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1.
采用水热合成方法,通过调控反应物中Ca2+与La3+的摩尔比可控合成了钙钛矿结构La1-x-yCaxKyMnO3(0.05≤x≤0.49;0.05≤y≤0.21)系列样品,利用X射线衍射仪、扫描电子显微镜、等离子光谱仪及磁性测量系统对样品的结构、形貌、成分组成和磁学性质进行了研究.结果表明,该水热反应过程为歧化反应,K+离子的引入导致了样品中双铁磁相的出现.  相似文献   

2.
应用偏靶射频磁控溅射方法在SrTiO3(001)单晶衬底上制备了三重价态(Mn3+, Mn4+, Mn5+)锰氧化物薄膜La1-x-yCaxKyMnO3. 这种薄膜具有钙钛矿结构, A位拥有La3+, Ca2+和K+三种离子, 对应的B位为Mn3+, Mn4+和Mn5+三重价态离子共存. 通过18 kW高能X射线衍射仪和D8 X射线面探衍射仪检测证实制备的薄膜为取向多晶薄膜. 原子力扫描图像显示薄膜表面平整, 且随薄膜厚度增加表面平整度起伏增大. 表面光电压测试显示, 该薄膜具有明显的光生电压信号.  相似文献   

3.
用固相反应法制备了La0.7-xSm,Sr0.3MnO3,La0.7-x,GdxSr0.3MnO3和La0.7-xDyxSr0.3MnO3(x=0.00,0.10,0.20,0.30)系列样品.通过M-T'曲线,ρ-T曲线,研究了用稀土离子代换La对La0.7Sr0.3MnO3磁电性质和磁电阻的影响.结果表明:稀土离子代换La引起的晶格畸变和稀土离子的额外磁性对钙钛矿锰氧化物的磁电性质影响很大;稀土离子代换La是改变钙钛矿锰氧化物居里温度和增强MR的有效途径;适量稀土离子代换La可以在室温附近产生大的磁电阻.  相似文献   

4.
为进一步弄清La3+离子对光合磷酸化及Hill反应影响作用机制,采用分光光度法,控制反应液中La3+离子浓度在0~20μmol.L-1范围,对纯化的游离态CF1-ATPase水解ATP活性测定结果表明:La3+离子对CF1-ATPase具有明显的促进作用。而且随La3+离子浓度增大,CF1-ATPase活性动力学曲线明显呈现"S"型。但当La3+离子浓度大于25μmol.L-1之后,La3+离子对游离态CF1-ATPase则表现出一定的抑制作用。而La3+离子浓度在0~30μmol.L-1范围内,受La3+离子作用类囊体膜CF1-ATPase活性动力学曲线则呈现双"S"形曲线。热稳定性实验结果表明:La3+离子可以降低CF1-ATPase活化能,提高CF1-ATPase的热稳定性。La3+离子对CF1-ATPase活性的影响可能与CF1-ATPase分子上别构位点有关,这也可能是La3+离子促进叶绿体Hill反应的关键部位。  相似文献   

5.
Ce1-xM′xCa0.2O1.8-0.4x (M=Y,La和Gd)   总被引:4,自引:0,他引:4  
采用水热法合成了系列双掺杂的萤石结构Ce1-xLnxCa0.2O1.8-0.4x固溶体, 并研究了3种稀土离子对固溶体导电性的影响, 发现掺杂离子半径接近Ce4+时, 体系电导率增大而活化能降低. 同时发现水热合成的Ce1-xLnxCa0.2O1.8-0.4x样品的平均粒度按着掺入离子Y3+, Gd3+, La3+的顺序逐渐减小, 分别为32, 20和15 nm. 这种变化是由于Y3+半径比La3+和Gd3+更接近Ce4+, 因而在水热合成过程中, 掺Y3+的体系更有利于晶粒的生长, 得到的晶体粒度较大.  相似文献   

6.
本文采用高温固相法合成了La1-xSrxYO3-α(x=0.00,0.05,0.10,0.15)系列陶瓷样品,用XRD、SEM对样品进行了表征,并用交流阻抗谱、氢泵、氢浓差电池、氧浓差电池等系统地研究了该系列样品的电性能.结果表明,该系列陶瓷样品均为钙钛矿型单斜晶相结构:样品的氢浓差电池电动势的实测值和理论值吻合得很好,表明样品在氢气气氛中为纯离子导体;氢泵测试结果证实了样品在氢气气氛中基本上是质子导体;氧分压与电导率的关系表明样品在高氧分压气氛中是离子(质子+氧离子)和空穴的混合导体.在低氧分压气氛中是离子(质子+氧离子)导体;氧浓差电池测试结果表明样品在干燥的氧化性气氛中是氧离子和空穴的混合导体.  相似文献   

7.
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.  相似文献   

8.
采用溶胶-凝胶法制备了系列多晶CMR材料La0.7Ca0.3Mn1-xCuxO3(x=0%,1%,5%,10%,15%,20%)。在77-350 K温度范围内测量了样品的电阻率及磁电阻大小。实验结果发现:系列样品TC随掺杂量增加而递减;系列样品的电阻率峰及磁电阻峰在整个测温范围内随掺杂量的增加均依次被展宽直至消失,当掺杂量为x≥10%时,电阻率随温度的变化在整个测温范围内呈现绝缘相行为;同时还发现,掺杂量为x≥10%时,样品的磁电阻在整个测温区内基本表现为隧穿磁电阻。基于我们采用蒙特卡罗模拟方法提出的逾渗模型及隧穿磁电阻模型,对样品的磁电阻行为进行了很好的解释。对系列样品的ρ-T曲线进行lnρ-T^-(1/4)系拟合,发现掺杂量为x=10%样品在整个温区内的lnρ-T^-(1/4)系基本呈线性。  相似文献   

9.
采用氨基多羧酸配合物法合成La2Ni1-yCoyO4+δ(y=0~0.2)超细粉料, 研究陶瓷样品的结构和混合导电性能. 研究结果表明, La2Ni1-yCoyO4+δ具有正交结构(Fmmm空间群), Co离子取代增加了钙钛矿层中ab平面上Ni/Co—O键的键长、岩盐层中沿c 轴方向上La—O键的键长和非化学计量氧含量, 并有利于改善材料的烧结性能. 随着Co离子含量的增加, 总电导率的峰值温度向高温移动, 高温段总电导率随温度的变化趋于平缓, 但总电导率水平出现降低; 增加Co离子含量还有利于提高氧离子导电性能. Co离子取代对陶瓷样品混合导电性能的影响与晶体结构参数的变化紧密相关.  相似文献   

10.
LaMnyCo1-yO3催化剂中氧状态的XPS研究   总被引:1,自引:0,他引:1  
钙铁石型稀土复合氧化物因其结构和性能的多样性,作为重要的功能材料(超导体、电极材料、光学材料、催化剂等)受到普遍重视[1]ABO3型稀土复合氧化物热稳定性高·文献[2-4]曾报导了La1-xCexCoO3、La1-xAx-Mno。、Lal。Sr。CoO。催化剂体系A位离子的偏析、价态和氧的非化学计量问题.本文是保持A位离子La不变,B位离子由Mn、Co组成的体系,通过B位离子组合来讨论过渡金属离子的电子组态导致氧状态变化对催化性能的影响.1实验部分(1)试剂:La(NO3h、Mn(NO3h、Co(NO小分析结(2)催化剂制备:按化学计量比混合溶液,用…  相似文献   

11.
用X射线衍射分析、FT-IR、小角X光散射等方法研究了浸渍法制备的NiO/SiO_2和NiO/(La_2O_3+SiO_2)样品中组分之间的相互作用。La_2O_3在SiO_2上可形成近乎密置单层的分散。在负载了La_2O_3的SiO_2上,NiO的分散程度比在SiO_2上有明显提高,也更容易被还原,而且还原后所得金属镍粒子的平均粒度降低,小粒子所占百分比提高。这些结果表明,NiO/(La_2O_3+SiO_2)比NiO/SiO_2样品具有更高的加氢还原硝基普鲁卡因为胺基普鲁卡因的活性,与Ni/(La_2O_3+SiO_2)比Ni/SiO_2活性高的情形相一致。  相似文献   

12.
潘勇  朱崇业  李全芝 《化学学报》1994,52(4):313-319
在不同条件下制备了一系列La~2O~3样品,以CH~4与CD~4间的氢原子交换反应作为测试反应来测量La~2O~3对CH~4分子中C-H键的断键能力.采用NH~3-TPD,CO~2-TPD和NH~3,CO~2对催化剂的中毒反应来研究La~2O~3表面的酸中心和活性中心.La~2O~3的表面组成用XPS测量.实验发现尽管酸中心在活性中心只占较小的部分. 但它与碱中心一样对于CH~4分子的C-H断键是必不可少的.本文提出, 组成活性中心的酸中心各碱中心很可能分别是一部分具有较强酸性的晶格La^3^+和具有较强碱性的晶格O^2^-,而La~2O~3晶体中晶格缺陷的形成能使更多的晶格离子成为活性中心.  相似文献   

13.
The preparation of ZnAlLa-hydrotalcite-like compounds [ZnAlLa-HTLcs] was studied.ZnAlLa-HTLcs were synthesized by a method of variable pH with the raw materials of Zn(NO3)2.Al(NO3)3, La(NO3)3, and NaOH. The effects of some factors (i.e. pH values, the mole ratio of Al^3- to La^3-.temperature and the period of hydrothermal treatment) on the preparation of HTLcs were discussed systematically. XRD. TG-DTA. FT-IR spectroscopy, and ICP were performed to characterize ZnAlLa-HTLcs samples, and the thermal stability of HTLcs was also discussed. It was shown that unique ZnAlLa-HTLcs with high crystallinity can be prepared, under the conditions of pH=5.5-6.5. n(Zn^2 )/n(Al^3 La^3 )=2 and the atomic ratio of La^3 to Al^3 ranging from 0.07 to 2. hydrothermal treatment at 120℃ for 5 h. When the calcination of the HTLcs is performed at temperatures above 200℃. ZnO phase is detected with Al2O3 and La2O3 spreading on its top. The complex metal oxides derived from ZnAlLa-HTLcs at 500℃ have higher catalytic activity and selectivity than those from ZnAl-HTLcs for the esterification of acetic acid with n-butanol under the same reaction conditions.  相似文献   

14.
In this paper we explore Gd(3+)-doped zeolite NaY nanoparticles for their potential application as a contrast agent in magnetic resonance imaging (MRI). The nanoparticles have an average size of 80-100 nm, as determined by TEM and XRD. A powdered sample loaded with La3+ was characterised by means of multinuclear solid-state NMR spectroscopy. The NMR dispersion (NMRD) profiles obtained from aqueous suspensions of samples with Gd3+ doping ratios of 1.3-5.4 wt% were obtaining at different temperatures. The relaxivity increases drastically as the Gd3+ loading decreases, with values ranging between 11.4 and 37.7 s-1 mM-1 at 60 MHz and 37 degrees C. EPR spectra of aqueous suspensions of the samples suggest that an interaction between neighbouring Gd3+ ions within the same particle produces a significant increase in the transversal electronic relaxation rates in samples with a high Gd3+ content. The experimental NMRD and EPR data are explained with the use of a model that considers the system as a concentrated aqueous solution of Gd3+ in the interior of the zeolite that is in exchange with the bulk water outside the zeolite. The results obtained indicate that the Gd3+ ion is immobilised in the interior of the zeolite and that the relaxivity is mainly limited by the relatively slow diffusion of water protons from the pores of the zeolite channels into the bulk water.  相似文献   

15.
The fluorescence spectra of Quin 2, (2-[(2-bis-[carboxymethyl] amino-5-methylphenoxy)methyl]-6-methoxy-8-bis [carboxymethyl] aminoquiniline), a Ca^2 probe, were investigated upon incubation with Ca^2 or La^3 . The results showed that binding of La^3 to Quin 2 resulted in different fluorescent spectrum from that of Ca^2 . Based on this observation, a fluorescent method was developed for simultaneously determination of the dissociation rates of Ca^2 and La^3 from a Ca-La- calmodulin complex (Ca2La2CaM).  相似文献   

16.
Multinuclear solid-state NMR spectroscopy and powder X-ray diffraction (XRD) experiments are applied to comprehensively characterize a series of pure and lanthanide-doped LaF3 nanoparticles (NPs) that are capped with di-n-octadectyldithiophosphate ligands (Ln3+ = diamagnetic Y3+ and Sc3+ and paramagnetic Yb3+ ions), as well as correlated bulk microcrystalline materials (LaF3, YF3, and ScF3). Solid-state 139La and 19F NMR spectroscopy of bulk LaF3 and the LaF3 NPs reveal that the inorganic core of the NP retains the LaF3 structure at the molecular level; however, inhomogeneous broadening of the NMR powder patterns arises from distributions of 139La and 19F NMR interactions, confirming a gradual change in the La and F site environments from the NP core to the surface. 139La and 19F NMR experiments also indicate that low levels (5 and 10 mol %) of Ln3+ doping do not significantly change the LaF3 structure in the NP core. Similar doping levels of paramagnetic Yb3+ ions severely broaden 19F resonances, but only marginally effect 139La powder patterns, suggesting that the dopant ions are uniformly distributed throughout the NP core and occupy vacant La sites. Measurements of 139La T1 and T2 relaxation constants are seen to vary between the bulk material and NPs and between samples with diamagnetic and paramagnetic dopants. 45Sc NMR experiments confirm that the dopants are integrated into the La sites of the LaF3 core. Solid-state 1H and 31P magic-angle spinning (MAS) NMR spectra aid in probing the nature of the capping ligands and their interactions at the NP surface. 31P cross-polarization (CP)/MAS NMR experiments identify not only the dithiophosphate head groups but also thiophosphate and phosphate species which may form during NP synthesis. Finally, 19F-31P CP/MAS and 1H MAS experiments confirm that ligands are coordinated to the NP surface.  相似文献   

17.
Cadmium, lead, copper and manganese were determined in human deciduous teeth and bone ash 1400 standard reference material by electrothermal atomic absorption spectrometry (ETAAS), using a lanthanum + palladium + citric acid (CA) modifier mixture. Optimum masses and mass ratios of La, La + Pd and La + Pd + CA modifiers for analytes in bone ash 1400 sample solution were investigated. Pyrolysis and atomization temperatures of analytes in a tooth sample solution were obtained with and without modifiers. The mixture of La + Pd + CA was found to be preferable for the determination of analytes in tooth samples and bone ash 1400, dissolved in a mixture of HNO3 + H2O2. The detection limits and characteristic masses of analytes were obtained with or without modifiers based on integrated absorbance for tooth sample solution (2% m/v). The detection limits obtained with La + Pd + CA are 6,24,16 and 46 ng g?1 for Cd, Cu, Mn and Pb, respectively. Recovery tests for analytes in bone ash 1400 and a tooth solution with La and La + Pd + CA modifier mixture were studied and compared with certified and non certified values. The La + Pd + CA mixture was also applied to the determination of Cd, Pb, Cu and Mn in tooth samples.  相似文献   

18.
通过高温固相法合成了一系列Sr3La2-xGe3O12:xSm^3+(0≤x≤0.04)红色荧光粉,并对样品的形貌、元素组成、晶体结构、发光性能及热稳定性进行了探究。结果表明:样品Sr3La2Ge3O12:xSm^3+为较宽尺寸分布的颗粒,且结构中仅含有Sr、La、Ge、O、Sm等元素。样品Sr3La1.97Ge3O12:0.03Sm^3+的Rietveld结构精修图与实测XRD图完全吻合,具有六方晶系结构。漫反射测试结果显示基质Sr3La2Ge3O12的带宽为5.54 eV,属于宽带隙材料。在404 nm激发下,样品Sr3La2-xGe3O12:xSm^3+(0≤x≤0.04)的最大发射峰位于601nm处,属于Sm^3+的6H5/2→4L13/2能级跃迁。此外,样品Sr3La1.97Ge3O12:0.03Sm^3+的发光性能最佳,其CIE色坐标为(0.5321,0.4601),色纯度高达94.2%,在298-473 K范围内具有较好的热稳定性,测试温度达到423 K时发射强度仍为室温时的81.6%。  相似文献   

19.
A study was initiated to investigate the chronological deposition of uranium in certain species of trees growing on the site of a former uranium metal processing facility. The Feed Materials Production Center (FMPC) is located in Fernald, Ohio, and for roughly 40 years operated as a large scale uranium processing center. Core samples from several species of trees growing in different locations throughout the site were extracted using a 12.5 mm incremental wood boring drill bit. After extraction, each core sample was cut and packaged into individual sections representing 4 annual growth rings and submitted for instrumental neutron activation analysis (INAA). The reaction 235U(n,f)140Ba→140La+γ was evaluated using high resolution germanium gamma-spectroscopy to detect the 1.596 MeV photon emission from the fission product 140La following a minimum of a 3 week decay. A total of 106 samples representing 7 individual trees of 3 unique species were irradiated. In addition to the tree-core samples, 18 quality control (QC) samples and 18 standard reference material (SRM) Fly Ash samples were irradiated with the core samples for determining neutron flux. The activity in any one sample in a batch was determined by comparison with the amount of natural uranium in the QC standards. No significantly measurable amount of uranium was detected in any of the tree core samples, although 3 tree core samples were in excess of the minimum detectable amount (30 ng).  相似文献   

20.
The La + O and La + O 2 chemiionization reactions have been investigated with quantum chemical methods. For La + O 2(X (3)Sigma g) and La + O 2(a (1)Delta g), the chemiionization reaction La + O 2 --> LaO 2 (+) + e (-) has been shown to be endothermic and does not contribute to the experimental chemielectron spectra. For the La + O 2(X (3)Sigma g) reaction conditions, chemielectrons are produced by La + O 2 --> LaO + O, followed by La + O --> LaO (+) + e (-). This is supported by the same chemielectron band, arising from La + O --> LaO (+) + e (-), being observed from both the La + O( (3)P) and La + O 2(X (3)Sigma g) reaction conditions. For La + O 2(a (1)Delta g), a chemielectron band with higher electron kinetic energy than that obtained from La + O 2(X (3)Sigma g) is observed. This is attributed to production of O( (1)D) from the reaction La + O 2(a (1)Delta g) --> LaO + O( (1)D), followed by chemiionization via the reaction La + O( (1)D) --> LaO (+) + e (-). Potential energy curves are computed for a number of states of LaO, LaO* and LaO (+) to establish mechanisms for the observed La + O --> LaO (+) + e (-) chemiionization reactions.  相似文献   

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