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1.
晶界对庞磁电阻颗粒薄膜的磁学和输运性能的影响   总被引:1,自引:0,他引:1       下载免费PDF全文
采用脉冲电子束沉积技术,在Si(100)单晶衬底上沉积庞磁电阻La0.67Ca0.33MnO3颗粒薄膜,并对它的磁学性能和电学输运性能进行了表征.研究晶界对庞磁电阻薄膜的物理性能的影响,结果表明,晶界的存在使得晶粒之间的耦合变弱,在变温磁化过程中表现出团簇玻璃态行为,金属—绝缘体转变温度(Tp)远远低于铁磁—顺磁转变温度(Tc).低温下电子输运具有弱局域化行为.在低磁场下,晶界的存在掩盖了La0.67Ca0.33MnO3的本征磁电阻行为. 关键词: 脉冲电子束沉积 晶界 磁学和电学输运性能 庞磁电阻  相似文献   

2.
一种新的庞磁电阻氧化物薄膜La1-xPrxMnO3(x=0.1,0.2)薄膜用脉冲激光沉积(PLD)方法生长在(100)SrTiO3单晶基底上.XRD结果显示薄膜具有很好的外延单晶取向.电输运和磁性质的研究表明薄膜具有显著的庞磁电阻效应(CMR)效应,其中磁电阻比率达95%(在5T的磁场下).X射线光电子能谱(XPS)的结果表明薄膜体系中Pr离子的价态为+4价,因此该薄膜很可能是电子掺杂的庞磁电阻体系.  相似文献   

3.
常雷  蒋毅坚 《物理学报》2009,58(3):1997-2001
利用脉冲激光沉积技术在LaAlO3(00l)单晶衬底上制备了La067Ba033MnO3薄膜,研究了CO2激光辐照对La067Ba033MnO3薄膜的微结构和磁电性能的影响.结果表明,经激光辐照后,La067Ba033MnO3薄膜的结晶性增强,薄膜应变减小;薄膜表面形貌由“岛状”结构变为“平原"结构,且粗糙度大大降低;同时,薄膜的饱和磁化强度、铁磁居里温度、金属—绝缘态转变温度和磁电阻增大,而矫顽场和电阻率减小.根据对传统退火效应的分析和理论计算,认为激光辐照导致的表面微结构的变化以及薄膜的氧含量和均匀性的提高对La067Ba033MnO3薄膜的磁电性能的改善与优化密切相关. 关键词: 庞磁电阻 激光辐照 脉冲激光溅射沉积  相似文献   

4.
钙钛矿结构La0.9Sb0.1MnO3的庞磁电阻性质   总被引:12,自引:7,他引:5       下载免费PDF全文
一种新的钙钛矿结构的庞磁电阻氧化物La0.9Sb0.1MnO3已用固态反应方法制 成,通过超导量子干涉器件(SQUID)装置测量研究了它的电输运性质和磁性质.x射线光电子 能谱分析证明,该氧化物中Sb的价态是+5价,因此该氧化物是一种新的电子掺杂型庞磁电阻 材料. 关键词: 钙钛矿结构 0.9Sb0.1MnO3')" href="#">La0.9Sb0.1MnO3 电子掺杂 庞磁电阻  相似文献   

5.
朱丹丹  章晓中  薛庆忠 《物理学报》2003,52(12):3181-3185
利用脉冲激光沉积方法在Si(100)上制备了Cox-C1-x颗粒膜,并研 究了其正磁电阻 效应.实验结果表明,样品在室温下的正磁电阻效应要远远高于低温下的正磁电阻效应;Co 0.02-C0.98样品具有最大的室温正磁电阻效应,在外加磁场B=1T时 ,其磁电阻 率MR=22%;随着Co含量的增加,Cox-C1-x颗粒膜的正磁电阻效应呈 减小趋势.样品 的MR-B的曲线与传统的多 关键词: 正磁电阻效应 x-C1-x颗粒膜')" href="#">Cox-C1-x颗粒膜 脉冲激光沉积  相似文献   

6.
李廷先  张铭  王光明  郭宏瑞  李扩社  严辉 《物理学报》2011,60(8):87501-087501
使用脉冲激光沉积技术,在LaAlO3(001)单晶基片上制备了La2/3Sr1/3MnO3(LSMO)/BaTiO3(BTO)双层薄膜.X射线衍射分析显示,LSMO层和BTO层呈现纯(001)取向.原子力显微镜研究表明,薄膜表面晶粒大小均匀,排列致密,表面均方根粗糙度为1.4 nm.复合薄膜的磁学、电学性能研究表明,其具有良好的磁学和介电性能.电输运测试显示,与在BTO层上施加正方向 关键词: 磁电效应 铁电/铁磁异质结构 脉冲激光沉积  相似文献   

7.
用脉冲激光沉积法制备了非金属Te掺杂的钙钛矿锰氧化物La0.82Te0.18MnO3单晶薄膜.该薄膜从83 K升温至373 K过程中发生金属-绝缘体相变,转变点温度为283 K.其电阻率在T<TMI时符合电子-电子、电子-磁振子散射公式;在T>TMI时为小极化子输运.薄膜在低温段连续激光(波长为532 nm,40 mW)作用下电阻率显著增大,电阻变化率在253 K达到最大值51.1%,该变化率远大于相同条件下的空穴掺杂材料;在高温段产生了较小的光电导,电阻变化率小于10%.这些现象主要与激光激励下自旋系统和小极化子的变化有关.La0.82Te0.18MnO3薄膜在激光诱导下具有明显的与自旋相关的弛豫现象.激光开始作用时薄膜电阻率随时间的变化符合指数关系. 关键词: 0.82Te0.18MnO3薄膜')" href="#">La0.82Te0.18MnO3薄膜 光诱导 输运特性 电子掺杂  相似文献   

8.
A位的Gd掺杂对La0.7Sr0.3MnO3体系磁电性质的影响   总被引:7,自引:2,他引:5       下载免费PDF全文
刘宁  高贵珍  童伟  张裕恒 《物理学报》2003,52(12):3168-3175
通过实验研究了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、红外光谱、拉曼光谱、ρ-T曲线和M R-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,高掺杂时的输运性质在其磁背景下发生异常.Gd掺杂引起的磁结构变化和额外 的磁性耦合将导致庞磁电阻效应. 关键词: 磁结构 输运行为 庞磁电阻效应  相似文献   

9.
利用室温下压电调制反射光(PzR)谱技术系统测量了N掺杂浓度为0.0%—3%的分子束外延生长GaNxAs1-x薄膜,并对图谱中所观察的光学跃迁进行了指认.在GaN0.005As0.995和GaN0.01As0.99薄膜的PzR谱中观察到此前只在椭圆偏振谱中才看到的N掺杂相关能态E11N.当N掺杂浓度达到 关键词: 压电调制反射光谱(PzR) xAs1-x薄膜')" href="#">GaNxAs1-x薄膜 分子束外延(MBE)  相似文献   

10.
万冀豫  金克新  谭兴毅  陈长乐 《物理学报》2010,59(11):8137-8141
利用固相反应法制备Pr0.5Ca0.5MnO3(PCMO)靶材,并采用脉冲激光沉积法(PLD)在n型Si(111)基片上沉积PCMO外延薄膜,研究了薄膜的输运特性及薄膜与Si衬底形成异质结的整流特性.结果表明:在80—300 K温度范围内,PCMO薄膜的阻温关系符合变程跳跃模型,随着温度的升高表现出从一维到二维再到三维的转变,分析认为可能源于轨道自由度对电子输运特性的影响.PCMO/Si异质结在磁场作用下整流特性得到改善,且在正向电流方向出 关键词: 0.5Ca0.5MnO3')" href="#">Pr0.5Ca0.5MnO3 Si 整流 正磁电阻  相似文献   

11.
P Raychaudhuri  C Mitra  K Dorr  KH Muller  G Kobernik  R Pinto 《Pramana》2002,58(5-6):1179-1182
Hole-doped rare-earth manganite La0.7Ca0.3MnO3 and the electron-doped manganite La0.7Ce0.3MnO3 both show a metal-insulator transition around 250 K associated with a ferromagnetic transition and colossal magnetoresistance. In an earlier publication we have reported the rectifying characteristic of La0.7Ca0.3MnO3/SrTiO3/La0.7Ce0.3MnO3 tunnel junction at room temperature, showing that it is possible to fabricate a diode out of the polaronic insulator regime of doped manganites. Here we report the magneto-transport properties of such a tunnel junction above and below the metal-insulator transition. We show, from the large positive magnetoresistance of the tunnel junction at low temperature, that La0.7Ce0.3MnO3 could be a minority spin carrier ferromagnet. The implication of this observation is discussed.  相似文献   

12.
La1−xPrxMnO3 (LPrMO) thin films have been epitaxially grown on (1 0 0)SrTiO3 single-crystal substrates by pulsed-laser deposition. The films have a perovskite structure and give rise to the colossal magnetoresistance effect with the maximum magnetoresistance ratio of 103% (at 240 K and 5 T). The electrical transport and magnetic properties have been investigated for the La0.8Pr0.2MnO3 film with thickness 3000 Å. The results indicate that the films have quite a distinctive magnetotransport behavior compared to the bulk. The analysis of X-ray photoemission spectroscopy suggests that the valence state of Pr is 4+ in LPrMO film. Therefore, the epitaxial film is most likely an electron-doped colossal magnetoresistance system.  相似文献   

13.
Epitaxial Pr0.5Ca0.5MnO3 films have been synthesized on (0 0 1) SrTiO3 substrate using a chemical solution deposition technique and two-step post-annealing process. The zero field resistivity of the films shows semiconducting behavior and a characteristic of charge ordering is observed at 230 K. The resistivity of the 10 nm film did not show any effect with the magnetic field. However, melting of charge ordering was observed for the 120 nm film at an applied magnetic field of 4 T. Large decrease in the resistivity of the 120 nm film (<100 K) resulted in magnetoresistance of nearly −100% at 75 K.  相似文献   

14.
The effect of simultaneous substitution of a fluctuating cation and a divalent cation in LaMnO3 perovskite modifies the properties of the material to exhibit large valence colossal magnetoresistance (CMR) effect. A good example of these properties is (La1−2x Pr x Ca x )MnO3 (LPCMO) type CMR material. In this communication it is reported that, with the increase in x (for x=0.1, 0.15, 0.2), the T c varies between 100 and 120 K with improvisation in metal-insulator transition. Interestingly, resistance increases with x from few hundred ohms to few kilo ohms with corresponding decrease in the unit cell volume. The results of the studies using X-ray diffraction (XRD), electrical resistivity, magnetoresistance and ac susceptibility measurements on LPCMO samples for understanding the structural, transport and magnetic properties are discussed in detail.  相似文献   

15.
The colossal negative magnetoresistance (approximately 12%) in a field of 8.4 kOe over a wide range of temperatures below the Curie point T C ≈240 K in a single-crystal La0.35Nd0.35Sr0.3MnO3 film on a single-crystal (001)ZrO2(Y2O3) wafer substrate is discussed. Isotherms of the magnetoresistance of this film reveal that its absolute value increases with the field, abruptly in the technical magnetization range and almost linearly in stronger fields. For three single-crystal films of the same composition on (001)LaAlO3, (001)SrTiO3, and (001)MgO substrates, colossal magnetoresistance only occurred near T C ≈240 K and at T<T C it increased weakly, almost linearly, with the field. In the film on a ZrO2(Y2O3) substrate the electrical resistivity was almost 1.5 orders of magnitude higher than that in the other three films. It is shown that this increase is attributable to the electrical resistance of the interfaces between microregions having four types of crystallographic orientations, while the magnetoresistance in the region before technical saturation of the magnetization is attributable to tunneling of polarized carriers across these interfaces which coincide with the domain walls (in the other three films there is one type of crystallographic orientation). The reduced magnetic moment observed for all four samples, being only 46% of the pure spin value, can be attributed to the existence of magnetically disordered microregions which originate from the large thickness of the domain walls which is greater than the size of the crystallographic microregions and is of the same order as the film thickness. The colossal magnetoresistance near T C and the low-temperature magnetoresistance in fields exceeding the technical saturation level can be attributed to the existence of strong s-d exchange which is responsible for a steep drop in the carrier mobility (holes) and their partial localization at levels near the top of the valence band. Under the action of the magnetic field the carrier mobility increases and they become delocalized from these levels.  相似文献   

16.
研究了典型的层状钙钛矿结构超导单晶Sr2RuO4在c方向的磁阻(Δρ/ρ0)(H∥ab,J∥c)的变化.实验发现,磁阻表现出强烈的各向异性,并且随着温度T的降低,磁阻效应越明显;当在平面ab内旋转磁场H的方向时,磁阻成周期性变化;实验表明,磁场沿(110)方向时,出现磁阻的极大值.分别从Sr2RuO4的费米面的各向异性、载流子散射率、c方向能带色散的各向异性等方面来解释这些输运性质. 关键词: 2RuO4')" href="#">Sr2RuO4 磁阻  相似文献   

17.
The effect of crystal lattice disorder on the conductivity and colossal magnetoresistance in La1-xCaxMnO3 ( ) films has been examined. The lattice defects are introduced by irradiating the film with high-energy ( MeV) electrons with a maximal fluence of about cm-2. This comparatively low dose of irradiation produces rather small radiation damage in the films. The number of displacements per atom (dpa) in the irradiated sample is about 10-5. Nevertheless, this results in an appreciable increase in the film resistivity. The percentage of the resistivity increase in the ferromagnetic metallic state (below the Curie temperature ) was much greater than that observed in the insulating state (above ). At the same time irradiation has much less effect on or on the magnitude of the colossal magnetoresistance. A possible explanation of such behavior is proposed. Received 21 July 1999 and Received in final form 27 December 1999  相似文献   

18.
采用固相烧结法合成了单相巨介电常数氧化物CaCu3Ti4O12(CCTO).用阻抗分析仪分析了10—420 K温度范围内的介电频谱和阻抗谱特性,并结合ZVIEW软件进行了模拟.结果表明:温度高于室温时,频谱出现两个明显的弛豫台阶,低频弛豫介电常数随温度升高而显著增大,表现出热离子极化特点;温度低于室温时,频谱表现出类德拜弛豫,且高、低平台介电常数值基本不随温度变化,表现出界面极化特点和较好的温度稳定性.频谱中依次出现的介电弛豫对应于阻抗谱中 关键词: 3Ti4O12')" href="#">CaCu3Ti4O12 介电频谱 阻抗谱 Cole-Cole半圆弧  相似文献   

19.
La0.7Sr0.3MnO3 films were prepared by dc sputtering on Si (100) substrate at different working pressure. The possibility of controlling the magnetic and transport properties of colossal magnetoresistance film is investigated, which has attracted great research interest for practical application. The as-grown film shows different magnetic, transport and magnetoresistance change at different working pressure at room temperature, which is quite attractive from technological point of view. Maximum magnetoresistance (MR) of ?5.56%, Curie temperature (Tc) of 325 K and metal insulator transition temperature (TMI) of 278 K was achieved at room temperature.  相似文献   

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