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1.
La0.7-xGdxSr0.3MnO3中的相分离和输运行为   总被引:16,自引:6,他引:10  
研究了La0.7-xGdxSr0.3MnO3(x=0.00,0.10,0.15,0.20,0.30,0.40,0.50,0.60,0.70)体系的M-T曲线、M-H曲线、ESR曲线、ρ-T曲线和MR-T曲线。实验结果表明:随着Gd掺杂的增加,体系从长程铁磁有序向自旋团簇玻璃态和反铁磁状态转变,x=0.30和0.40时,样品在Tc以上温区发生相分离;高掺杂时的输运行为在其磁背景下发生异常,Gd掺杂引起的磁结构的变化将导致CMR效应。  相似文献   

2.
The expanding range of optoelectronic applications of lead-halide perovskites requires their production in diverse forms (single crystals, thin- and thick-films or even nanocrystals), motivating the development of diverse materials processing and deposition routes that are specifically suited for these structurally soft, low-melting semiconductors. Pressure-assisted deposition of compact pellets or thick-films are gaining popularity, necessitating studies on the pressure effects on the atomic structure and properties of the resulting material. Herein we report the phase transformation in bulk polycrystalline cesium lead bromide from its three-dimensional perovskite phase (γ-CsPbBr3) into the one-dimensional polymorph (δ-CsPbBr3) upon application of hydrostatic pressure (0.35 GPa). δ-CsPbBr3 is characterized by a wide bandgap of 2.9 eV and broadband yellow luminescence at 585 nm (2.1 eV) originating from self-trapped excitons. The formation of δ-CsPbBr3 was confirmed and characterized by Raman spectroscopy, 207Pb and 133Cs solid-state nuclear magnetic resonance, X-ray diffraction, absorption spectroscopy, and temperature-dependent and time-resolved photoluminescence spectroscopy. No such phase transition was observed in colloidal CsPbBr3 nanocrystals.  相似文献   

3.
Many theoretical and experimental efforts have been focused on the origin of the electric-pulse-induced resistance change effect. However, there are still various reports of the origin supporting either the bulk nature or the interface nature. To resolve the controversies, nanoscale electronic measurements may provide essential clues. In this work, we report microscopic electrical properties of Pr(0.7)Ca(0.3)MnO(3) thin films. The resistance of a single-crystalline grain is not homogeneous in nanometer scale. We deduce that nanoscale inhomogeneity is related to the periodic relaxation of substrate-induced strain, which is caused by the lattice mismatch between the substrate and the thin film.  相似文献   

4.
La0.7Ca0.3MnO3薄膜庞磁电阻(CMR)现象的分析   总被引:3,自引:0,他引:3  
针对La0.7Ca0.3MnO3薄膜材料中磁团簇的特性及其对材料庞磁电阻(CMR)现象的影响进行了研究。根据实验数据,利用Wagner等提出的数学模型,对La0.7Ca0.3MnO3薄膜中的磁团簇随温度的变化行为特性进行了研究;通过对La0.7Ca0.3MnO3薄膜相关实验数据的拟合,发现La0.7Ca0.3MnO3薄膜的居里温度范围应当在245~250K之间,从而进一步缩小了该材料居里温度的误差范围;还通过计算MR随磁团簇总角量子数J的变化,研究了制约和影响MR值的主要因素,发现磁团簇尺寸在La0.7Ca0.3MnO3薄膜的CMR现象中扮演了重要角色。  相似文献   

5.
Enhanced magnetoresistance in La0.7Sr0.3MnO3 nanoscaled granular composites   总被引:1,自引:0,他引:1  
By soft chemical processing, two kinds of nanoscaled lanthanum manganite granular composites, La0.7Sr0.3MnO3/CoFe2O4 (LSMO/CF) and La0.7Sr0.3MnO3 / Nd0.7Sr0.3MnO3 (LSMO/ NSMO), were fabricated. Enhancement in magnetoresistance is observed in both of the composites. Different magnetic compounds, CF and NSMO, embedded in LSMO matrix, result in different temperature ranges where the enhancement occurs. It is considered that the phenomenon is associated with electron tunneling between sorts of grains as well as spin-dependent scattering.  相似文献   

6.
(Pr0.7Sm0.3)0.7Ca0.3CoO3 belongs to a class of cobalt oxides undergoing a first-order transition (T* ≈90 K) associated to a coupled change in the valence and spin-state degrees of freedom. The Curie–Weiss regime present around room temperature (T >> T*) was analyzed in detail to address the controversial issue of the cobalt spin states above the transition. This magnetic investigation indicates that the Co4+ are in an intermediate spin-state, while the Co3+ are in a mixed state combining low-spin and high-spin states. These results are discussed with respect to the literature on related compounds and recent results of X-ray absorption spectroscopy.  相似文献   

7.
以甘氨酸和硝酸盐为原料,采用燃烧法制得陶瓷粉末,在马弗炉中焙烧2 h制备了钙钛矿型复合氧化物La0.3Ca0.7Ni0.7Co0.3O3,其结构经扫描电镜, XRD和IR表征.  相似文献   

8.
We report the fabrication of La(0.7)Ca(0.3)MnO(3) nanotubes (LCMONTs) with a diameter of about 200 nm, by a modified sol-gel method utilizing nanochannel alumina templates. High resolution transmission electron microscopy confirmed that the obtained LCMONTs are made up of nanoparticles (8-12 nm), which are randomly aligned in the wall of the nanotubes. The strong irreversibility between zero field cooling (ZFC) and field cooling (FC) magnetization curves as well as a cusplike peak in the ZFC curve gives strong support for surface spin glass behavior.  相似文献   

9.
10.
A series of high quality Bi3.15Nd0.85TiO3 (BNT) ferroelectric thin films and La0.7Ca0.3MnO3/Bi3.15Nd0.85TiO3 (LCMO/BNT) multiferroic composite thin films were deposited on Pt(111)/Ti/SiO2/Si(100) substrates by chemical solution deposition (CSD) method. The microstructure, surface morphology and leakage mechanisms of BNT and LCMO/BNT composite films were revealed by X-ray diffraction, scanning electron microscopy and semiconductor device analyzer, respectively. Ferroelectric behavior along with a remnant polarization (2Pr) of 20 μC/cm2, saturated magnetization around 56 emu/cm3 and magnetoelectric effect (ME) voltage coefficient αME of 33 mV/cm Oe at 1 kHz for LCMO/BNT composite films were obtained at room temperature, indicating that the coupling effects of electric and magnetic field exist in the fabricated LCMO/BNT multiferroic composite thin films. And our observations provide an effective way to manipulate the conduction behavior and push forward understanding the leakage mechanism in LCMO/BNT composite films.  相似文献   

11.
利用柠檬酸盐前驱物法制备了La2-xSmxCa2MnO7系列样品,并利用Rietveld方法对结构进行了精修.结果表明,体系中存在两个单相区(x≤0.8和x≥1.0)和一个两相区(O.8相似文献   

12.
13.
The crystal structure of Aurivillius phase ferroelectric Bi2WO6 has been studied in detail as a function of temperature by using high-resolution powder neutron diffraction. In agreement with an earlier study, a transition from space group P2(1)ab to B2cb occurs at about 660 degrees C. This transition corresponds to the loss of one octahedral tilt mode within the perovskite-like WO4 layer of the structure. A second, reconstructive, phase transition occurs around 960 degrees C, corresponding to the ferroelectric Curie point; in contrast to previous suggestions, the structure of this high-temperature phase contains layers of stoichiometry WO4, with WO6 octahedra sharing edges and corners, and with the fluorite-like Bi2O2 layers remaining essentially unchanged. This structure is closely related to that of the ambient temperature phase of lanthanide-doped derivatives, for example, Bi0.7Yb1.3WO6 recently reported. This phase-transition behaviour is in stark contrast to that of other members of the Aurivillius family, such as SrBi2Ta2O9 and Bi4Ti3O12, which retain the archetypal Aurivillius connectivity at all temperatures.  相似文献   

14.
The state diagrams (T-x) of the systems Ag2Te-ZnTe(I) and Ag2Te-Zn(II) are offered on the ground of data obtained by differential thermal analysis, X-ray phase analysis, microstructural analysis and measurements of the density and the microhardness of samples synthesized. The systems studied are quasibinary sections of the ternary system Ag-Zn-Te. System I is characterized by two eutectic and three eutectoidal non-variant equilibria as well as by an intermediate compound Ag2ZnTe2, which melts congruently at 880°C. The latter exists in the range from 120 to 880°C in two polymorphic modifications (Tʅ→β=515°C). System II is characterized by one eutectic, two eutectoidal and one peritectic nonvariant equilibria, boundary solid solutions on the ground of Ag2Te and Zn and one intermediate phase of the composition Ag4Zn3Te2, which melts congruently at 880°C.  相似文献   

15.
The study of trans- and cis-1,2-cyclohexanediol by infrared spectroscopy was performed. The variation of the maximum frequency and of the bandwidth of the OH stretching vibration give evidence of the role played by hydrogen bonding in the solid and liquid phases of both isomers and allows to follow the phase transitions. A solid rotator phase is shown for the cis compound.This revised version was published online in November 2005 with corrections to the Cover Date.  相似文献   

16.
Massive efforts have been devoted to designing molecular ferroic materials by molecular modification. For molecular ferroelastic, previous work is focused on the temperature-dependent ferroelastic domains, however, few are related to controlling the ferroelastic domain by the stress. Inspired by the “quasi-spherical theory” and fluorination effect, we designed a more flexible (MedabcoF)2+ (MedabcoF=1-fluoro-4-methyl-1,4-diazoniabicyclo[2.2.2]octane) cation by introducing a methyl group and a fluorine atom at the two symmetrical ends of the Dabco (1,4-diazoniabicyclo[2.2.2]octane) and synthesized a hybrid 3D perovskite (MedabcoF)Rb(BF4)3 ( 1 ) which displays three reversible phase transitions accompanying dual ferroelastic behavior. Besides, it not only exhibits ferroelastic domains switching by the thermal stimulation, and the sensitive reaction of in situ domains under the stress of it is also realized. This work not only achieves a force-controlled ferroelastic domain but develops a more profound comprehension of the relationship between the thermal motion behavior of guest cations and the intriguing properties of materials.  相似文献   

17.
La0.7-xDyxSr0.3MnO3(0.00≤x≤0.70)的TCR研究   总被引:2,自引:0,他引:2  
研究了La位Dy掺杂对La0.7-xDyxSr0.3MnO3(0.00≤x≤0.70)电阻温度系数(TCR)的影响.实验结果表明:Dy掺杂将引起电阻率曲线的急剧变化,导致出现大的TCR;随Dy掺杂的增加,TCR在x=0.30出现峰值,然后随掺杂量的增加逐步降低.体系出现大的TCR,来源于Dy掺杂引起的晶格畸变和额外磁性耦合.  相似文献   

18.
取代-3-甲酰色酮与(硫代)巴比妥酸的固相缩合反应   总被引:1,自引:0,他引:1  
刘锦贵  邓林  党珊 《合成化学》2008,16(1):93-95
在无溶剂无催化剂条件下,取代-3-甲酰色酮与(硫代)巴比妥酸通过固相Knoevenagel缩合反应合成了一系列5-(取代色酮基-3-亚甲基)(硫代)巴比妥酸,收率68.0%~85.5%,其结构经1H NMR确证.  相似文献   

19.
20.
Transformations of the nonequilibrium solid solution Re0.3Ir0.7 at increased pressure (1–10 GPa) and temperature (2000°C) have been studied. A phase transition from the hexagonal close-packed cell to the face-centered cubic cell without a loss of density and volume per atom has been detected.  相似文献   

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