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Lattice Effect on Magnetic and Electrical Properties of Ln_(2/3)Pb_(1/3)MnO_3(Ln=La,Pr,Nd)Films 被引量:2
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作者 Li'an HAN Huaping YANG Yongjun HE 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2008年第5期709-711,共3页
Lattice effect on magnetic and electrical transport properties of Ln2/3Pb1/3MnO3 (Ln=La, Pr, Nd) films prepared by RF magnetron sputtering technique were investigated. With the decrease of the average ions radius ... Lattice effect on magnetic and electrical transport properties of Ln2/3Pb1/3MnO3 (Ln=La, Pr, Nd) films prepared by RF magnetron sputtering technique were investigated. With the decrease of the average ions radius 〈rA〉, the structure of Ln2/3Pb1/3MnO3 (Ln=La, Pr, Nd) targets transit from the rhombohedral phase to the orthorhombic phase, and the Curie temperature reduces rapidly with the decrease of 〈rA〉. The electrical properties show that films are the metallic state which can be fitted to the formula: ρ(T)=ρ0 + ρ1T^2 + ρ2T^4.5 at low temperatures. The temperature range of the ferromagnetic metallic state becomes narrow with the decrease of 〈rA〉. The phenomenon can be explained by the lattice effect. 展开更多
关键词 Lattice effect ln2/3pb1/3mno3 films Electrical properties
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Pb(In_(1/2)Nb_(1/2))O_(3)-Pb(Mg_(1/3)Nb_(2/3))O_(3)-PbTiO_(3)弛豫铁电薄膜厚度尺寸效应研究
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作者 贾慧霞 杨嘉倩 +3 位作者 沈逸尘 谢济舟 段志华 王飞飞 《上海师范大学学报(自然科学版)》 2023年第5期574-581,共8页
新一代弛豫铁电薄膜Pb(In_(1/2)Nb_(1/2))O_(3)-Pb(Mg_(1/3)Nb_(2/3))O_(3)-PbTiO_(3)(PIMNT)因兼具优异的电学性能与高的相变温度,在国内外获得广泛关注.为了探究不同薄膜厚度对PIMNT薄膜的结构及电学性能的影响,通过溶胶凝胶法制备了1... 新一代弛豫铁电薄膜Pb(In_(1/2)Nb_(1/2))O_(3)-Pb(Mg_(1/3)Nb_(2/3))O_(3)-PbTiO_(3)(PIMNT)因兼具优异的电学性能与高的相变温度,在国内外获得广泛关注.为了探究不同薄膜厚度对PIMNT薄膜的结构及电学性能的影响,通过溶胶凝胶法制备了150 nm~1μm不同厚度的PIMNT薄膜,对其形貌结构以及电学性能进行了对比研究,在此基础上进一步研究了极化对其电学性能的影响.实验结果表明:随着厚度的增加,薄膜介电常数先增加后略有降低,剩余极化强度先增大后减小,矫顽场逐渐增大;在极化电压为18 V、极化温度和时间分别为100℃和5 min时,1μm厚度PIMNT薄膜的介电常数和损耗在100 Hz下分别为1009和0.022,室温下的热释电系数达6.85×10^(-4) C∙m^(-2)∙K^(-1),是目前主流的锆钛酸铅(PZT)薄膜的3倍左右. 展开更多
关键词 pb(In_(1/2)Nb_(1/2))O_(3)-pb(Mg_(1/3)Nb_(2/3))O_(3)-pbTiO_(3)(PIMNT)薄膜 厚度尺寸效应 电学性能 极化 热释电系数
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La_(2/3)Pb_(1/3)MnO_3外延膜的结构及磁电特性研究
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作者 韩立安 陈长乐 《空军工程大学学报(自然科学版)》 CSCD 北大核心 2007年第3期91-94,共4页
通过射频磁控溅射法在单晶LaAlO3(100)衬底上成功的沉积了膜厚为300 nm的La2/3Pb1/3MnO3外延膜。利用X射线衍射仪、原子力和超导量子干涉仪、直流四探针法对其结构、磁电特性进行了系统的研究。结果表明,薄膜为赝立方钙钛矿结构,沿(100... 通过射频磁控溅射法在单晶LaAlO3(100)衬底上成功的沉积了膜厚为300 nm的La2/3Pb1/3MnO3外延膜。利用X射线衍射仪、原子力和超导量子干涉仪、直流四探针法对其结构、磁电特性进行了系统的研究。结果表明,薄膜为赝立方钙钛矿结构,沿(100)方向择优生长,具有良好的单晶外延结构。居里温度TC=345 K,在居里温度附近,发生铁磁-顺磁转变。此材料呈现出一种典型的自旋玻璃特性,是由于应力造成的。对于顺磁态、自旋玻璃态及铁磁态时其磁矩分布给予了合理的解释。在1 T磁场下,其磁电阻极大值为23.4%。 展开更多
关键词 La2/3pb1/3mno3外延膜 磁性 电特性
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钙钛矿La_(2/3)Pb_(1/3)MnO_3外延膜的制备及磁性
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作者 韩立安 陈长乐 《河北师范大学学报(自然科学版)》 CAS 北大核心 2007年第3期333-336,共4页
利用磁控溅射法在单晶LaAlO3(100)衬底上成功地外延生长了La2/3Pb1/3MnO3薄膜.用X射线衍射仪、原子力显微镜和超导量子干涉仪、直流四探针法对其进行了表征.结果表明,薄膜为赝立方钙钛矿结构,晶格常数为3.861 nm,晶格失配度为2.1%,具有... 利用磁控溅射法在单晶LaAlO3(100)衬底上成功地外延生长了La2/3Pb1/3MnO3薄膜.用X射线衍射仪、原子力显微镜和超导量子干涉仪、直流四探针法对其进行了表征.结果表明,薄膜为赝立方钙钛矿结构,晶格常数为3.861 nm,晶格失配度为2.1%,具有良好的单晶外延结构和较光滑的表面,且薄膜中晶粒的生长模式是“柱状”模式.居里温度为325 K,在居里温度附近,发生铁磁-顺磁转变.此材料呈现出一种典型的自旋玻璃特性,是由于应力造成的.在1.0 T磁场下,其磁电阻为23.4%. 展开更多
关键词 La2/3pb1/3mno3薄膜 磁性 磁电阻
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La_(2/3)Ca_(1/3)MnO_3薄膜结构与输运性质 被引量:2
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作者 吴小山 徐金 +8 位作者 蔡宏灵 张爱梅 蒋树声 谭伟石 陈中军 陈兴 孙民华 吴忠华 高炬 《核技术》 CAS CSCD 北大核心 2004年第5期329-333,共5页
用磁控溅射方法在不同单晶衬底材料上制备了一系列含La2/3Ca1/3MnO3(LCMO)薄膜。当薄膜厚度大于200?,在我们实验条件下可观测到金属-绝缘体转变,且转变温度随厚度和衬底材料而变化。渗流电阻模型被用来解释薄膜材料的电输运特性,结合薄... 用磁控溅射方法在不同单晶衬底材料上制备了一系列含La2/3Ca1/3MnO3(LCMO)薄膜。当薄膜厚度大于200?,在我们实验条件下可观测到金属-绝缘体转变,且转变温度随厚度和衬底材料而变化。渗流电阻模型被用来解释薄膜材料的电输运特性,结合薄膜外延特性(晶格失配)和薄膜与衬底的相互作用,及薄膜表面、界面粗糙度的测量可知薄膜的剩余电阻、极化子的激活能、金属-绝缘体转变温度等密切与薄膜质量相关。 展开更多
关键词 La2/3Ca1/3mno3薄膜 衬底效应 界面粗糙度 晶格失配
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A phenomenological description of temperature dependence of magnetoresistance in La_( 2/3)Ca_(1/3)MnO_(3-δ) thin films
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作者 李西军 李可斌 +6 位作者 杜家驹 许小军 方军 王智河 曹效文 朱警生 张裕恒 《Science China Mathematics》 SCIE 1998年第3期308-312,共5页
The electrical resistance in zero magnetic field and magnetoresistance in different external magnetic fields have been measured in a temperature range of 77-300 K. It is found that the temperature dependence of magnet... The electrical resistance in zero magnetic field and magnetoresistance in different external magnetic fields have been measured in a temperature range of 77-300 K. It is found that the temperature dependence of magnetoresistance can be well described by a phenomenological formula of ρ(T)=(1σ(T)= (1α(M/M s) 2+βexp(-E 0/k BT), where the fitting parameters α,β vary as the external magnetic field H changes, E 0 is the activation energy, E 0/k B =1160 K, M s is the saturation magnetization, the temperature and magnetic field dependence of M/M s is obtained by the mean-field expression. 展开更多
关键词 LA 2/3Ca 1/3mno 3 EPITAXIAL THIN films MAGNETORESISTANCE MEAN-FIELD expression.
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Giant magnetoresistance effect and temperature dependence of magnetoresistance in La_(2/3)Ca_(1/3)MnO_2 thin film
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作者 李可斌 刘玲 +7 位作者 孙建三 许小军 方军 王胜 王福堂 曹效文 朱警生 张裕恒 《Science China Mathematics》 SCIE 1996年第6期624-630,共7页
Magnetoresistanoe in the temperature region from 300 K to liquid helium temperature has been measured on good (100) oriented La2/3Ca1/3MnO2 thin films prepared by d.c. magnetron sputtering on ZrO2 (100) substrates. It... Magnetoresistanoe in the temperature region from 300 K to liquid helium temperature has been measured on good (100) oriented La2/3Ca1/3MnO2 thin films prepared by d.c. magnetron sputtering on ZrO2 (100) substrates. It is found that there appears a resistance peak at about TP = 72K at zero magnetic field, and this peak moves to higher temperature with increasing field H, and R decreases simultaneously. However, the magnetoresistance ratio MR = 5R /R (H) = (Ro~ RH) /RH has a different temperature dependence. There are also MR peaks, but the temperature of maximum MR is at about 25 K which does not change with changing external magnetic field. The heat treatment (annealed at 700C in 105’Pa O2 for 30min) will make R reduce dramatically and has an effect on the temperature dependence of R and its MR. 展开更多
关键词 La_(2/3)Ca_(1/3)mno_2 thin film MAGNETORESISTANCE negative giant magnetoresistance.
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Field dependence of magnetoresistance in epitaxial single-crystal La_(2/3)Ca_(1/3)MnO_(3-δ) thin film
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作者 李可斌 程荣胜 +7 位作者 王守国 陈志祥 方军 王智河 曹效文 许小军 朱警生 张裕恒 《Science China Mathematics》 SCIE 1999年第1期99-105,共7页
Epitaxial La2/3Ca1/3 MnO3 thin films were prepared on NdGaO3(110) substrates by d. c. magnetron sputtering method. The measurements of magnetoresistance ρ(H) upon magnetic field at different temperatures were carried... Epitaxial La2/3Ca1/3 MnO3 thin films were prepared on NdGaO3(110) substrates by d. c. magnetron sputtering method. The measurements of magnetoresistance ρ(H) upon magnetic field at different temperatures were carried out in the field range of 0 - 8 T. It is found that p(H) obeys the following relations: when the temperature(T) is higher than the Curie temperature Tc, ρ ( H ) =1/α(T)+β(T)H2; below Tc, ρ ( H ) = ρ0 ( T ) 1/A(T)+B(T)exp(H/C(Y)),and ρ(H) =1/κa(T)+γ(T)H when T is far below TC. It is Suggested that the negative magnetoresistive effect is mainly due to enhancement of the magnetoconductance. 展开更多
关键词 epitaxial La_(2/3)Ca_(1/3)mno_3 thin films colossal magnetoresistive effect field dependence of magnetore-sistance.
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压电微机械超声换能器仿真与结构优化 被引量:1
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作者 余卿 遆金铭 +1 位作者 樊青青 李俊红 《压电与声光》 CAS 北大核心 2022年第3期403-406,共4页
压电微机械超声换能器(PMUT)在医疗阵列成像、手势识别、内窥成像、指纹识别等领域有着重要的应用,而灵敏度等性能是影响其成像质量的主要因素。该文对基于PMN-PT圆形压电复合振动膜的压电微机械超声换能器等效电路模型进行分析,并通过... 压电微机械超声换能器(PMUT)在医疗阵列成像、手势识别、内窥成像、指纹识别等领域有着重要的应用,而灵敏度等性能是影响其成像质量的主要因素。该文对基于PMN-PT圆形压电复合振动膜的压电微机械超声换能器等效电路模型进行分析,并通过有限元法研究了压电层PMN-PT厚度对PMUT的发射电压响应、接收灵敏度的影响。仿真结果表明,当压电层厚度为4.5μm(厚度为基底厚度的90%)时,换能器的发射电压响应级最大,达到191.6 dB,接收灵敏度级随厚度的增加基本呈线性上升趋势;当压电层厚度为5.1μm(厚度为基底厚度的102%)时,回路增益(损耗)最大,达到-64.50 dB。 展开更多
关键词 PMN-PT薄膜 PMUT 回路增益(损耗) 接收灵敏度 发射电压响应
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