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 共查询到10条相似文献,搜索用时 15 毫秒
1.
司继伟  曹庆琪  顾本喜  都有为 《中国物理》2005,14(10):2117-2121
A series of polycrystalline Cu-doped n=2 Ruddlesden-Popper manganates La1.2Sr1.8CuzMn(2-x)O7 (x=0, 0.04, 0.13) were synthesized by the solid state reaction method. The effect of Cu doping on the magnetic and transport properties has been studied. It is found that Cu substitution for Mn greatly affects the magnetic and electrical properties of the parent phase La1.2Sr1.8Mn2O7. With the increase of Cu content, the system undergoes a transition from longrange ferromagnetic order to the spin glass state and further to an antiferromagnetic order. A little of Cu dopant can lead to the samples showing semiconductor or insulator behaviour in the whole observed temperature range while the parent phase has a metal-insulator transition. These samples show colossal magnetoresistance at low temperatures and the value of it decreases with increasing Cu content.  相似文献   

2.
Vanadium dioxide thin films have been fabricated through sputtering vanadium thin films and rapid thermal annealing in oxygen. The microstructure and the metal–insulator transition properties of the vanadium dioxide thin films were investigated by X-ray diffraction, X-ray photoelectron spectroscopy, and a spectrometer. It is found that the preferred orientation of the vanadium dioxide changes from(1ˉ11) to(011) with increasing thickness of the vanadium thin film after rapid thermal annealing. The vanadium dioxide thin films exhibit an obvious metal–insulator transition with increasing temperature, and the phase transition temperature decreases as the film thickness increases. The transition shows hysteretic behaviors, and the hysteresis width decreases as the film thickness increases due to the higher concentration carriers resulted from the uncompleted lattice. The fabrication of vanadium dioxide thin films with higher concentration carriers will facilitate the nature study of the metal–insulator transition.  相似文献   

3.
Multiferroic material as a photovoltaic material has gained considerable attention in recent years.Nanoparticles(NPs)La_(0.1)Bi_(0.9-x)Sr_xFeO_y(LBSF,x = 0,0.2,0.4) with dopant Sr~(2+)ions were synthesized by the sol–gel method.A systematic change in the crystal structure from rhombohedral to tetragonal upon increasing Sr doping was observed.There is an obvious change in the particle size from 180 nm to 50 nm with increasing Sr substitution into LBFO.It was found that Sr doping effectively narrows the band gap from~2.08 e V to~1.94 e V,while it leads to an apparent enhancement in the electrical conductivity of LBSF NPs,making a transition from insulator to semiconductor.This suggests an effective way to modulate the conductivity of BiFeO_(3-)based multiferroic materials with pure phase by co-doping with La and Sr at the A sites of BiFeO_3.  相似文献   

4.
徐芳  白洋  艾芬  乔利杰 《中国物理 B》2008,17(12):4652-4655
The magnetic and dielectric properties of Sr-substituted Zn2-Y hexagonal ferrites (Ba2-x SrxZn2Fe12O22, 1.0 〈 x ≤ 1.5) are studied in this paper. Sr substitution will lead to the variation of cation occupation, which influences both the magnetic and electric properties. As Sr content x rises from 1.0 to 1.5, magnetic hysteresis loop gets wider gradually and the permeability drops rapidly due to the transformation from ferrimagnetic to antiferromagnetic phase. Moreover, permittivity rises with increasing Sr content. Under a certain external magnetic field, the phase transition of helical spin structure of Ba0.5Srl.5Zn2Fe12O22 at about 295 K seems to open a possibility for the room-temperature ferroelectricity induced by magnetic field. But its low resistivity prevents the observation of ferroelectric and magnetoelectric properties at room-temperature.  相似文献   

5.
The pseudopotential method has been used to investigate the structural, electronic and magnetic properties of La_(1-x)Eu_xGaO_3(x = 0, 0.25, 0.5, 0.75, and 1) within the scheme of generalized gradient approximation. The spin-polarized calculations demonstrate that the ground state is an antiferromagnetic insulator for x ≤ 0.5, while it is ferromagnetic halfmetal at x 0.5. The substitutions of magnetic Eu ions for non-magnetic La ions produce and strength spin polarization,which forcefully urges the system from the insulator to the half metal. Meanwhile, Eu doping strengthens a stoner mechanism for ferromagnetism of La_(1-x)Eu_xGaO_3(x = 0.75 and 1), which may lead to a rapid increasing in the total magnetic moment and therefore, antiferromagnetic–ferromagnetic transition happens.  相似文献   

6.
ErGa_(3-x)Mn_x disordered alloy is successfully prepared by the vacuum arc melting technology, and the crystal structure and magnetic properties are investigated by using the x-ray diffraction and magnetic measurements. The Rietveld structural analysis indicates that the ErGa_(3-x)Mn_x crystallizes into a cubic structure with space group of Pm3m in Mn doping range of x = 0–0.1. However, the disordered alloy with structural formula of Er_(0.8)Ga_2~Ⅰ(Ga~Ⅱ, Mn)0.4 as the second phase is separated from cubic phase for the samples with x = 0.2 and 0.3, which is induced by substituting the(Ga~Ⅱ, Mn)–(Ga~Ⅱ, Mn) pair at 2e crystal position for the rare earth Er at 1 a site. The lattice parameters tend to increase with Mn content increasing due to the size effect at Ga(1.30°A) site by substituting Mn(1.40°A) for Ga. The paramagnetic characteristic is observed by doping Mn into ErGa_3 at room temperature. With Mn content increasing from x = 0 to 0.1, the magnetic susceptibility χtends to increase. This phenomenon can be due to the increase of effective potential induced by doping Mn into ErGa_3.However, the magnetic susceptibility χ continues to decrease with the increase of Mn content in a range of x 0.2, which is due to the phase separation from the cubic Er(Ga, Mn)_3 to the hexagonal Er_(0.8)Ga_2(Ga, Mn)_(0.4).  相似文献   

7.
In this article, the influence of La substitution for Sr on structure and physi-cal properties of the 2201 phase is studied. First, the crystal microstructure of the Bi2.1Sr1.9-xLaxCuOy (0≤x≤1.0) is characterized by means of X-ray diffraction and electron diffraction analyses, it is discovered that in the La-doped 2201 system with increasing La content the 2201 phase undergoes tetragnoal-orthorhombic-monoclinic structural transition. With this phase transition, the modulation vector of the 2201 phase transforms from incommensurate to commensurate, and the period of the mod- ulation wave decreases. Secondly, the superconductivity of this system is analyzed systematically. The results of the resistivity measurement show that the appropriate amount of La doping can raise the superconducting transition temperature (Tc) of the 2201 phase, with x=0.2, Tc reaches as high as 25K. However the excessive doping of La (x≥0.3) leads the 2201 phase to transit from metal to insulator and the su-perconductivity disappears. The measurement of thermoelectric power (TEP) of this system shows that with increasing La content the TEP value also increases gradu-ally. But the interesting point is that the transition from positive to negative in TEP occurs for x=0.2 sample. In addition, the electronic structure and oxygen content of this system are also studied. Based on these, we analyze the relation between the microstructure, electronic structure of the La-doped 2201 phase and its superconduc-tivity, indicating that the type of element substitution with higher valence, together with the microstructural distortion induced by the substitution affects the electronic states of Cu 3d seriously, that is, changes the degree of coulomb correlation of Cu 3d electrons, thus resulting in the transition of the type of carrier of this system and the decrease of hole carrier concentration, as well as the corresponding variation of the superconductivity of La-doped 2201 phase.  相似文献   

8.
The heavy fermion ferromagnet CeRh_6 Ge_4 is the first example of a clean stoichiometric system where the ferromagnetic transition can be continuously suppressed by hydrostatic pressure to a quantum critical point.In order to reveal the outcome when the magnetic lattice of CeRh_6 Ge_4 is diluted with non-magnetic atoms,this study reports comprehensive measurements of the physical properties of both single crystal and polycrystalline samples of La_xCe_(1-x)Rh_6 Ge_4.With increasing x,the Curie temperature decreases,and no transition is observed for x0.25,while the system evolves from exhibiting coherent Kondo lattice behaviors at low x to the Kondo impurity scenario at large x.Moreover,non-Fermi liquid behavior is observed over a wide doping range,which agrees well with the disordered Kondo model for 0.52≤x≤0.66,while strange metal behavior is revealed in the vicinity of x_c=0.26.  相似文献   

9.
郑琳  鲁毅  赵建军  张向群  邢茹  吴鸿业  金香  周敏  成昭华 《中国物理 B》2010,19(12):127501-127501
The effect of Dy substitution for La site in layered manganese oxides La1.3-x Dyx Sr1.7 Mn2O7 on the magnetic and electrical properties has been investigated.With the La 3+ substituting by Dy3+,the long range three-dimensional ferromagnetism transition and the insulator-metal transition disappear.These effects are attributed to the lattice distortion due to the substitution of the smaller Dy3+.Addtionally,the small Dy3+ is inclined to occupy the R site which is in the rock-salt layer,then the distribution of La,Sr,Dy ions in Dy-doped sample should be more orderly than that in La1.3 Sr1.7 Mn2O7,so there is only one insulator-metal transition in the ρ-T curve of the sample with x = 0.05 and x = 0.1.  相似文献   

10.
Mott transition in a ruby lattice with fermions described by the Hubbard model including on-site repulsive interaction is investigated by combining the cellular dynamical mean-field theory and the continuous-time quantum Monte Carlo algorithm. The effect of temperature and on-site repulsive interaction on the metallic–insulating phase transition in ruby lattice with fermions is discussed based on the density of states and double occupancy. In addition, the magnetic property of each phase is discussed by defining certain magnetic order parameters. Our results show that the antiferromagnetic metal is found at the low temperature and weak interaction region and the antiferromagnetic insulating phase is found at the low temperature and strong interaction region. The paramagnetic metal appears in whole on-site repulsive interaction region when the temperature is higher than a certain value and the paramagnetic insulator appears at the middle scale of temperature and on-site repulsive interaction.  相似文献   

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