的光催化降解为模型反应,考察了不同掺杂量的样品在紫外和可见光下的光催化性能. 结果表明,用模板法制备的TiO2纤维材料具有中空结构,共掺杂的TiO2纤维在紫外和可见光条件下较纯TiO2纤维和单掺杂TiO2纤维对苯酚溶液具有更好的光催化降解效果, 且铈和磷钨酸的掺杂量显著影响该纤维材料的催化性能;当铈掺杂量为0.3mol%和磷钨酸掺杂量为2mol%,在500 oC焙烧2 h所得中空纤维材料的催化性能最佳,4 h即可使苯酚溶液的降解率达98.5%;重复使用4次仍可使苯酚溶液的降解率保持在87%以上,且该催化剂材料易于离心分离去除.  相似文献   

3.
以钛酸四正丁酯和硝酸镧为原料, 以P123为模板剂,采用模板法合成了La掺杂型介孔TiO2光催化剂, 借助TGA-DSC、BET、XRD及UV-Vis等测试手段对样品进行了表征,并以苯酚为模型污染物考察了镧掺杂量对样品光催化活性的影响.结果表明: La掺杂介孔TiO2光催化剂孔径分布较均匀(~10 nm),比表面积可达165 m2/g.与纯介孔TiO2相比,经掺杂改性后的样品在紫外光区及可见光区的吸收显著增强,对光具有更高的利用率,La掺杂可显著提高介孔TiO2的光催化活性.  相似文献   

4.
本文通过简单的溶剂热法制备了g-C3N4与高比表面积的TiO2复合材料,该方法操作简单且能耗低. 甲基橙降解实验结果表明,高比表面积的TiO2有效提高了光催化活性. 光电化学测试结果表明,与g-C3N4复合后,TiO2的电荷载流子迁移速率得到明显改善. g-C3N4/高比表面积-TiO2的光催化活性很强,在100分钟内,6%-g-C3N4/高比表面积-TiO2对甲基橙的降解程度可达92.44%. 6%-g-C3N4/高比表面积-TiO2不仅具有良好的光催化降解性能,还具有较高的稳定性. 本文对6%-g-C3N4/高比表面积-TiO2的光催化机理也进行了系统的研究.  相似文献   

5.
 冲击相变及冲击诱导化学反应可导致材料的物理、化学性能发生显著改变。采用炸药爆轰驱动飞片高速碰撞产生冲击波的方法,对富氮掺杂物双氰胺(C2N4H4)与P25 TiO2或偏钛酸(H2TiO3)的粉末混合物进行冲击加载,对回收产物进行X射线粉末衍射、透射电子显微镜、X光电子能谱、比表面积及紫外-可见漫反射光谱表征,通过亚甲基蓝和罗丹明B评价了回收产物的可见光催化降解活性。结果表明:以P25 TiO2为原料的冲击氮掺杂浓度可达8.88%,掺杂样品具有明显的可见光吸收,能带宽度减小到1.75 eV,样品中形成了少量Srilankite高压相;而以偏钛酸为原料的冲击氮掺杂浓度为3%~4%,能带宽度变化较小,但是由于其独特的冲击脱水膨胀机理,比表面积剧增。冲击氮掺杂样品对亚甲基蓝和罗丹明B染料有较好的吸附和可见光催化降解作用,其中高飞片速度处理的样品有更高的光催化降解活性。  相似文献   

6.
通过四苯基铁卟啉敏化Cr掺杂TiO2微球成功合成了一种复合改性可见光催化剂FeTPP-Cr-TiO2.利用XRD、FT-IR、SEM、XPS、UV-Vis和N2吸附-脱附等温线等技术对其结构和形貌进行了表征.以亚甲基蓝为目标降解物,在150 W氙灯的辐照下,考察了其可见光催化活性.结果表明FeTPP-Cr-TiO2呈锐钛矿相,表面积为74.7 m2/g.与Cr-TiO2和FeTPP-TiO2相比,FeTPP-Cr-TiO2表现出很好的可见光降解性能.以三种喹诺酮类抗生素(洛美沙星、诺氟沙星和氧氟沙星)为实验对象,考察了FeTPP-Cr-TiO2降解水体中抗生素的可行性,对三种抗生素均有很高的降解率,降解过程符合一级动力学模型,反应动力学常数分别为3.02×10-2、2.81×10-2和3.86×10-2min-1,半衰期为22.9、24.6及17.9 min.  相似文献   

7.
基于DFT+U方法,对镧掺杂锐钛矿TiO2及其氧空缺的稳定性以及对电子结构、光催化性质的性质进行了第一性原理研究.计算结果表明掺杂浓度和位置对结构稳定性的影响机制符合鲍林规则;结合晶体场理论和结构形变以及态密度的分析发现镧掺杂对带隙的调制不是通过掺杂带的引入,而是由结构形变决定.吸收光谱的模拟结果显示通过镧掺杂会提高可见光的吸收效率,和实验结果吻合.对氧空缺的后续研究表明氧空缺的存在会增强镧掺杂锐钛矿TiO2的稳定性,提高其光催化活性.  相似文献   

8.
用不同温度控制分解草酸氧钛铵制备N掺杂TiO2光催化剂.利用XRD、IR、热分析、N2吸-脱附等温线、XPS、紫外可见漫反射光谱和SEM表征了N-TiO2光催化剂的结构.400~600 oC焙烧的N-TiO2光催化剂为纯锐钛矿相,而700 oC焙烧的N-TiO2光催化剂为锐钛矿和金红石混合相.N掺杂在TiO2的间隙位使锐钛矿相TiO2带隙变窄.在光降解甲基橙的反应中,600和400 oC焙烧的N-TiO2催化剂分别在紫外光和全波长光照射下有最好活性;700 oC焙烧的N-TiO2催化剂无论在紫外光和全波长光下都表现出最好的比活性,即最高的光量子效率,这可以归因于700 oC焙烧的N-TiO2光催化剂良好的结晶程度和锐钛矿-金红石异相结的存在.  相似文献   

9.
本文采用微纳加工方法制备了负载高密度Ag-Cu纳米颗粒的N掺杂TiO2纳米棒阵列样品. 通过TiO2的N掺杂,可将其吸光范围调控至与Ag纳米颗粒的等离激元吸收频率相匹配的波段,从而实现复合材料中肖特基结与共振能量转移过程的协同作用. 与此同时,Cu纳米颗粒可以为CO2还原提供活性位点. 在全谱光照射下,复合样品光催化CO2还原的活性显著提高,CH4生成速率可达720 μmol·g-1·h-1.  相似文献   

10.
采用水热合成法,制备出Er掺杂的BiVO4复合光催化剂,并采用XRD、SEM、XPS和紫外-可见漫反射光谱技术对其进行分析表征.通过可见光下降解水溶液中甲基橙分子来考察其光催化性能,结果显示掺杂组份以氧化物Er2O3形式存在于的复合光催化剂中;且掺杂复合光催化剂的可见光吸收和催化活性都比纯BiVO4有所增强.  相似文献   

11.
Titanium dioxide (TiO2) nanoparticles co-doped with N and Fe were prepared via modified sol-gel process. The products were characterized by transmission electron microscopy (TEM), N2 adsorption, X-ray diffraction (XRD), Raman spectroscopy, UV-vis spectroscopy, photoluminescence (PL), and X-ray photoelectron spectroscopy (XPS). It is shown that the prepared TiO2 particles were less than 10 nm with narrow particle size distribution. The addition of MCM-41 caused the formation of Ti-O-Si bond which fixed the TiO2 on MCM-41 surface, thus restricted the agglomeration and growth of TiO2 particles. The photocatalytic performance in the degradation of methylene blue showed that N, Fe co-doped TiO2 exhibited much higher photocatalytic activity than doped sample with nitrogen or Fe3+ alone under both UV and visible light. N, Fe co-doping decreased the loss of doping N during the degradation reaction, thus increased the photocatalytic stability. It was also found that the nitridation time had significant influence on the photocatalytic activity of prepared TiO2 catalysts.  相似文献   

12.
Titanium dioxide photocatalysts co-doped with iron (III) and lanthanum were prepared by a facile sol-gel method. The structure of catalysts was characterized by X-ray diffraction (XRD), Raman spectroscopy, UV-vis diffuse reflectance spectroscopy and X-ray photoelectron spectroscopy (XPS). The photocatalytic activities of the samples were evaluated by the degradation of methylene blue in aqueous solutions under visible light (λ > 420 nm) and UV light irradiation. Doping with Fe3+ results in a lower anatase to rutile (A-R) phase transformation temperature for TiO2 particles, while doping with La3+ inhibits the A-R phase transformation, and co-doping samples indicate that Fe3+ partly counteracts the effect of La3+ on the A-R transformation property of TiO2. Fe-TiO2 has a long tail extending up the absorption edges to 600 nm, whereas La-TiO2 results in a red shift of the absorption. However, Fe and La have synergistic effect in the absorption of TiO2. Compared with Fe3+ and La3+ singly doped TiO2, the co-doped simple exhibits excellent visible light and UV light activity and the synergistic effect of Fe3+ and La3+ is responsible for improving the photocatalytic activity.  相似文献   

13.
The ferric ions in Fe(NO3)3·9H2O are connected in pairs by a screw dyad axis. When a magnetic field is applied, two neighbouring ions may have different energy splittings unless the field is applied parallel or perpendicular to the screw dyad axis. As a flip-flop process on the whole must be energy conserving, the spin-spin relaxation time depends on the angle between the field and the screw dyad axis. This effect is demonstrated by Mössbauer effect measurements on single crystals of Fe(NO3)3·9H2O.  相似文献   

14.
We discuss possible directions for searching for prospective materials based on low-valency uranium (III–V) as detection media for hard electromagnetic radiation. We have studied the processes of formation of tetravalent and pentavalent uranium complexes from UO2(NO3)3·6H2O and UO2Cl2·H2O in DMF and with addition of CCl4, including when the systems are exposed to radiation in the visible range (400–450 nm). In the first case (UO2(NO3)3·6H2O solutions in DMF), upon irradiation we observe stable complexes of pentavalent uranium, and when CCl4 is added to the solution we observe complexes of tetravalent uranium. In the system UO2Cl2·3H2O in DMF, we do not observe the appearance of new forms of uranium; but when CCl4 is added, then complexes of tetravalent uranium are formed. __________ Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 74, No. 2, pp. 184–187, March–April, 2007.  相似文献   

15.
Nickel hydroxides with hierarchical micro-nano structures are prepared by a facile homogeneous precipitation method with different nickel salts (Ni(NO3)2·6H2O, NiCl2·6H2O, and NiSO4·6H2O) as raw materials. The effect of nickel sources on the microstructure and lithium storage performance of the nickel hydroxides is studied. It is found that all the three prepared samples are α-nickel hydroxide. The nickel hydroxides synthesized with Ni(NO3)2·6H2 or NiCl2·6H2O show a similar particle size of 20–30 μm and are composed of very thin nano-sheets, while the nickel hydroxide synthesized with Ni(SO4)2·6H2O shows a larger particle size (30–50 μm) and consists of very thin nano-walls. When applied as anode materials for lithium-ion batteries (LIBs), the nickel hydroxide synthesized with NiSO4·6H2O exhibits the highest discharge capacity, but its cyclic stability is very poor. The nickel hydroxides synthesized with NiCl2·6H2O exhibit higher discharge capacity than the nickel hydroxides synthesized with Ni(NO3)2·6H2O, and both of them show much improved cyclic stability and rate capability as compared to the nickel hydroxide synthesized with Ni(SO4)2·6H2O. Moreover, pseudocapacitive behavior makes a great contribution to the electrochemical energy storage of the three samples. The discrepancies of lithium storage performance of the three samples are analyzed by ex-situ XRD, FT-IR, electrochemical impedance spectroscopy (EIS), and cyclic voltammetry (CV) tests.  相似文献   

16.
New type photocatalytic materials of Zn2+–Ni2+–Fe3+–CO32?LDHs were prepared by complexing agent-assisted homogeneous precipitation technique and Zn(NO3)2·6H2O, Ni(NO3)·6H2O, Fe(NO3)3·9H2O used as raw materials in the case of molar ratio of Zn2+/Ni2+/Fe3+ = 1:6:2. Zn2+–Ni2+–Fe3+–CO32?LDHs having a specific surface area of 96.5 m2/g. The structure and catalytic properties of the material were systematically studied. The experimental results show that the Zn2+–Ni2+–Fe3+–CO32?LDHs has a higher adsorption performance and lower band gap which make it an excellent catalyst for reducing the degradation of the methyl orange. Study on the process of photocatalytic reaction shows that Methyl Orange was adsorbed to the layer of Zn2+–Ni2+–Fe3+–CO32?LDHs, and then it was photodecomposed to inorganic molecules and ions by Zn2+, Ni2+, and Fe3+ on the surface of Zn2+–Ni2+–Fe3+–CO32?LDHs.  相似文献   

17.
王庆宝  张仲  徐锡金  吕英波  张芹 《物理学报》2015,64(1):17101-017101
采用基于密度泛函理论(DFT)的平面波超软赝势方法(PWPP), 利用Material studio 计算N, Fe, La三种元素掺杂引起的锐钛矿TiO2晶体结构、能带结构和态密度变化. 并通过溶胶-凝胶法制得锐钛矿型本征TiO2, N, Fe共掺杂TiO2和N, Fe, La共掺杂TiO2; 用X射线衍射和扫描电镜表征结构; 紫外-可见分光光度计检测TiO2对甲基橙的降解效率变化. 计算结果表明, 由于N, Fe, La三掺杂TiO2的晶格体积、键长等发生变化, 导致晶体对称性下降, 光生电子-空穴对有效分离, 同时在导带底和价带顶形成杂质能级, TiO2禁带宽度由1.78 eV变为1.35 eV, 减小25%, 光吸收带边红移, 态密度数增加, 电子跃迁概率提升, 光催化能力增加. 实验结果表明: 离子掺杂使颗粒变小, 粒径大小: 本征TiO2>N/Fe_TiO2>N/Fe/La_TiO2, 并测得N/Fe/La_TiO2发光峰425 nm, 能隙减小, 光催化能力比N/Fe_TiO2强, 增强原因是杂质能级和电子态数量增加引起.  相似文献   

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