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1.
通过对La0.3Ca0.7Mn1-xWxO3(x=0.00,0.04,0.08,0.12,0.15)多晶样品M-T曲线、M-H曲线及ESR谱的测量,研究了Mn位W掺杂对电荷有序体系La0.3Ca0.7MnO3磁结构的影响.结果表明,当掺杂量为0.00≤x≤0.08时,体系存在电荷有序(CO)相,AFM/CO态共存于相变温度以下,电荷有序温度TCO随着W掺杂量的增加而增加;x=0.04时,样品在低温下为FM相与AFM/CO相共存,在CO相建立前、后均有FM从PM中分离出来;当x≥0.12时,CO态融化,在极低温度下存在顺磁-铁磁(PM-FM)相变.
关键词:
磁结构
电荷有序
融化
Mn位掺杂 相似文献
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报道了两个典型掺杂的镍氧化物Nd_2-xSr_xNiO_4(x =0.33,1.35)的低温热导率、电阻率和低场交流磁化率,测试温区为77—300K. 在Nd_2-xSr_xNiO_4 (x=0.33)样品的热导率-温度曲线上在电荷有序转 变温度(T_CO)和自旋有序转变温度(T_SO)附近分别观测到反常, 电荷有序使热导率在T_CO以下有所增加,反铁磁自旋有序使热导率在T_SO附近被压制. 在低场交流磁化率-温度曲线上也分别观测到对电荷有序和自旋有 序的响应,而在其电阻率-温度曲线上仅观测到电荷有序. 作为比较,Nd_1.67Sr0.33NiO_4样品中没有观测到输运性质和磁性质上的反常. 两个样品中声子热导占 主导地位. Nd_1.67Sr0.33NiO_4样品中电荷有序和自旋有序导致的热导 率的反常表明样品中存在强的电荷-声子和自旋-声子相互作用.
关键词:
热导率
电荷有序
自旋有序 相似文献
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通过对La0.3Ca0.7Mn1-xVxO3(x=0.05,0.10,0.134,0.20)体系的M-T曲线、ρ-T曲线、ESR谱的测量,研究了Mn位掺V对La0.3Ca0.7MnO3体系电荷序和自旋序的影响.结果表明,当0.05≤x≤0.134时, 体系存在电荷有序(CO)相,其自旋序随温度降低发生顺磁(PM)-电荷有序(CO)-反铁磁(AFM)变化.当x=0.20时,CO相逐步融化,在40 K发生自旋玻璃转变,表现出再入型的自旋玻璃行为,低温下的基态存在着多种复杂的磁相互作用之间的竞争机理.
关键词:
电荷有序
自旋序
相分离
再入型自旋玻璃行为 相似文献
6.
报道了两个典型掺杂的镍氧化物Nd2 -xSrxNiO4 (x=0 33,1 35 )的低温热导率、电阻率和低场交流磁化率 ,测试温区为 77— 30 0K .在Nd2 -xSrxNiO4 (x=0 33)样品的热导率_温度曲线上在电荷有序转变温度 (TCO)和自旋有序转变温度 (TSO)附近分别观测到反常 ,电荷有序使热导率在TCO 以下有所增加 ,反铁磁自旋有序使热导率在TSO 附近被压制 .在低场交流磁化率_温度曲线上也分别观测到对电荷有序和自旋有序的响应 ,而在其电阻率_温度曲线上仅观测到电荷有序 .作为比较 ,Nd0 6 5Sr1 35NiO4 样品中没有观测到输运性质和磁性质上的反常 .两个样品中声子热导占主导地位 .Nd1 6 7Sr0 33NiO4 样品中电荷有序和自旋有序导致的热导率的反常表明样品中存在强的电荷_声子和自旋_声子相互作用 相似文献
7.
对Zn,Ni,Mg高掺杂的La1.85Sr0.15CuO4(LSCO)超导体的X射线衍射谱进行了仔细的分析,从而获得了各掺杂样品的晶格常量、原子结构参量及衍射的峰形参量,比较了不同掺杂所引起的晶体结构的差异,计算了由于掺杂所产生的晶格内部的微应变,结果表明非磁性金属Zn,Mg掺杂比磁性金属Ni掺杂更强烈地抑制了LSCO的超导电性可能与材料中晶格的微应变有关.
关键词:
1.85Sr0.15CuO4')" href="#">La1.85Sr0.15CuO4
磁、非磁掺杂
原子结构参量
晶格微应变 相似文献
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The dependence of critical current density Jc on the angle α between the directions of the applied magnetic field H (which was rotated in the c-axis-I plane) and the in-plane current I was measured on a c-axis oriented epitaxial YBa2Cu3O7-δ films at 81 K, with the magnetic field strength up to 6T, Analysis of the experimental results on the basis of the classical scaling law of pinning force shows that there exist simultaneously planar-pinning and volume-pinning mechanisms, and the contribution of volume pinning increases wish decreasing while that of the planar pinning decreases, We propose that the decrease of Lorentz-force-independent critical current density with increasing H for H∥I results from the suppression of superconductivity by the magnetic field, The fact that the contribution of volume pinning increases with decreasing α also arises from the suppression of superconductivity in CuO2 plane by the magnetic field. 相似文献
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In this paper, we present the results of measurements of the thermal conductivity of Cu2Te2O5Br2, a compound where tetrahedra of Cu2+ ions carrying S=1/2 spins form chains along the c-axis of the tetragonal crystal structure. The thermal conductivity was measured along both the c- and the a-direction as a function of temperature between 3 and 300 K and in external magnetic fields H up to 69 kOe, oriented both parallel and perpendicular to the c-axis. Distinct features of (T) were observed in the vicinity of TN=11.4 K in zero magnetic field.
These features are unaltered in external fields which are
parallel to the c-axis, but are more pronounced when a field is applied perpendicularly to the c-axis. The transition temperature increases upon enhancing the external field, but only if the field is oriented along the a-axis. 相似文献
13.
Dulić D Hak SJ van der Marel D Hardy WN Koshelev AE Liang R Bonn DA Willemsen BA 《Physical review letters》2001,86(20):4660-4663
We investigated the temperature dependence and c-axis magnetic field dependence of the Josephson plasma resonance in optimally doped Tl2Ba2CaCu2O8 thin films and underdoped YBa2Cu3O6.5 (YBCO) ortho-II single crystals using infrared spectroscopy. We obtained the c-axis penetration depths, at low temperature, in zero fields of about 20 and 7 microm, respectively. While the temperature dependencies of the resonances in the two compounds are very similar, the magnetic field dependence in YBCO is much weaker. We attribute this weak magnetic field dependence to the lower anisotropy of YBCO and interpret the observed behaviors in terms of thermal fluctuations and pinning of pancake vortices. 相似文献
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It is shown that, in an edge superconducting layer of a thin film in a magnetic field perpendicular to the film plane, phase slip centers are formed. The centers arise below the superconducting transition temperature because of the thermal fluctuations of the order parameter and lead to the suppression of superconductivity. The resistance corresponding to such fluctuations is determined, and the contribution of the Aslamazov-Larkin correction to the conductivity of a thin film in magnetic fields slightly exceeding the critical field that breaks the surface superconductivity is calculated. 相似文献
15.
Hess C Elhaes H Waske A Büchner B Sekar C Krabbes G Heidrich-Meisner F Brenig W 《Physical review letters》2007,98(2):027201
We present experimental results for the thermal conductivity kappa of the pseudo-two-leg ladder material CaCu2O3. The strong buckling of the ladder rungs renders this material a good approximation to a S=1/2 Heisenberg chain. Despite a strong suppression of the thermal conductivity of this material in all crystal directions due to inherent disorder, we find a dominant magnetic contribution kappa mag along the chain direction. kappa mag is linear in temperature, resembling the low-temperature limit of the thermal Drude weight D th of the S=1/2 Heisenberg chain. The comparison of kappamag and Dth yields a magnetic mean-free path of l mag approximately 22+/-5 A, in good agreement with magnetic measurements. 相似文献
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We report the temperature and magnetic field dependence of the in-plane thermal conductivity (kappa(ab)) of high-quality monocrystalline Nd2CuO4. Isothermal measurements of the field dependence of kappa(ab) at low temperatures (2 K相似文献
17.
Li Q Liu BT Hu YF Chen J Gao H Shan L Wen HH Pogrebnyakov AV Redwing JM Xi XX 《Physical review letters》2006,96(16):167003
We report a large normal-state magnetoresistance with temperature-dependent anisotropy in very clean epitaxial MgB2 thin films (residual resistivity much smaller than 1 microOmega cm) grown by hybrid physical-chemical vapor deposition. The magnetoresistance shows a complex dependence on the orientation of the applied magnetic field, with a large magnetoresistance (Delta(rho)/(rho)0=136%) observed for the field H perpendicular ab plane. The angular dependence changes dramatically as the temperature is increased, and at high temperatures the magnetoresistance maximum changes to H||ab. We attribute the large magnetoresistance and the evolution of its angular dependence with temperature to the multiple bands with different Fermi surface topology in MgB2 and the relative scattering rates of the sigma and pi bands, which vary with temperature due to stronger electron-phonon coupling for the sigma bands. 相似文献
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The c-axis reflectivity spectrum of underdoped YBa2Cu3O6.6 (YBCO) is measured below T(c)=59 K in parallel magnetic fields H parallel CuO2 up to 7 T. Upon application of a parallel field, a new peak appears at finite frequency in the optical conductivity at the expense of suppression of c-axis condensate weight. We conclude that the dramatic change originates from different Josephson coupling strengths between bilayers with and without Josephson vortices. We find that the 400 cm(-1) broad conductivity peak in YBCO gains the spectral weight under parallel magnetic field; this indicates that the condensate weight at omega=0 is distributed to this peak as well as to the new optical Josephson mode. 相似文献
19.
Dubroka A Kim KW Rössle M Malik VK Drew AJ Liu RH Wu G Chen XH Bernhard C 《Physical review letters》2008,101(9):097011
We present far-infrared ellipsometric measurements of polycrystalline samples of the pnictide superconductor RFeAsO0.82F0.18 (R=Nd and Sm). We find evidence that the electronic properties are strongly anisotropic such that the optical spectra are dominated by the weakly conducting c-axis response similar to the cuprate high-temperature superconductors. We deduce an upper limit of the c-axis superconducting plasma frequency of omega pl,c(SC)< or =260 cm(-1) corresponding to a lower limit of the c-axis magnetic penetration depth of lambda c > or =6 microm and lambda c/lambda ab > or =30 as compared to lambda ab=185 nm from muon spin rotation [A. Drew, arXiv:0805.1042 [Phys. Rev. Lett. (to be published)]]. We also observe a gaplike suppression of the conductivity in the superconducting state with a shoulderlike feature at omegaSC* approximately 300 cm(-1) and spectral shape which is consistent with an unconventional order parameter with 2Delta approximately omegaSC* approximately 37 meV. 相似文献
20.
Tanatar MA Suzuki M Nagai S Mao ZQ Maeno Y Ishiguro T 《Physical review letters》2001,86(12):2649-2652
The dependence of in-plane and interplane thermal conductivities of Sr2RuO4 on temperature, as well as magnetic field strength and orientation, is reported. We found no notable anisotropy in the thermal conductivity for the magnetic field rotation parallel to the conducting plane in the whole range of experimental temperatures and fields, except in the vicinity of the upper critical field H(c2), where the anisotropy of the H(c2) itself plays a dominant role. This finding imposes strong constraints on the possible models of superconductivity in Sr2RuO4 and supports the existence of a superconducting gap with a line of nodes running orthogonal to the Fermi surface cylinder. 相似文献