Polycrystalline samples of Lal-x(Srl-yAgy)x MnO3 (y = 0.0, 0.2, 0.4, 0.6, 1.0) were prepared by the solid-state reaction method. The temperature stability of magnetoresistance and magnetoresistance enhancement in ...Polycrystalline samples of Lal-x(Srl-yAgy)x MnO3 (y = 0.0, 0.2, 0.4, 0.6, 1.0) were prepared by the solid-state reaction method. The temperature stability of magnetoresistance and magnetoresistance enhancement in Lal_x(Srl_yAgy)~MnO3 system with both univalent and bivalent elements doped at A site and with unchanged value of Mn~+/Mn4+ ratio were explored through the measurements of X-ray diffraction patterns, magnetiza- tion-temperature (M-T) curves, resistivity-temperature (p-T) curves and magnetoresistance-temperature (MR-T) curves. The results are as follows: there are two peaks in the p-T curves of the samples with Ag doping, one is caused by resistance change during the paramagnetism- ferromagnetism transition, and the other is from boundary- dependent scattering of conduction electrons on the boundaries of grains. The peak value of MR increases with increasing Ag doping content, and it increases from 8.2 % for y ---- 0.2 to 29.6 % for y ---- 1.0 under the magnetic field of B = 0.8 T; MR remains a constant of 12 % in the temperature range of 218-168 K for the sample with y = 1.0, and the temperature stability of MR is in favor of the practical application of MR.展开更多
The effect of cobalt-doping on the magnetic,transport and magnetoresistance characteristics of La1-xSrxMnO3 was investigated.The results show that the magnetoelectric property of rare-earth doped manganites is greatly...The effect of cobalt-doping on the magnetic,transport and magnetoresistance characteristics of La1-xSrxMnO3 was investigated.The results show that the magnetoelectric property of rare-earth doped manganites is greatly affected by substitution of Co for Mn sites.The Curie temperature as well as the magnetic moment decreases with the increase of doping concentration,and the samples exhibit obvious characteristics of the spin glass state.Moreover,the magnetoresistance is evidently modulated by doping concentration,and the relevant temperature dependence is also suppressed.In addition,low-temperature magnetoresistance is significantly promoted as doping concentration increases,which renders a value of approximately 50% in the temperature range of 5-200 K and varies within 12.5%.It can be attributed to the effect of spin scattering, induced by cobalt doping,on the itinerant electrons of Mn ions,thus introducing a spin-disorder region into the ferromagnetic region of double-exchange interaction between neighbouring Mn^3+ and Mn^4+ ions.展开更多
The samples of La0.80Sr0.15Ag0.05MnO3/x(CuO) (x = 0, 0.05, 0.10, 0.15, 0.20) were prepared by the solid-state reaction method, and the structure of the sampies was detected by X-ray diffraction (XRD), scanning e...The samples of La0.80Sr0.15Ag0.05MnO3/x(CuO) (x = 0, 0.05, 0.10, 0.15, 0.20) were prepared by the solid-state reaction method, and the structure of the sampies was detected by X-ray diffraction (XRD), scanning electron microscope (SEM) equipped with energy dispersive spectroscopy (EDS), electric transport mechanism, and magnetoresistance enhancement, and the temperature stability of magnetoresistance of the samples was studied through resistivity-temperature (ρ-T) curves, ρ-T fitted curves, and magnetoresistance-temperature (MR-T) curves. The results indicate that ρ-T data can be fitted by the formula ρ = ρ0 + AT^2 very well, and the electric transport mechanism of all the samples in metal-like area is the scattering of single magneton upon spin electron; the magnetoresistance of composite samples is far larger than that of the original material, and the MR peak value of the sample with x = 0.20 is nearly 4 times as large as that of the sample with x = 0; composite samples have comparatively good temperature stability of magnetoresistance in the temperature range of 200-260 K, and the magnetoresistance of the sample with x = 0.15 almost does not change with temperature and keeps at (5.03 ± 0.20) % in the temperature range of 210-260 K.展开更多
基金supported by the National Natural Foundation of China (No. 19934003)the Natural Science Research Key Program of Anhui Educational Committee (No. KJ2011A259)+2 种基金the Cultivating Base of Anhui Key Laboratory of Spintronics and Nano-materials Research Program(No. 2010YKF01No. 2010YKF04)the Professors’ and Doctors’ Research Startup Foundation of Suzhou University (Nos. 2011jb01 and 2011jb02)
基金financially supported by the National Natural Science Foundation of China(NSFC)(No.19934003)the Key Program of Natural Science Foundation of Anhui Province(No.KJ2011A259)+1 种基金the Program of Professors and Doctors'Research Startup Foundation of Suzhou College(Nos.2011jb01 and 2011jb02)the Cultivating Base of Anhui Key Laboratory of Spintronics and Nano-materials Research Program(No.2010YKF04)
文摘Polycrystalline samples of Lal-x(Srl-yAgy)x MnO3 (y = 0.0, 0.2, 0.4, 0.6, 1.0) were prepared by the solid-state reaction method. The temperature stability of magnetoresistance and magnetoresistance enhancement in Lal_x(Srl_yAgy)~MnO3 system with both univalent and bivalent elements doped at A site and with unchanged value of Mn~+/Mn4+ ratio were explored through the measurements of X-ray diffraction patterns, magnetiza- tion-temperature (M-T) curves, resistivity-temperature (p-T) curves and magnetoresistance-temperature (MR-T) curves. The results are as follows: there are two peaks in the p-T curves of the samples with Ag doping, one is caused by resistance change during the paramagnetism- ferromagnetism transition, and the other is from boundary- dependent scattering of conduction electrons on the boundaries of grains. The peak value of MR increases with increasing Ag doping content, and it increases from 8.2 % for y ---- 0.2 to 29.6 % for y ---- 1.0 under the magnetic field of B = 0.8 T; MR remains a constant of 12 % in the temperature range of 218-168 K for the sample with y = 1.0, and the temperature stability of MR is in favor of the practical application of MR.
基金Project suppprted by the doctor start-up fund of the Southwest University of Science and Technology of China (Grant No07ZX0110)
文摘The effect of cobalt-doping on the magnetic,transport and magnetoresistance characteristics of La1-xSrxMnO3 was investigated.The results show that the magnetoelectric property of rare-earth doped manganites is greatly affected by substitution of Co for Mn sites.The Curie temperature as well as the magnetic moment decreases with the increase of doping concentration,and the samples exhibit obvious characteristics of the spin glass state.Moreover,the magnetoresistance is evidently modulated by doping concentration,and the relevant temperature dependence is also suppressed.In addition,low-temperature magnetoresistance is significantly promoted as doping concentration increases,which renders a value of approximately 50% in the temperature range of 5-200 K and varies within 12.5%.It can be attributed to the effect of spin scattering, induced by cobalt doping,on the itinerant electrons of Mn ions,thus introducing a spin-disorder region into the ferromagnetic region of double-exchange interaction between neighbouring Mn^3+ and Mn^4+ ions.
基金financially supported by the Key Program of National Natural Science Foundation of China(No.19934003)the Program of Natural Science Foundation of Anhui Province(No.1308085MA11)+1 种基金the Key Programs of Natural Science Research of Anhui Education Department(Nos.KJ2013A245 and KJ2012Z404)the Open Projects of Anhui Key Laboratory of Spintronic and Nanometric Materials(Nos.2012YKF09,2012YKF10,and 2012YKF08)
文摘The samples of La0.80Sr0.15Ag0.05MnO3/x(CuO) (x = 0, 0.05, 0.10, 0.15, 0.20) were prepared by the solid-state reaction method, and the structure of the sampies was detected by X-ray diffraction (XRD), scanning electron microscope (SEM) equipped with energy dispersive spectroscopy (EDS), electric transport mechanism, and magnetoresistance enhancement, and the temperature stability of magnetoresistance of the samples was studied through resistivity-temperature (ρ-T) curves, ρ-T fitted curves, and magnetoresistance-temperature (MR-T) curves. The results indicate that ρ-T data can be fitted by the formula ρ = ρ0 + AT^2 very well, and the electric transport mechanism of all the samples in metal-like area is the scattering of single magneton upon spin electron; the magnetoresistance of composite samples is far larger than that of the original material, and the MR peak value of the sample with x = 0.20 is nearly 4 times as large as that of the sample with x = 0; composite samples have comparatively good temperature stability of magnetoresistance in the temperature range of 200-260 K, and the magnetoresistance of the sample with x = 0.15 almost does not change with temperature and keeps at (5.03 ± 0.20) % in the temperature range of 210-260 K.