Griffiths phase;
Nd0.5Sr0.5MnO3;
Transport;
Magnetic property;
METAL-INSULATOR-TRANSITION;
MAGNETIC STATES;
SEPARATION;
MANGANITES;
CHARGE;
FIELD;
INHOMOGENEITIES;
CONDUCTIVITY;
LA1-XSRXMNO3;
DENSITY;
D O I:
10.1016/j.jmmm.2013.01.009
中图分类号:
T [工业技术];
学科分类号:
08 ;
摘要:
This work is devoted to study the influence of the Griffiths phase in colossal magnetoresistance manganites. Griffiths-phase-like behavior of the paramagnetic susceptibility chi(0) is observed in Nd0.5Sr0.5MnO3 oxygen-deficient thin films fabricated by magnetron sputtering deposition. In Nd0.5Sr0.5MnO3-delta films with oxygen deficiency for T-G approximate to 260-280 K > T > T-C = 138 K (T-G and T-C-Griffiths and Curie temperatures, respectively), paramagnetic matrix consists of a magnetic phase with short-range order (similar to 1-1.5 nm) (which is responsible for the colossal magnetoresistance (CMR) above T-C), and is embedded in this matrix region with long-range ferromagnetic order (>> 10 nm), responsible for the Griffiths phase-like behavior of the paramagnetic susceptibility. Electrical resistivity is caused by carrier tunneling between the localized states and obeys the Efros-Shklovskii law. Magnetic resistivity is caused by change of the localized state sizes under the magnetic field. The temperature and magnetic field dependencies of size of the phase inhomogeneity inclusions, found from measurements of magneto-transport properties, can be satisfactorily described by the model of thermodynamic phase separation into metallic droplets of small radius in a paramagnetic matrix. Intrinsic nanoscale inhomogeneities caused by thermodynamic phase separation, rather than the Griffiths phase, determine the electrical resistivity and colossal magnetoresistance of the films. In half-doped manganites, the nature of long-range ordered magnetic phases may be related, besides the chemical heterogeneity, to proximity to a ferromagnetic-antiferromagnetic boundary at the phase diagram as well. The results are in good agreement with the model of existence of an analog of Griffiths phase temperature in half-doped manganites. (C) 2013 Elsevier B.V. All rights reserved.
机构:
Xi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
Xi An Jiao Tong Univ, MOE Key Lab Nonequilibrium Synth & Modulat Conden, Xian 710054, Peoples R ChinaXi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
Liu, Yao
Ma, Tianyu
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机构:
Xi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
Xi An Jiao Tong Univ, MOE Key Lab Nonequilibrium Synth & Modulat Conden, Xian 710054, Peoples R ChinaXi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
Ma, Tianyu
Qiao, Kaiming
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h-index: 0
机构:
Chinese Acad Sci, Inst Phys, Beijing Natl Lab Condensed Matter Phys, Beijing 100190, Peoples R China
Chinese Acad Sci, Inst Phys, State Key Lab Magnetism, Beijing 100190, Peoples R ChinaXi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
Qiao, Kaiming
Li, Jia
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机构:
Chinese Acad Sci, Inst Phys, Beijing Natl Lab Condensed Matter Phys, Beijing 100190, Peoples R China
Chinese Acad Sci, Inst Phys, State Key Lab Magnetism, Beijing 100190, Peoples R ChinaXi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
Li, Jia
Xiao, Andong
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机构:
Xi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
Xi An Jiao Tong Univ, MOE Key Lab Nonequilibrium Synth & Modulat Conden, Xian 710054, Peoples R ChinaXi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
Xiao, Andong
Wang, Jing
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机构:
Chinese Acad Sci, Inst Phys, Beijing Natl Lab Condensed Matter Phys, Beijing 100190, Peoples R China
Chinese Acad Sci, Inst Phys, State Key Lab Magnetism, Beijing 100190, Peoples R ChinaXi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
Wang, Jing
Hu, Fengxia
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机构:
Chinese Acad Sci, Inst Phys, Beijing Natl Lab Condensed Matter Phys, Beijing 100190, Peoples R China
Chinese Acad Sci, Inst Phys, State Key Lab Magnetism, Beijing 100190, Peoples R China
Songshan Lake Mat Lab, Dongguan 523808, Guangdong, Peoples R ChinaXi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
Hu, Fengxia
Shen, Baogen
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机构:
Chinese Acad Sci, Inst Phys, Beijing Natl Lab Condensed Matter Phys, Beijing 100190, Peoples R China
Chinese Acad Sci, Inst Phys, State Key Lab Magnetism, Beijing 100190, Peoples R ChinaXi An Jiao Tong Univ, Frontier Inst Sci & Technol, State Key Lab Mech Behav Mat, Xian 710054, Peoples R China
机构:
Zhejiang Normal Univ, Dept Phys, Jinhua 321004, Peoples R China
Univ Hong Kong, Dept Phys, Hong Kong, Hong Kong, Peoples R ChinaZhejiang Normal Univ, Dept Phys, Jinhua 321004, Peoples R China
Chen, Liping
Guo, Xuexiang
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机构:
Zhejiang Normal Univ, Dept Phys, Jinhua 321004, Peoples R ChinaZhejiang Normal Univ, Dept Phys, Jinhua 321004, Peoples R China
Guo, Xuexiang
Gao, J.
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h-index: 0
机构:
Univ Hong Kong, Dept Phys, Hong Kong, Hong Kong, Peoples R ChinaZhejiang Normal Univ, Dept Phys, Jinhua 321004, Peoples R China