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用两线法和四线法对球磨合成后热处理的Nd0.7Sr0.3MnO3陶瓷样品的电脉冲诱导电阻转变(EPIR)效应进行了测试.结果表明:在Nd0.7Sr0.3MnO3块体中用四线法测得的I-V曲线为非线性,说明Nd0.7Sr0.3MnO3样品在晶(相)界处存在空间电荷层和界面电阻.但用四线法测量EPIR效应时,没有EPIR效应发生,表明晶(相)界处的空间电荷层和肖特基势垒不能产生EPIR效应;对同一样品采用直流两线法测量,其I-V曲线也为非线性,但却发生明显的EPIR效应.说明在Nd0.7Sr0.3MnO3陶瓷中发现的EPIR效应起源于样品与电极之间的接触界面,块体内的晶(相)界处虽能产生相似I-V特性,但却不能发生EPIR效应.
关键词:
电脉冲诱导电阻转变(EPIR)
亚锰酸盐
空间电荷层
I-V非线性')" href="#">I-V非线性 相似文献
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采用磁控溅射,紫外线光刻和离子束刻蚀制备了La2/3Ca1/3MnO3/Eu2CuO4/La2/3Ca1/3MnO3磁性隧道结.通过对获得的磁性隧道结的I-V特性测量,发现非线性的I-V特性,显示结样品的隧穿特性.有趣的是发现在电极材料La2/3Ca1/3MnO3的金属-绝缘体转变温度(Tp)以下,I-V曲线出现一个跳变.随着温度降低,开始出现跳变的临界电流增大,但是跳变都发生在同样的电压下~209mV.当电流增大或减小在跳变点附近出现回滞.这一跳变只发生在铁磁金属态,表明这是一个磁性相关联的效应,可能对应一种新的磁性开关过程.虽然,目前对这一现象背后的物理机理还不清楚,但是,这一现象有可能在未来自旋电子学器件方面具有潜在的应用价值.
关键词:
庞磁电阻
磁性隧道结
开关效应 相似文献
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自LaAlO3/SrTiO3异质界面发现高迁移率的二维电子气以来,其二维超导电性、界面磁性和自旋轨道耦合等诸多物理性质已经被广泛研究.对于二维超导体,零温下超导-反常金属相变的起源仍然是一个悬而未决的问题.传统理论认为在超导-绝缘量子相变中只存在2种基态,即库珀对的超导基态和绝缘基态.然而在研究超导颗粒膜中超导电性的演化与厚度和温度的关系时发现,存在一个中间金属态破坏了超导体和绝缘体之间的直接过渡.这种中间金属态的标志性特征是,在超导转变温度之下存在饱和的剩余电阻,与之对应的基态称作反常金属态.本文主要对在LaAlO3/SrTiO3(001)异质界面磁场诱导的超导-反常金属量子相变进行了系统的研究.在没有外加磁场的情况下,电阻-温度(R-T)曲线和电流-电压(I-V)特性曲线表明样品在超导转变温度之下处于超导态.外加磁场会导致样品在低温下出现饱和电阻、正的巨磁阻和低电流范围内的线性I-V曲线.另外,霍尔电阻在一定的磁场之下会出现零电阻平台,而此时纵向电阻不为零,表现出明显的玻色金属态的特征.研究结果... 相似文献
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采用改进的溶胶-凝胶方法在单晶Si(100)衬底上制备了介电性能优异的(Ba0.7Sr0.3)TiO3/LaNiO3异质薄膜.实验发现,在750 ℃下 、O2气氛中晶化的LaNiO3薄膜的电阻率最小.C-V与I-V特性测量表明(Ba0.7Sr0.3)TiO3薄膜具有优异的介电性能,在频率为50kHz、零偏压下的相对介电常数εr>300,偏压为6V时漏电流密度JL<1.2×10-6A/cm2.
关键词:
xSr1-x)TiO3铁电薄膜')" href="#">(BaxSr1-x)TiO3铁电薄膜
3底电极')" href="#">LaNiO3底电极
溶胶-凝胶法 相似文献
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使用牛津震动样品磁强计(VSM)研究了Bi2Sr2CaCu2O8单晶的磁滞回线.在20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20K温度处,在20K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
关键词:
2Sr2CaCu2O8单晶')" href="#">Bi2Sr2CaCu2O8单晶
磁滞回线
尖锋效应
相变 相似文献
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R.Z. Mehdiyeva Mir Hasan Yu. Seyidov I.B. Baykulov 《Journal of Physics and Chemistry of Solids》2006,67(12):2623-2627
Boundaries of morphotropic phase transitions region in the system of solid solutions K2Pb4Nb10O30-Na2Pb4Nb10O30-K6W4Nb6O30 with the structure of the tetragonal tungsten bronze have been specified. Presence of the second morphotropic phase transition, perpendicular to the first one has been revealed. The temperature dependences of the structural parameters of some compounds have been investigated. The compounds with high values of Curie temperatures and working temperatures have been obtained. 相似文献
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本文用差热分析法和高温、室温X射线衍射法对Li3VO4,Li4SiO4的相变过程,Li3VO4-Li4SiO4,Li3O4-Li-4GeO4赝二元系相图以及Li3VO4-Li4SiO4-Li4GeO4赝三元系相图室温截面进行了研究。发现在Li3VO4-Li4SiO4,Li3VO4-Li4GeO4赝二元系中,由于Li4SiO4或Li4GeO4的加入而使Li3VO4的高温γII相稳定存在于室温,从而得到一种新的具有高电导率的锂离子导体。作者认为探寻使高温态稳定存在于室温的方法是探索新的离子导体研究中有效途径之一。
关键词: 相似文献
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Tetsuo Hanaguri Takashi Tsuboi Atsutaka Maeda Yasutoshi Kotaka Jun-ichi Shimoyama Kohji Kishio 《Czechoslovak Journal of Physics》1996,46(Z3):1559-1560
In Bi2Sr2CaCu2Oy under magnetic fields along the c-axis, both the local and the macroscopic magnetization show clear steps indicating the
first order phase transition (FOPT) in the vortex lattice (VL). Local measurements have revealed that the FOPT occurs from
the center of the sample owing to the field inhomogeneity originated from the geometrical effect. The heights of the steps
are strongly suppressed in local measurements by the demagnetization effect. With decreasing temperature, the irreversibility
in the magnetization just below the step begins to increase and is smoothly connected to the second peak at low temperatures. 相似文献
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Nguyen Ba Chanh Christian Hauw Alain Meresse Madeleine Rey-Lafon Laure Ricard 《Journal of Physics and Chemistry of Solids》1985,46(12):1413-1420
The existence of three main crystalline phases (called III, II and I) in (C12H25NH3)2CdCl4 has been revealed by differential scanning calorimetry. X-ray diffraction and spectroscopic studies. The crystal- lographic evolution with increasing temperature appears to be monoclinic (III) → orthorhombic (II) → tetragonal (I). The low temperature phase III is the only ordered structure. The phase transition (III-II), which is of first order type, corresponds to an order-disorder mechanism involving the organic part of the structure (alkylammonium chains) whereas the phase transition (II-I), which is of second-order type, is related to the arrangement of the mineral matrix (octahedra of perovskite layers). An intermediate disordered form II', stable in a very narrow temperature range and structurally similar to the form II, has also been observed, so that the transformation (III-II) proceeds, in fact, in two steps (III-II'-II). The variation enthalpies observed at the transitions (III-II'-II) and analyzed through an order-disorder mechanism demonstrate the high disorder of the alkylammonium chains in form II, in agreement with spectroscopic results. No thermal anomaly or spectroscopic modification is observed for the high temperature transition (II-I). 相似文献
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The proton polarization in 16O(p, p0)16O has been measured for laboratory proton energies between 10.0 and 16.0 MeV. Measurements were made for 18 or more angles at 60 energies. In addition, excitation functions of polarization were measured at 6 angles in 50 keV steps from 12.8 to 16.0 MeV. Both optical-model and phase-shift analyses were performed using published cross-section data in conjunction with the polarization data. The energy dependence of the complex phase shifts yielded spin, parity, and width assignments for 10 levels in 17F and possible assignments for 10 additional levels. A review of the energy levels of 17F below 16 MeV is given. 相似文献
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V.S. VassilevZ.G. Ivanova E.S. DospeiskaS.V. Boycheva 《Journal of Physics and Chemistry of Solids》2002,63(5):815-819
The glass-forming regions of the GeSe2-CdI2-TeO2 (I), GeSe2-CdI2-Bi2O3 (II) and GeSe2-TeO2-Bi2O3 (III) systems have been determined. The obtained glassy phases have been characterized by their basic physicochemical parameters such as temperatures of glass transition, crystallization, and melting, density and microhardness. The phase T-X diagram of the GeSe2-CdI2 system, which is the basic joint line for systems I and II, has been specified. Three non-variant equilibria (two eutectic and one syntectic) have been observed at temperatures 350, 280 and 375 °C for compositions containing 15, 95 and 33.3 mol% GeSe2, respectively. A new intermediate phase with probable composition of 2CdI2·GeSe2 has been formed. 相似文献
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The magnetic phase diagrams of Mn(Nb0.5Ta0.5)2O6 have been determined by means of neutron diffraction. Two spin-flop-transitions GxAz → AxGz → Gy have been detected in a magnetic field parallel to the x-direction. The first phase boundary increases as the temperature rises up to a triple point at 4.74 K and 20.5 kOe, whereas the second phase boundary decreases until another triple point at 4.55 K and 35.5 kOe is reached. In fields parallel to the z-direction a transition GxAz → GxGz has been revealed, the phase boundary meets the paramagnetic one in a triple point at 4.65 K and 55 kOe. 相似文献
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用透射电子显微镜对Ni51Zr49非晶合金的晶化过程进行了研究,发现晶化初期首先从非晶基体上析出的是具有C心单斜点阵的NiZr'相,a=0.3268nm,b=0.4101nm,c=0.5224nm,β=71.8°。与稳定相NiZr有很明确的取向关系:[100]NiZr'∥[100]NiZr [001]NiZr'∥[110]NiZr。它可以看成是NiZr相的亚稳态或超结构。随温度升高,逐渐转变成NiZr相。温度再高时,在非晶基体上还会析出少量Ni10Zr7相。晶化初期,无论是NiZr还是NiZr'相,都是以多次孪晶的形式析出。孪晶有这两种基本形式,一种是以NiZr或NiZr'的[021]方向为轴的180°孪晶,一种是以NiZr的[001]或NiZr'的[010]方向为轴的36°旋转孪晶,其它孪晶为这两种孪晶方式的重复与组合。随着温度的升高,孪晶逐渐减少。
关键词: 相似文献