NaTaO_3及NaTaO_3∶Bi~(3+)光催化剂的光致发光光谱研究

采用光致发光光谱技术对一系列不同条件下制备的NaTaO3及不同掺杂量的NaTaO3∶Bi3 进行了研究.结果表明,NaTaO3的发光性质与其制备条件密切相关在钠离子不足的条件下合成的样品,其发光带主要位于515和745nm左右;而在钠离子充足条件下合成的样品,其发光带位于460nm左右,随着n(Na)/n(Ta)的降低,发光带向长波长方向移动;掺入Bi3 之后,其发光峰由515nm移至455nm,随着Bi3 掺入量的增加,455nm的发光带强度减弱.515nm的发光带与替位缺陷Ta.N.a..相关;745nm的发光带与VN`a缺陷相关;而460nm的发光带与本征TaO6基团相关.将Bi3 掺入到钽酸钠样品,TaN..a..由BiN..a替代,相应的发光带向高的n(Na)/n(Ta)方向移动,从而呈现出本征TaO6基团的发光带.     

Growth and Spectral Properties of Yb^3＋-doped Ba3Gd（BO3）3 Crystal

Crystal of Yb3+-doped Ba3Gd(BO3)3 has been grown by the Czochralski method. The spectroscopic characterizations have been investigated at room temperature. The Yb3+:Ba3Gd(BO3)3 crystal exhibits broad absorption at 976nm with FWHM of 7nm and large overall spitting of 2F7/2 manifold (823cm-1). The absorption and emission cross sections are 5.09×10-21cm2 at 976nm and 0.97×10-21cm2 at 1040nm,respectively. The fluorescence lifetime is 2.84 ms.     

La(NO3)3和Pr(NO3)3对高岭石脱羟基动力学的影响

采用热重和微商热重(TG/DTA)综合热分析技术在不同升温速率下研究了掺入La(NO₃)₃和Pr(NO₃)₃的高岭石的热分解过程, 利用Coats-Redfern积分法和Achar微分法对热分析实验数据进行动力学计算, 得到了高岭石脱羟基反应过程中的控制机理函数、 活化能和指前因子等动力学参数; 分析了2种稀土掺入对高岭石脱羟基过程动力学参数的影响, 并用Ozawa法对活化能进行了验证. 结果表明, 未掺稀土和掺入Pr(NO₃)₃的高岭石的脱羟基反应过程均受化学反应模型F₃控制, 反应的活化能分别为307.94和282.86 kJ/mol, 指前因子lnA的值分别为47.8980和44.1718; 掺入La(NO₃)₃的高岭石脱羟基反应过程控制机理函数发生改变, 受化学反应模型F₂控制, 反应活化能为196.02 kJ/mol, 指前因子lnA的值为29.5551. 与未掺稀土的高岭石对比, 掺入Pr(NO₃)₃后活化能和指前因子略有降低; 而掺入La(NO₃)₃后则显著降低, 分别降低了36.34%和38.30%. 采用Ozawa法验证得到的活化能与Coats-Redfern积分法和Achar微分法结果一致.     

醋酸铅作为铅源合成CH3NH3PbBr3-xClx纳米晶体颗粒

Lead acetate, which is highly soluble in dimethylformamide, was used to synthesize mixed halide perovskite CH₃NH₃PbBr_3-xCl_x (MA = CH₃NH₃, 0 ≤ x ≤ 3) nanocrystals (NCs). This method provides an approach to address the low solubility of lead halides, especially lead chloride. Different Br/Cl ratios in MAPbBr_3-xCl_x lead to various optical properties. The photoluminescence emission peak can be tuned from 399 to 527 nm. Their full-widths at half-maxima (FWHM) are about 20 nm. MAPbBr_3-xCl_x NCs have an average diameter of ~(11 ± 3) nm and have uniform dispersion in toluene. The MAPbBr₃ NCs have a long average recombination lifetime (τ_ave = 97.4 ns) and a photoluminescence quantum yield (PLQY) of up to 73%.     

白光LED用荧光材料Ba3Gd（BO3）3∶Eu^（3＋）的发光性能研究

用高温固相反应法制备了稀土离子Eu^3＋掺杂的三元稀土硼酸盐Ba3Gd（BO3）3发光材料,通过X射线衍射（XRD）、荧光光谱和扫描电镜（SEM）等测试手段对Ba3Gd（BO3）3∶Eu^3＋荧光粉的制备条件、发光性能以及形貌进行了研究。XRD结果表明,在1000℃时可得到Ba3Gd（BO3）3纯相。扫描电镜照片显示颗粒基本为球形,粒径约为200-400 nm。发光光谱测试表明,Ba3Gd（BO3）3∶Eu^3＋荧光粉在近紫外区（UV）（396 nm）和蓝光区（466 nm）可以被有效地激发,分别用255和396 nm的紫外光激发样品时,以Eu3＋的5D0-7F2（611和616 nm）超灵敏跃迁为主要发射峰。当Eu3＋的掺杂浓度为10%（摩尔分数）时,Ba3Gd（BO3）3∶Eu3＋在611和616 nm处的发光强度最大。因此,这种荧光粉是一种可能应用在白光LED上的红色荧光材料。     

PbMg1/3Nb2/3O3 (PMN)和PbMg1/3Nb2/3-PbTiO3 (PMNT)中几种局域结构与晶格形变的从头算研究

建立了钙钛矿结构铌镁酸铅PbMg1/3Nb2/3O3(PMN)的2×2×3复晶胞模型; 采用ab initio方法讨论了PMN晶体各种可能构型的稳定性; 选取了PMN三种高、中、低稳定性的代表构型, 并对Ti替换B位离子后的结构进行了结构优化. 计算结果表明复晶胞刚性模型的最低和最高能量差约0.74 a.u. (1940 kJ); Pb2＋离子结构框架的形变是PMN晶格发生形变的主要因素; 在不考虑被替换离子电荷差异的情况下, MgO6含量越少越有利于Ti离子替换Nb与晶胞的形变. PMNT材料中构型的分布和局域形变取决于生长PMNT材料的工艺过程.     

Ca_4GdO(BO_3)_3:Eu~(3 ),Sm~(3 )的发光及离子间的能量转移

Ca4 RO( BO3 ) 3 ( R=La,Ln,Y)三硼酸盐具有优良的非线性特征 . Khamaganova等[1] 以Pb O作助熔剂在合成 Ca4 Sm2 ( BO3 ) 4的过程中发现了一种新相 ,经过结构分析判定是一种新的化合物 .Norrestam等通过高温固相反应合成出此类三硼酸盐 .Iiykhuin[2 ] 对 Ca4 RO( BO3 ) 3( R=Lu,Tb,Gd)的结构进行了研究 .Dirkse等 [3 ]报道了 Ca4 Gd O( BO3 ) 3 粉末的发光特性 .1 996年 ,Aka[4 ] 采用提拉法 ( Czochralski)首次生长出较大尺寸的 Ca4 Gd O( BO3 ) 3 单晶 .孟宪林等 [5]报道了 Ca4 YO( BO3 ) 3 :Nd晶体的激光发射和自倍…     

GdF3∶Er^3＋,Yb^3＋的合成和上转换发光特性

采用水热法制备了Er^3＋离子浓度为3%,Yb^3＋离子浓度分别为10%,20%的GdF3∶Er^3＋,Yb^3＋。XRD结果表明：合成的样品均为正交结构的GdF3,Gd0.87Yb0.10Er0.03F3和Gd0.77Yb0.20Er0.03F3样品的晶粒尺寸分别为28和26nm。研究了980nm红外光激发的上转换发射光谱。结果表明：红光和绿光发射分别来自于Er^3＋离子的2H11/2,4S3/2→4I15/2和4F9/2→4I15/2跃迁。样品的绿光发射强度较红光发射强。但绿光和红光发射的相对强度比例与Yb^3＋离子浓度有关。对Gd0.87Yb0.10Er0.03F3和Gd0.77Yb0.20Er0.03F3样品中可能的上转换发光机制进行了讨论。     

Ba_3Y(PO_4)_3∶Dy~(3+),Eu~(3+)单基质白光荧光粉的制备与发光性能

为了探究在Dy~(3+)掺杂Ba_3Y(PO_4)_3荧光粉中共掺Eu~(3+)离子对其发光性能的影响,我们采用传统高温固相法制备了一系列Dy~(3+)、Eu~(3+)单掺杂和共掺杂Ba_3Y(PO_4)_3荧光粉。通过X射线衍射(XRD)、荧光发射光谱和荧光衰减曲线对样品进行了表征。结果表明,所制备的荧光粉呈闪铋矿立方相。在近紫外光激发下,Ba_3Y(PO_4)_3∶Dy~(3+)发射光谱在487和578 nm处有两个窄带发射峰,呈冷白光发射;Ba_3Y(PO_4)_3∶Eu~(3+)发射光谱的窄带发射位于594和616 nm处,呈发橙红光。在Ba_3Y(PO_4)_3∶Dy~(3+),Eu~(3+)中,由于Eu~(3+)离子补偿Dy~(3+)冷白光发射所缺的红色组分,从而实现了色纯度高、色温适中的暖白光发射。进一步探索了Ba_3Y(PO_4)_3∶Dy~(3+),Eu~(3+)荧光粉发光机理。所制备的Ba_3Y(PO_4)_3∶Dy~(3+),Eu~(3+)单基质白光荧光粉在白光近紫外激发白光二极管(UVWLED)领域具有潜在应用价值。     

不同掺杂浓度Yb3+:YAl3 (BO3)4晶体光谱研究

采用顶部籽晶法生长了不同浓度Yb3+:YAl3(BO3)4(Yb:YAB)晶体,X射线粉末衍射(XRD)结果表明晶体的结构与YAB相同.研究了室温下不同掺杂浓度Yb:YAB晶体的偏振吸收光谱,以及块状的偏振荧光谱和粉末的非偏振荧光光谱,通过对不同浓度掺杂Yb:YAB晶体粉末的非偏振荧光谱的分析,实验结果表明:随着Yb3+离子掺杂浓度的增加,辐射陷阱效应对荧光谱的影响越来越严重;因此,提出了Yb:YAB晶体中荧光谱的重心波长移动与Yb3+离子掺杂浓度之间的经验关系来定量分析Yb3+离子掺杂浓度变化对辐射陷阱的影响.并且比较了不同浓度Yb:YAB晶体的光谱参数.结果表明高浓度Yb:YAB晶体是一种潜在的微片和自倍频激光材料.     

The Solgel Preparation and Electric Properties of MnO2-doped PbTiO3 Ceramics

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Application of the spectroscopic modifications of Pippard relations to NaNO2 in the ferroelectric phase

This study examines a linear variation of the specific heat C_P with the frequency shifts 1/ν(∂ν/∂T) for the Brillouin frequencies of the L-mode [010], [001] and [100] in the ferroelectric phase of NaNO₂ according to our spectroscopically modified Pippard relation. We obtain this linear relationship for those modes studied and calculate dT_C/dP in the ferroelectric phase of NaNO₂. Our calculated values of dT_C/dP for the [001] and [100] modes are in good agreement with the values given in the literature.     

钙钛矿铁电纳米片诱导的P (VDF-TrFE)取向生长

Ferroelectric polymers are particularly attractive for applications in flexible electronic devices, and controlling its crystalline phase growth is crucial for obtaining optimized ferroelectric properties. Herein we report that a very low introduction (0.2% (w)) of single-domain ferroelectric PbTiO₃ nanoplates can effectively mediate the nucleation and subsequent growth of a crystalline phase within P (VDF-TrFE) (denoted by PVTF), forming highly oriented films and significantly improving the ferroelectric properties due to an alignment of the polarization directions of the polymer and the nanoplates.     

Substrate-induced anisotropy of c-axis textured NaxCoO2 thin films

Na_xCoO₂ [x = 0.51, 0.54, and 0.59] thin films have been grown on SrTiO₃ (100)-oriented single crystals with a 5° vicinal cut towards [010] by pulsed laser deposition. We analysed the films by X-ray diffractometry, atomic force microscopy (AFM), and dc-transport measurements. X-ray diffraction patterns of the films show single phase and c-axis textured growth with the film plane closely aligned to the [001]-direction of 5° miscut SrTiO₃ (001) substrates. In addition to the structural analysis of these films we performed transport measurements along and perpendicular to the substrate tilt direction and determined the resistivity anisotropy as a function of temperature. The results enable the development of a strategy for the fabrication of Na_xCoO₂ based thermoelectric thin film devices.     

第一性原理计算钛酸铅A位掺杂对其负热膨胀性的影响

近年来,实验发现钛酸铅基材料具有负热膨胀性,且其热膨胀程度会受到掺杂元素的影响.目前所研究的A位掺杂体系中,仅Cd原子掺杂能使钛酸铅负热膨胀性增强.所以研究A位掺杂钛酸铅,比较Cd原子与其他原子在掺杂钛酸铅时化学键的异同,有助于深刻理解钛酸铅负热膨胀的本质.本文利用第一性原理,分别优化了Sr、Ba、Cd掺杂钛酸铅的晶格常数,计算了它们的态密度和电荷密度.结果表明Cd―O键的共价性强于Pb―O键,而Ba―O键和Sr―O键几乎呈离子性,Ba/Sr对Pb的替代削弱了化合物的共价性,降低了自发极化强度.与实验测量的热膨胀系数对比可以发现,A位原子与氧原子之间的共价性增强,化合物负热膨胀程度升高;若A位原子与氧原子之间的共价性削弱,负热膨胀程度降低.可见A位原子与氧原子之间的共价性影响了钛酸铅基化合物负热膨胀性.     

脉冲激光沉积制备SrSn1-xCoxO3外延薄膜的微结构表征及能带调控

钙钛矿结构SrSnO₃因其独特的介电和半导体性质而备受关注,通过掺杂可显著调控其电学、磁学性能,拓宽其应用范围。本研究在单晶SrTiO₃(001)衬底上通过脉冲激光方法外延生长了SrSn_1-xCo_xO₃ (x = 0, 0.16, 0.33, 0.5) (SSCO)薄膜,探究了Co含量对薄膜结晶性、微观结构、光学性能以及介电性能的影响。结果表明, SrSn_1-xCo_xO₃薄膜可在SrTiO₃(001)衬底上外延生长, Co掺杂不会导致薄膜结晶质量的劣化。薄膜表面形貌平整、致密,膜厚200 nm,表面粗糙度为0.44 nm。随薄膜中Co掺杂量增加,薄膜透过率从90%降至25%,光学带隙从4.24 eV降至2.44 eV。介电性能测试表明,掺杂薄膜在10⁶Hz时介电常数为70.1,比无掺杂SrSnO₃薄膜提高57%。室温时SSCO薄膜表面电阻率为172 MΩ,在1000℃范围内薄膜结构稳定。     

Hydrothermal Synthesis and Characterization of Per ovskite PbTiOs3Powders from Different Precursors

Perovskite-type of PbTiO₃ fine powders which are homogeneous in physic-chemical properties has been hydrothermally synthesized from the different precursors. The borderline reaction conditions, such as temperature and time, for the formation of PbTiO₃ were established and the effect of the precursor on the particle properties was investigated. As a precursor, Pb-Tialko-carbonate xerogel dispersed in 2-methoxyethanol was found to be effective for the synthesis of the PbTiO₃ powders with a lower agglomeration and a simple mode of particle-size.     

Influence of the size of doping ion on phase stability and oxygen permeability of SrCo0.8Fe0.2O3−δ oxide

The compounds of SrCo_0.8Fe_0.2O_3−δ (SCF) doped with Mg²⁺, Ca²⁺, Sr²⁺, Ba²⁺, Ti⁴⁺ and Zr⁴⁺ are synthesized by conventional solid-state reaction. The phase stabilities and oxygen permeabilites of these synthesized oxides are investigated. It is found that the doping Mg²⁺, Ca²⁺, Sr²⁺ and Ba²⁺ totally dissolve into the SCF unit cell, while SrTiO₃ and SrZrO₃ phases form when SCF is doped with Ti⁴⁺ and Zr⁴⁺, respectively. A possible mechanism of the doping behavior is proposed to interpret the structure transformation of the SCF unit cell. Phase stability increases directly with the size of the doping ion when SCF is doped with the ions in the same group. However, the influence of the size of the doping ion on the oxygen permeation behavior is negligible for the membranes doped with the ions in the same group.     

引入应力的锐钛矿TiO_2(001)薄膜的外延生长

锐钛矿TiO_2(001)(anataseTiO_2(001),简记为ATO)表面因其优异的催化活性受到了广泛的关注。理论计算结果表明,ATO表面应力导致的晶格畸变可能会增强该表面的催化活性。因此有必要研究应力对ATO表面结构的影响。本文利用BaTiO_3(001)(简记为BTO)与ATO之间存在较大的晶格失配度,将ATO薄膜外延生长在BTO衬底上从而引入应力,研究了存在应力情况下的ATO薄膜的结构特征。实验中,利用脉冲激光沉积方法在Nb掺杂的SrTi O_3(001)(简记为STO)单晶衬底上制备了ATO/BTO/STO外延薄膜。X射线衍射(XRD)和扫描透射电子显微术(STEM)结果表明,作为应力引入层的BTO薄膜厚度约为4–6nm时,能够部分地将应力引入到ATO薄膜中。X射线光电子能谱(XPS)结果显示,ATO薄膜合适的厚度应大于15 nm,从而降低从衬底反向扩散至表面的Sr和Ba原子的浓度;Ti 2p的高分辨XPS谱仅呈现出Ti~(4+)峰,表明ATO表面Ti原子为完全氧化的价态。ATO外延薄膜表面的扫描隧道显微术(STM)图像仍然呈现为(1×4)重构的结构,但在(1×4)重构的脊上存在明暗交替并具有一定周期性的特征。根据完全氧化的"增氧原子模型"(ad-oxygen model,AOM),脊上观察到的明暗交替特征可归因于表面应力导致的"TiO_2"空位缺陷结构。     

掺杂Eu2O3的SrTiO3及SnO2光致发光

用具有大能隙的本征半导体(SrTiO₃及SnO₂)粉末作本体,分别掺杂1%(原子百分数)的Eu₂O₃;所得物质表现出Eu³⁺离子的线发射光谱特性,但相对发光强度及光谱形状有相当大的变化。X射线衍射结构分析显示Eu³⁺在SrTiO₃晶格里是处在间隙位置,而它在SnO₂晶格里则形成新物相Eu₂Sn₂O₇。