首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 31 毫秒
1.
Here we report the evidence of a disorder-to-order photo-induced phase transition (PIPT) under X-ray (h x = 12.4 keV) illumination in oxygen doped La 2 CuO 4 + i . The commensurate striped polaron crystalline phase is induced by the irradiation of X-rays in a cuprate perovskite at hole doping i ¨ 1/8 and high Cu-O micro-strain, k >7%. The nucleation of long range crystalline phases of holes on the oxygen 2 p x,y orbitals in the CuO 2 plane associated with pseudo Jahn Teller local lattice distortions (LLD) is favored by mobile counter-ions (interstitial oxygen ions in the La 2 O 2 layer) in the temperature range 200-350 K. The PIPT appears beyond a threshold dose of 10 17 photons/cm 2 at 220 K and a power law of the polaron crystal growth is observed as a function of the X-ray illumination dose.  相似文献   

2.
采用水热方法合成Ce1-x(Fe0.5 La0.5)xO2-δ固溶体.利用X射线衍射技术(X-ray diffraction technique,XRD)表征样品的相结构,并对固溶体的晶胞参数进行拟合,通过紫外可见漫反射光谱(UV-Vis diffraction spectrum)及拉曼光谱(Raman spectru...  相似文献   

3.
采用磁控溅射的方法在Si基片上制备了La0.85Sr0.015MnO3-δ/Fe异质结构,对所制备结构中La0.85Sr0.015MnO3-δ薄膜的输运及光诱导特性进行了分析,表明薄膜在整个测量的温度区间内呈现金属一半导体相变,相变温度为130K.在低温金属相,磁场作用导致电阻减小,而高温半导体相则使电阻增大;激光辐照导致样品电阻减小,并产生瞬间光电导效应,即随着激光的关闭电阻瞬间恢复到原值,其相对变化值随着温度的降低而增大,并在温度为80K时达到极大值约1660%,分析认为该瞬态光电导效应可能与薄膜本身的氧缺陷有关.  相似文献   

4.
我们用传统的固相反应法制备了(La0.7Ca0.3MnO3)1-x(MgAl2O4)x复合样品.通过XRD分析发现在此系列复合样品中La0.7Ca0.3MnO3和MgAl2O4两相共存;电阻率温度关系分析表明MgAl2O4的引入没有改变母体相在温度TP1处本征的金属-绝缘体转变峰,但使复合样品在较低温度TP2处出现另外一个电阻率峰值.有趣的是,随着MgAl2O4掺量的增加,在低掺量时,TP2向低温偏移很快;但在高掺量时,TP2向低温偏移较慢.  相似文献   

5.
Superconductivity below 0.3 K and a charge-density-wave-like(CDW-like) anomaly at 280 K were observed in EuBiS_2F recently.Here we report a systematic study of structural and transport properties in Eu_(0.5)Ln_(0.5)BiS_2F(Ln=La,Ce,Pr,Nd,Sm) by electrical resistivity,magnetization,and specific heat measurements.The lattice constants have a significant change upon rare earth substitution for Eu,suggesting an effective doping.As Ln is changed from Sm to La,the superconducting transition temperature T_c increases from 1.55 K to 2.8 K.In contrast to the metallic parent compound,the temperature dependence of electrical resistivity displays semiconductinglike behavior for all the Eu_(0.5)Ln_(0.5)BiS_2F samples.Meanwhile,the CDW-like anomaly observed in EuBiS2F is completely suppressed.Unlike the mixed valence state in the undoped compound,Eu ions in these rareearth-doped samples are mainly divalent.A specific anomaly at 1.3 K resembling that in EuBiS2F suggests the coexistence of superconductivity and spin glass state for Eu_(0.5)La_(0.5)BiS_2F.Coexistence of ferromagnetic order and superconductivity is found below 2.2 K in Eu_(0.5)Ce_(0.5)BiS_2F samples.Our results supplies a rich diagram showing that many interesting properties can be induced in BiS_2-based compounds.  相似文献   

6.
以钛酸四丁酯为原料,采用溶胶-微波法(Sol-Microwave Method)合成了镧和铈共掺型纳米TiO2粉体(La-Ce-TiO2),借助XRD、XPS和UV-Vis等测试手段对其进行了表征,并以甲基橙为模型污染物考察了掺杂量对样品光催化活性的影响规律.XRD分析表明,所得粉体均为锐钛矿相纳米TiO2,且稀土元素镧和铈掺杂后纳米TiO2特征衍射峰宽化,强度降低;XPS分析表明,镧和铈掺杂后样品表面存在大量的氧缺位;UV-Vis吸收光谱表明,所得粉体在400 nm以下均有连续宽化的吸收带,且La和Ce掺杂后样品对光的吸收显著增强,这足由于La(Ⅲ)-O荷移跃迁以及Ce(Ⅳ)f→d跃迁和Ce(Ⅳ)-O荷移跃迁所致;光催化实验表明,La和Ce共掺杂能显著提高纳米TiO2的光催化活性,其中当La(Ⅲ)和Ce(Ⅳ)掺杂量分别为2%和0.04%时,纳米TiO2光催化剂具有较高的催化活性,自然光照射下光催化氧化处理卷烟厂蒸叶车间废水,效果较好,废水COD去除率达到86.11%.  相似文献   

7.
使用牛津震动样品磁强计 (VSM)研究了Bi2 Sr2 CaCu2 O8单晶的磁滞回线 .在 2 0到 40K温度之间发现了反常的尖锋效应 ,随样品O含量的增加 ,发生尖锋效应的外场也相应提高 .可以认为在尖峰效应处发生了由涡漩物质的有序固态到无序固态的相变 ,在有少量点缺陷存在的BSCCO单晶相图上 ,Bsp线终止于 2 0K温度处 ,在 2 0K以下温区没有发生准格子到涡漩玻璃的相变 ,涡漩固相始终以准格子形式存在 ;可以认为尖峰效应是外场、温度、无序的复杂函数  相似文献   

8.
A powder X-ray diffraction study, combined with magnetic susceptibility and electric transport measurements, was performed on a series of LnCoO3 perovskites (Ln = Y, Dy, Gd, Sm, Nd, Pr and La) over a temperature range 100–1000 K. A non-standard temperature dependence of the observed thermal expansion was modelled as a sum of three contributions: (1) weighted sum of lattice expansions of the cobaltite in the diamagnetic low spin state and in the intermediate (IS) or high (HS) spin state. (2) An anomalous expansion due to the increasing population of excited (IS or HS) states of Co3+ ions over the course of the diamagnetic-paramagnetic transition. (3) An anomalous expansion due to excitations of Co3+ ions to another paramagnetic state accompanied by an insulator-metal transition. The anomalous expansion is governed by parameters that are found to vary linearly with the Ln ionic radius. In the case of the first magnetic transition it is the energy splitting E between the ground low spin state and the excited state, presumably the intermediate spin state. The energy splitting E, determined by a fit to magnetic susceptibility, decreases with temperature. The values of E determined for LaCoO3 and YCoO3 at T=0 K are 164 K and 2875 K respectively, which fall to zero at T=230 K for LaCoO3 and 860 K for YCoO3. The second anomalous expansion connected with a simultaneous magnetic and insulator-metal transition is characterized by its center at T=535 K for LaCoO3 and 800 K for YCoO3. The change of the unit cell volume during each transition is independent of the Ln cation and is about 1% in both cases.  相似文献   

9.
PEG-Na2SO4-PAR体系中Pd(Ⅱ)、U(Ⅵ)、Mo(Ⅵ)的萃取分离   总被引:5,自引:0,他引:5  
本文研究了在聚乙二醇-2000(PEG)-硫酸钠(Na2SO4)-4-(2-吡啶偶氮)-间苯二酚(PAR)体系中,Pd(Ⅱ)、U(Ⅵ)、La(Ⅲ)、Mo(Ⅵ)的萃取行为。实验结果表明,在pH4.5 ̄7.5溶液中,Pd(Ⅱ)、U(Ⅵ)、可被PEG相几乎完全萃取,La(Ⅲ)部分被萃取,而Mo(Ⅵ)则不被蔺取,从而实现了Mo(Ⅵ)与Pd(Ⅱ)、U(Ⅵ)混合离子间的定量分离,并初步探讨了PEG相的萃取机理  相似文献   

10.
合成了以稀土离子Sm3+、Eu3+、Tb3+、Dy3+及Tb3+为发光中心,以苯氧乙酸(HPOA)和邻菲罗啉(phen)为配体,掺杂La3+、Gd3+、 Y3+的7种稀土配合物, 对配合物进行了C、H、N元素分析、稀土络合滴定、红外光谱、紫外光谱和发光光谱的研究。结果表明配合物的组成分别为SmL3L'·1/2H2O,EuL3L'·1/2H2O,TbL3L'· 1/2H2O,DyL3L'·1/2H2O,掺杂配合物组成分别为Tb0.5Gd0.5L3L'·1/2H2O,Tb0.5Y0.5L3L'·1/2H2O,Tb0.5La0.5L3L'·1/2H2O(L=C6H5OCH2COO-, L'=phen)。配合物中的稀土离子与苯氧乙酸中羧基的一个氧原子和苯氧基的氧原子配位,与邻菲罗啉中的两个氮原子配位成键;荧光光谱表明,铽三元配合物的发射强度要远大于其它三元配合物的发光强度,掺杂发光惰性稀土离子La3+、Gd3+、Y3+的铽配合物中,Y3+掺杂配合物的发光强度有所增强。  相似文献   

11.
Infinite-layer-type superconductors Sr1−xLnxCuO2 are synthesized under high pressure of 3 GPa for Ln=Sm, Gd as well as for Ln=La, Nd. Their chemical and superconducting properties are systematically studied as functions of doping concentration and the kind of lanthanide ion. As a result, it is demonstrated that the variation of these properties with doping concentration is similar for all the examined Ln3+ ions. The solubility limit lies at x ≈ 0.10. CuO2 sheets are expanded with increasing x, while their spacing decreases. The Tc onset determined by magnetic measurements remains constant for any doping concentration; only the Meissner fraction increases with increasing x.  相似文献   

12.
刘胜利  厉建峥  程杰  王海云  李永涛  张红光  李兴鳌 《物理学报》2015,64(20):207103-207103
利用固相反应法成功制备了Sr2-xLaxIrO4系列掺杂样品, 并详细研究了样品晶体结构随掺杂的演变. 拉曼散射峰向高频移动和X射线衍射谱的结构精修数据发现随着掺杂量的增加, c轴晶格常数减小, 顶角Ir–O1键键长随之减小, 表明掺杂导致晶格收缩, 而且IrO6八面体畸变程度减弱. 变温拉曼散射谱显示随着温度降低也出现蓝移现象, 且与顶角氧相关的拉曼振动模式的蓝移在110 K附近出现明显跳变, 表明在该温度附近出现了结构变化和磁性质转变.  相似文献   

13.
The gamma-->alpha isostructural transition in the Ce0.9-xLaxTh0.1 system is measured as a function of La alloying using specific heat, magnetic susceptibility, resistivity, thermal expansivity or striction measurements. A line of discontinuous transitions, as indicated by the change in volume, decreases exponentially from 118 K to close to 0 K with increasing La doping, and the transition changes from being first-order to continuous at a critical concentration, x(c) approximately 0.14. At the tricritical point, the coefficient of the linear T term in the specific heat gamma and the magnetic susceptibility increase rapidly near x(c) and approach large values at x=0.35 signifying that a heavy Fermi-liquid state evolves at large doping. The Wilson ratio reaches a value above 2 for a narrow range of concentrations near x(c), where the specific heat and susceptibility vary most rapidly with the doping concentration.  相似文献   

14.
掺Sb纳米ZnO的光致发光的研究   总被引:2,自引:1,他引:1  
用柠檬酸盐法合成了不同掺杂浓度的纳米ZnO,粒径约为15nm。探讨了Sb掺杂对ZnO光致发光峰的影响。随着掺杂量的提高,样品的发射峰从428nm移至444nm。未掺杂ZnO的发光主要是源于电子从锌填隙形成的缺陷能级到价带顶的跃迁;随着掺杂量的提高,体系的氧空位增加,从而使得电子从氧空位所形成的缺陷能级到价带顶的跃迁占据主导,光致发射峰向长波方向移动。  相似文献   

15.
Magnetic phase transitions in disordered crystalline iron germanates of the type Sr2LnFe3Ge3O14 (Ln=La; Nd) were observed at low temperatures by means of57Fe Mössbauer spectroscopy. The hyperfine interaction of Fe3+ magnetic moments ordered in one octahedral and two tetrahedral magnetic sublattices is discussed. A local environment computation on the octahedral sites confirms the assumption that the wide distribution found for the 4.2 K octahedral hyperfine fields is due to the random occupation by Fe3+ and Ge4+ ions of the nearest cation environment of the octahedral iron. The effect of substituting Ln rare earth ions in the Thompson cubes on the magnetic behaviour of these compounds is pointed out.  相似文献   

16.
Only 3% hole doping by Li is sufficient to suppress the long-range three-dimensional (3D) antiferromagnetic order in La2CuO4. The spin dynamics of such a 2D spin liquid state at T相似文献   

17.
The electron-stimulated desorption (ESD) yields and energy distributions for potassium (K) and cesium (Cs) atoms have been measured from K and Cs layers adsorbed at 300 K on oxidized molybdenum surfaces with various degrees of oxidation. The measurements were carried out using a time-of-flight method and surface ionization detector. The ESD appearance threshold for K and Cs atoms is independent of the molybdenum oxidation state and is close to the oxygen 2s level ionization energy of 25 eV. Additional thresholds for both K and Cs atoms are observed at about 40 and 70 eV in ESD from layers adsorbed on an oxygen monolayer-covered molybdenum surface; they are associated with resonance processes involving Mo 4p and 4s excitations. The ESD energy distributions for K and Cs atoms consist of single peaks. The most probable kinetic energy of atoms decreases in going from cesium to potassium and with increasing adsorbed metal concentration; it lies in the energy range around 0.35 eV. The K and Cs atom ESD energy distributions from adlayers on an oxygen monolayer-covered molybdenum surface are extended toward very low kinetic energies. The data can be interpreted by means of the Auger stimulated desorption model, in which neutralization of adsorbed alkali-metal ions occurs after filling of holes created by incident electrons in the O 2s, Mo 4s or Mo 4p levels.  相似文献   

18.
樊永年  叶恒强 《物理学报》1986,35(5):672-676
用能量为一千电子伏,束流为6微安的氮离子轰击钼(111)表面15分钟,在俄歇能谱中出现很强的氮的俄歇峰。从室温至450℃退火低能电子衍射观察表明,表面是无序层。样品加热到562℃左右观察到正方的低能衍射图,可以解释为氮、氧在钼(433)小面的c(3×1)结构。 关键词:  相似文献   

19.
Magnetization and ac-susceptibility measurements are used to characterize the mixed phase of the high-temperature cuprate superconductor La2-xSrxCuO4 over a large range of doping (0.075 0.20). The first order vortex lattice phase transition line HFOT(T), the upper critical field Hc2(T) and the second peak Hsp(T) have been investigated up to high magnetic fields (8 Tesla applied perpendicular to the CuO2 planes). Our results reveal a strong doping dependence of the magnetic phase diagram, which can mainly be explained by the increasing anisotropy with underdoping. Within our interpretation, the first order vortex lattice phase transition is due to the sublimation (rather than melting) of the vortex lattice into a gas of pancake vortices, whereas the second peak is related to the transition to a more disordered vortex glass state.  相似文献   

20.
A magnesium–nickel (Mg–Ni) film with a palladium (Pd) overcoat is switchable between a conducting metallic state and a semiconducting state through hydridation and dehydridation processes. The Pd overcoat is added to suppress possible oxidation of the alloy layer. However, some Pd and oxygen (O) atoms are still able to diffuse into the alloy layer, such that the distributions of elemental and phase compositions along the direction of depth are quite complicated. In this work, we propose a method to obtain more detailed information on the elemental and phase compositions in a Pd/Mg–Ni film by means of analyzing Pd 3d5/2, Pd 3p3/2, Ni 2p3/2, Mg 1s and O 1s photoelectron spectra. The method was applied to analyze a typical Pd/Mg–Ni film sample. Results verified that Pd can diffuse into the alloy layer. An Mg–O phase is formed near the surface. An Mg–Ni alloy phase dominates at deeper regions. The Mg–Ni phase contains 80% of the total number of atoms in the film, and is non-stoichiometric and highly disordered. Nevertheless, it can give a remarkable change of electrical resistivity during hydridation–dehydridation processes. PACS 79.60.-i; 61.05.C-; 79.60.Ht  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号