Ferromagnetic insulating and spin glass properties of La0.7Sr0.3MnO3-TiO2 composites
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作者:
Phone, P. T.
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Dongguk Univ, Dept Adv Mat Chem, Gyeongju Si 780714, Gyeonbuk, South Korea
Nha Trang Pedag Coll, Nha Trang City, Khanh Hoa Provi, VietnamDongguk Univ, Dept Adv Mat Chem, Gyeongju Si 780714, Gyeonbuk, South Korea
Phone, P. T.
[1
,2
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Manh, D. H.
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Vietnam Acad Sci & Technol, Inst Mat Sci, Cau Giay Dist, Ha Noi, VietnamDongguk Univ, Dept Adv Mat Chem, Gyeongju Si 780714, Gyeonbuk, South Korea
Manh, D. H.
[3
]
Phuc, N. X.
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Vietnam Acad Sci & Technol, Inst Mat Sci, Cau Giay Dist, Ha Noi, VietnamDongguk Univ, Dept Adv Mat Chem, Gyeongju Si 780714, Gyeonbuk, South Korea
Phuc, N. X.
[3
]
Lee, I. -J.
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Dongguk Univ, Dept Adv Mat Chem, Gyeongju Si 780714, Gyeonbuk, South KoreaDongguk Univ, Dept Adv Mat Chem, Gyeongju Si 780714, Gyeonbuk, South Korea
Lee, I. -J.
[1
]
机构:
[1] Dongguk Univ, Dept Adv Mat Chem, Gyeongju Si 780714, Gyeonbuk, South Korea
[2] Nha Trang Pedag Coll, Nha Trang City, Khanh Hoa Provi, Vietnam
[3] Vietnam Acad Sci & Technol, Inst Mat Sci, Cau Giay Dist, Ha Noi, Vietnam
In this study, the effect of TiO2 doping on the electro-magnetic properties of (1-x)La0.7Sr0.3MnO3+xTiO(2) (with 0% <= x <= 6%, in wt%) composites has been investigated. X-ray diffraction observations show the evidence of reaction between the La0.7Sr0.3MnO3 and TiO2 grains. Also the results show that by increasing TiO2 doping levels, the metal insulator transition temperatures decrease and the system becomes an insulator. Furthermore, the paramagnetic-ferromagnetic transition temperature also decreases as TiO2 content increases. The spin glass state exists in the composites with x=5% and 6%. The dynamic properties of the magnetic properties are investigated by temperature dependence of dc magnetization and frequency dependence of ac susceptibilities. A dynamic scaling analysis of ac susceptibility data using conventional critical slowing down indicates that a finite spin-glass phase-transition temperature (T-g) and a dynamic exponent (z nu) change from 103 K and 9.30 correspondingly for 0.95La(0.7)Sr(0.3)MnO(3)/0.05TiO(2) to 133 K and 9.10, for 0.94La(0.7)Sr(0.3)MnO(3)/0.06TiO(2). In addition, MR in low temperature of these samples decline simultaneously with occur spin-glass behavior. These results are interpreted as the dilution of Mn3+/Mn4+ interactions by the random Ti substitution on the Mn site considerably reduces the ferromagnetic double exchange interaction within the manganese lattice. (C) 2012 Elsevier B.V. All rights reserved.
机构:
Univ Putra Malaysia, Fac Sci, Dept Phys, Superconductor & Thin Film Lab, Upm 43400, Selangor Darul, MalaysiaUniv Putra Malaysia, Fac Sci, Dept Phys, Superconductor & Thin Film Lab, Upm 43400, Selangor Darul, Malaysia
Awang Kechik, Mohd Mustafa
Chen, Soo Kien
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Univ Putra Malaysia, Fac Sci, Dept Phys, Superconductor & Thin Film Lab, Upm 43400, Selangor Darul, MalaysiaUniv Putra Malaysia, Fac Sci, Dept Phys, Superconductor & Thin Film Lab, Upm 43400, Selangor Darul, Malaysia
Chen, Soo Kien
Ibrahim, Noor Baa'yah
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Univ Kebangsaan Malaysia, Fac Sci & Technol, Dept Appl Phys, Ukm 43600, Selangor Darul, MalaysiaUniv Putra Malaysia, Fac Sci, Dept Phys, Superconductor & Thin Film Lab, Upm 43400, Selangor Darul, Malaysia
Ibrahim, Noor Baa'yah
Miryala, Muralidhar
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Shibaura Inst Technol, Koto Ku, 3 Chome 7-5 Toyosu, Tokyo 1358548, JapanUniv Putra Malaysia, Fac Sci, Dept Phys, Superconductor & Thin Film Lab, Upm 43400, Selangor Darul, Malaysia
Miryala, Muralidhar
Murakami, Masato
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Shibaura Inst Technol, Koto Ku, 3 Chome 7-5 Toyosu, Tokyo 1358548, JapanUniv Putra Malaysia, Fac Sci, Dept Phys, Superconductor & Thin Film Lab, Upm 43400, Selangor Darul, Malaysia
Murakami, Masato
Shaari, Abdul Halim
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Univ Putra Malaysia, Fac Sci, Dept Phys, Superconductor & Thin Film Lab, Upm 43400, Selangor Darul, MalaysiaUniv Putra Malaysia, Fac Sci, Dept Phys, Superconductor & Thin Film Lab, Upm 43400, Selangor Darul, Malaysia
机构:
Changwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South KoreaChangwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South Korea
Bian, Jin Long
Seo, Yong Jun
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Changwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South KoreaChangwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South Korea
Seo, Yong Jun
Kim, Geun Woo
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Changwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South KoreaChangwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South Korea
Kim, Geun Woo
Sung, Chang Hoon
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Changwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South KoreaChangwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South Korea
Sung, Chang Hoon
Kumar, Shalendra
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Changwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South KoreaChangwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South Korea
Kumar, Shalendra
Lee, Chan Gyu
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Changwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South KoreaChangwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South Korea
Lee, Chan Gyu
Koo, Bon Heun
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Changwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South KoreaChangwon Natl Univ, Sch Nano & Adv Mat Engn, Chang Won 641773, South Korea
Koo, Bon Heun
MULTI-FUNCTIONAL MATERIALS AND STRUCTURES III, PTS 1 AND 2,
2010,
123-125
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128
机构:
Indian Inst Technol Madras, Dept Phys, Nanoscale Phys Lab, Chennai 600036, IndiaIndian Inst Technol Madras, Dept Phys, Nanoscale Phys Lab, Chennai 600036, India
Das, Bibekananda
Padhan, Prahallad
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Indian Inst Technol Madras, Dept Phys, Nanoscale Phys Lab, Chennai 600036, India
Indian Inst Technol Madras, Funct Oxides Res Grp, Chennai 600036, IndiaIndian Inst Technol Madras, Dept Phys, Nanoscale Phys Lab, Chennai 600036, India