共查询到19条相似文献,搜索用时 162 毫秒
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利用电弧炉熔炼了Ni50Mn35In15多晶样品,根据磁性测量对其马氏体相变和磁热效应进行了系统研究.结果表明,随着温度的降低,样品在室温附近先后发生了二级磁相变与一级结构相变特征的马氏体相变,导致它的磁化强度产生突变. 同时通过低温下的磁滞回线的测量发现样品存在交换偏置行为,表明低温下马氏体相中铁磁和反铁磁共存. 此外,根据Maxwell方程,计算了样品在马氏体相变温度附近的磁熵变,当温度为309K,磁场改变5 T时,样品的磁熵变可达22.3J/kgK.
关键词:
哈斯勒合金
50Mn35In15')" href="#">Ni50Mn35In15
马氏体相变
磁热效应 相似文献
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对六种钨青铜结构的铌酸盐铁电晶体进行了从15K到室温范围的介电特性及热电特性的研究。分析其介电特性和热电特性与极化电场的关系,用X射线粉末衍射进行佐证。证实在50—70K的范围内,SBN,PBN,KNSBN三类铁电钨青铜型铌酸盐晶体均存在着一个新的相变。相变是由点群4mm铁电相到点群mm2铁电相的转变。铁电自发极化方向由四方晶胞的e轴方向转变到正交晶胞的b轴方向。介电特性的高频及低频测量表明该相变具有扩散(或称瀰散)型特征。比热的实验结果证明相变是属于高于一阶相变的高阶相变。对相变前
关键词: 相似文献
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研究了K3C60单晶薄膜在200K附近的导带结构.样品温度为190K时,同步辐射角分辨光电子谱能够观察到[111]方向有规律的能带色散.而在220K附近色散不存在.这一实验结果与K3C60在200K存在取向相变相符合.用反铁磁Ising模型对实验结果进行了分析.结果表明,K3C60在200K的相变是由低温下的一维无序取向结构转变为200K以上的双取向结构畴与无序分子(约占40
关键词:
3C60')" href="#">K3C60
取向相变机理 相似文献
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VO2是一种热致相变金属氧化物. 在341 K附近, VO2发生由低温绝缘体相到高温金属相的可逆转变, 同时伴随着光学、电学和磁学等性质的可逆突变, 这种独特的性质使得VO2在光电开关材料、智能玻璃、存储介质材料等领域有着广阔的应用前景. 因此, VO2金属-绝缘体可逆相变一直是人们的研究热点, 但其相变机理至今未有定论. 首先, 简要概述了VO2相变时晶体结构和能带结构的变化情况: 从晶体结构来讲, 相变前后VO2从低温时的单斜相VO2(M)转变为高温稳定的金红石相VO2(R), 在一定条件下此过程也可能伴随着亚稳态单斜相VO2(B)与四方相VO2(A)的产生; 从能带结构来看, VO2处于低温单斜相时, 其d//能带和π*能带之间存在一个禁带, 带宽约为0.7 eV, 费米能级恰好落在禁带之间, 表现出绝缘性, 而在高温金红石相时, 其费米能级落在π*能带与d//能带之间的重叠部分, 因此表现出金属导电性. 其次, 着重总结了VO2相变物理机理的研究现状. 主要包括: 电子关联驱动相变、结构驱动相变以及电子关联和结构共同驱动相变的3种理论体系以及支撑这些理论体系的实验结果. 文献报道争论的焦点在于, VO2是否是Mott绝缘体以及结构相变与MIT相变是否精确同时发生. 最后, 展望了VO2材料研究的发展方向. 相似文献
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铁基超导体中含有一类特殊的112型结构化合物,其层状结构中含有一层锯齿形的As链构型.本文报道了用CsCl助熔剂法生长新型铁基112型EuFeAs2母体单晶的具体方法,以及对该单晶的结构和物性的详细表征.通过能量色散X射线能谱扫描对单晶样品进行的化学成分分析,以及单晶X射线衍射的结构解析,确定该单晶样品属于EuFeAs2相,结构精修得到EuFeAs2具有空间群为Imm2(No.44)的正交晶体结构,晶格常数分别是a=21.285(9)Å,b=3.9082(10)Å,c=3.9752(9)Å.通过低温电阻测量,发现在110 K附近和46 K附近存在两个异常电阻跳变.进一步分析表明,110 K附近存在两个邻近的相变,这两个相变与铁基母体材料中常见的结构相变和Fe2+的反铁磁相变相符合.结合磁化率测量分析,可知46 K附近的相变属于Eu2+的反铁磁相变. 相似文献
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测量了在O2中退火不同时间的Sm1.85Ce0.15CuO4单晶样品的热电势S与电阻率ρ的温度依赖关系.所有的样品电阻率高温下呈现线性温度依赖行为.未退火的样品在148K发生超导转变,而退火后的样品在低温下发生金属半导体相变,其超导电性消失,表明退火引起了载流子浓度下降,体系进入欠掺杂态.随着温度降低,所有的样品ST和ρT曲线在200K附近(T)都发生斜率的改变,可以用赝能隙现象解释.热电势S在低温下出现一个正的曳引峰,意味着载流子符号发生改变,由电子型转变为空穴型
关键词:
电子型超导体
热电势
赝能隙 相似文献
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The dielectric, pyroelectric, and polarization properties of TlInS2 crystals doped with 0.1 mol % Cr and Mn are investigated. It is shown that TlInS2 compounds doped with chromium and manganese can be assigned to the class of relaxor ferroelectric materials. The temperature range of existence of the stable relaxor (nanodomain) state and the temperature of the phase transition from this state to the ferroelectric (macrodomain) state are determined. The temperature dependence of the pyroelectric current is characterized by an anomaly in the range of the phase transition. 相似文献
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对六种钨青铜结构的铌酸盐铁电晶体进行了从15 K 到室温范围的介电特性及热电特性的研究. 分析其介电特性和热电特性与极化电场的关系, 用x 射线粉末衍射进行佐证. 证实在50 一70 K 的范围内, SBN , PBN , KNSBN 三类铁电钨青铜铌酸盐晶体均存在着一个新的相变. 相变是由点群4mm铁电相到点群mm2 铁电相的转变. 铁电自发极化方向由四方晶胞的c轴方向转变到正交晶胞的b 轴方向.介电特性的高频及低频测量表明该相变具有扩散(或称弥散)型特征. 比热的实验结果证明相变是属于高于一阶相变的高阶相变. 对相变前后的晶胞结构提出了一个模型解释.
关键词: 相似文献
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The effect of a magnetic field on the dielectric properties of Tb0.95Bi0.05MnO3+δ single crystals has been analyzed. It has been shown that the state of the crystal for temperatures of 5–440 K is inhomogeneous and restricted domains of polar and spin correlations are exhibited in it. A phase transition in which the inhomogeneous state of the crystal changes substantially has been observed at a temperature of T ? 180 and 225 K (in the absence and presence of a magnetic field, respectively). The high-temperature phase contains large dielectric domains with a high dielectric constant (ε ~ 105) and thin conducting layers at the boundaries of these domains. The magnetic field significantly affects the state of both low-and high-temperature phases of the crystal, shifting the temperature of the phase transition between them, and induces an additional phase transition at T ? 441 K. 相似文献
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R. Von Der Mühll J. Ravez P. Hagenmuller P. Barbier M. Drache G. Mairesse 《Solid State Communications》1982,43(11):797-799
X-ray diffraction, calorimetric, dielectric and thermocurrent measurements have been carried out on Cs3BiCl6 ceramic samples. Three phase transitions have been detected at T1 = 395 K, T2 = 684 K and T3 = 727 K. The T3 transition is of ferroelastic-paraelastic type. The low temperature phase is characterized by remanent polarization. The depolarization current results probably from charge traps in potential minima which disappear at rising temperature. 相似文献
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The dielectric constant of deuterated ammonium Rochelle salt along the three crystallographic axes as well as the pyroelectric charge density developed on the crystal surface perpendicularly to the b-axis have been measured with a high temperature resolution. The para- to ferroelectric transition at Tc = ?159°C shows a thermal hysteresis of ΔT = 0.15°C. This and the discontinuities in the dielectric constant along all three axes show that the phase transition is of the first-order. No phase intermediate between the para- and the ferroelectric phases could be detected. 相似文献
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The ferroelectric lead germanate (Pb5Ge3O11) and its isomorphous compounds are important because of their uses as pyroelectric and electro-optic devices. Comparison
of inter-planar d-spacings of Pb5Ge3−x
Si
x
O11 (x=0, 0.3, 0.7 and 1.00) suggests that there is no change in basic structure of Pb5Ge3−x
Si
x
O11 when Si is substituted for Ge in small quantity (x<1). The dielectric properties of the Si-substituted compounds have been studied as a function of temperature (30 to 200°C).
The ferroelectric-paraelectric phase transition has been observed at 185°C. The Si doping causes (a) Curie point to shift
towards low temperature, (b) peak value of the dielectric constant to decrease and (c) phase transition diffuse. The fast
increase in dielectric constant of pure Pb5Ge3O11 with temperature (beyond transition temperature) may be attributed to the development of space charge polarization in the
system. 相似文献
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N. D. Scarisoreanu F. Craciun A. Chis R. Birjega A. Moldovan C. Galassi M. Dinescu 《Applied Physics A: Materials Science & Processing》2010,101(4):747-751
Na0.5Bi0.5TiO3-BaTiO3 (NBT-BT) thin films grown by pulsed laser deposition have been investigated by X-ray diffraction, scanning electron microscopy,
and dielectric spectroscopy in order to clarify the role of substrate temperature on crystalline structure, grain morphology,
and dielectric properties. We have shown that the structural and dielectric properties of NBT-BT thin films with composition
at morphotropic phase boundary (6% BT) critically depend on the substrate temperature: small variations of this parameter
induce structural changes, shifting the morphotropic phase boundary toward tetragonal or rhombohedral side. Higher deposition
temperature (1000 K) favor the formation of rhombohedral phase, films deposited at 923 K and 973 K have tetragonal symmetry
at room temperature. Grains morphology depends also on the deposition temperature. Atomic force micrographs show grains with
square or rectangular shape in a compact structure for films grown at lower temperatures, while grains with triangular shape
in a porous structure are observed for films grown at 1000 K. Dielectric spectroscopy measurements evidenced the phase transition
between ferroelectric and antiferroelectric phase at 370 K. Films grown at 1000 K shown low electrical resistivity due to
their porous structure. High dielectric constant values (about 800 at room temperature and 2700 at 570 K) have been obtained
for films grown at temperatures up to 973 K. 相似文献
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Zhang Qingfeng Jiang Shenglin Zeng Yike Fan Maoyan Wang Qingping Zhang Guangzu Zhang Yangyang Yu Yan Wang Jing 《Applied Physics A: Materials Science & Processing》2011,103(4):1159-1163
(Pb0.87La0.02Ba0.1)(Zr0.7Sn0.3−x
Ti
x
)O3 (PLBZST, 0.06≤x≤0.09) antiferroelectric ceramics were fabricated by conventional solid state reaction process, and their ferroelectric, dielectric,
and pyroelectric properties were systemically investigated. PLBZST with different Ti content were all confirmed to be in an
antiferroelectric phase at T=50°C, which is close to the lowest phase transition temperature. Compared with conventional FE ceramics, PLBZST antiferroelectric
ceramics exhibited higher electric field induced pyroelectric coefficient (p). As the content of Ti increased from 0.06 to 0.09, the pyroelectric coefficient increased from 1000 to 6500 μC/m2K under a 500 V/mm DC bias field. The maximum pyroelectric coefficient of 8400 μC/m2K was obtained at x=0.09 when an 850 V/mm DC bias field was applied, which is far larger than that of conventional phase transition pyroelectric
materials. Large pyroelectric response is beneficial for the development of infrared detectors and thermal imaging sensors. 相似文献
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用弱场介电温谱、热释电流谱、强场电滞回线和变温X射线衍射谱研究了微量La掺杂Pb(Zr,Sn,Ti)O3(PZST)反铁电(AFEt)陶瓷在-100—180℃温区内的结构与电学特性.弱场介电温谱显示,AFEt陶瓷在低温段(-100—50℃)呈现介电频率弥散(0.1—100kHz)和扩散型相变的特征,而变温X射线衍射谱却表明材料在这一温区内保持四方相结构;低温下经强场作用后,AFEt被诱导为亚稳三方铁电态,介电频率弥散消失.基于多元复杂化合物的组分起伏理论,讨论了PZST AFEt陶瓷
关键词:
Pb(Zr
Sn
3反铁电陶瓷')" href="#">Ti)O3反铁电陶瓷
反铁电弛豫
相变
变温X射线衍射 相似文献