The effect of artificial boundary grain on the magneto- and electro-transport properties of (1 − x)La0.7Ca0.3MnO3 + xA (A = Al2O3 and Ag) nanocomposite
Tiếng Anh
Tóm tắt
The magneto- and electro-transport properties of two series of nanocrystalline
(1 − x)La0.7Ca0.3MnO3 + xA (A: Al2O3 and Ag) composites have been systematically and
thoroughly studied. The observed electronic transport behavior over the whole temperature
range (5–300 K), especially the change in metal–insulator transition temperature with
increasing Al2O3 and Ag content while the ferromagnetic–paramagnetic transition remained
unaffected, was explained by applying a two-component phenomenological model. We have
attributed the unusual low-temperature resistivity upturn of composites to a change in charging
energy. Most interestingly, magneto-transport measurements showed that the low-field
magnetoresistance (LFMR), as well as the high-field magnetoresistance (HFMR), displayed a
Curie–Weiss-like law behavior. Basing on the spin-polarized transport of conduction electrons
at the grain boundaries, we have analyzed our experimental data and found that the
temperature dependence of low- and high-field magnetoresistance is controlled predominantly
by the nature of the temperature response of surface magnetization of particles. The
competition between grain-boundary pinning strength (k), magnetic field and thermal energy
(kBT ) created the temperature sensitive behavior of magnetoresistance as well as that of
surface spin susceptibility (χb).
Từ khoá
Keywords: manganite composites, low-field magnetoresistance, polarized tunneling
Tài liệu tham khảo
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[2] Hwang H Y, Cheong S W, Ong N P and Batlogg B 1996 Phys. Rev. Lett. 77 2041
[3] Gupta A and Sun J S 1999 J. Magn. Magn. Mater. 200 24
[4] Sandu V, Popa S, Ivan I, Plapcianu C, Sandu E, Hurduc N and Nor I 2009 Proc. SPIE 7493 74934F-1
[5] Balcells L, Fontcuberta J, Martínez B and Obradors X 1998 J. Phys.: Condens. Matter. 10 1883
[6] Gaur A and Varma G D 2008 J. Alloys Compd. 453 423
[7] Phong P T, Khiem N V, Dai N V, Manh D H, Hong L V and Phuc N X 2009 Mater. Lett. 63 353
[8] Kumar J, Singh R K, Singh H K, Siwach P K, Ramadhar Singh and Srivastava O N 2008 J. Alloys Compd. 455 289
[9] Miao J H, Yuan S L, Yuan L, Ren G M, Xiao X, Yu G Q, Wang Y Q and Yin S Y 2008 Mater. Res. Bull. 43 631
[10] Eshraghi M, Salamati H and Kameli P 2007 J. Alloys Compd. 437 22
[11] Hong C S, Kim W S and Hur N H 2002 Solid State Commun. 121 657 [12] Gaur A and Varma G D 2006 Solid State Commun. 139 310
[13] Khiem N V, Phong P T, Dai N V, Manh D H, Hong L V and Phuc N X 2009 Mater. Lett. 63 899
[14] Awana V P S, Tripathi R, Balamurugan S, Kishan H and Takayama-Muromachi E 2006 Solid State Commun. 140 410
[15] Phong P T, Khiem N V, Dai N V, Manh D H, Hong L V and Phuc N X 2009 J. Alloys Compd. 484 12
[16] Xiong C, Hu H, Xiong Y, Zhang Z, Pi H, Wu X, Li L, Wei F and Zheng C 2009 J. Alloys Compd. 479 357
[17] Phong P T, Dai N V, Manh D H, Khiem N V, Hong L V and Phuc N X 2009 J. Alloys Compd. 485 L39
[18] Phong P T, Khiem N V, Dai N V, Manh D H, Hong L V and Phuc N X 2009 J. Magn. Magn. Mater. 321 3330
[19] Thanh T D, Phong P T, Dai N V, Manh D H, Khiem N V, Hong L V and Phuc N X 2011 J. Magn. Magn. Mater. 323 179
[20] Lee S, Hwang H Y, Shraiman B I, Ratcliff W D II and Cheong S-W 1999 Phys. Rev. Lett. 82 4508
[21] de Andres, Garcia-Hernandez M and Martinez J L 1999 Phys. Rev. B 60 7328 8 Adv. Nat. Sci.: Nanosci. Nanotechnol. 2 (2011) 025003 T P Pham et al
[22] Rubinstein J M 2000 J. Appl. Phys. 87 5019
[23] Das D, Srivastava, Bahadur D, Nigam A K and Malik S K 2004 J. Phys.: Condens. Matter 16 4089
[24] Li J, Huang Q, Li Z W, You L P, Xu S Y and Ong C K 2001 J. Appl. Phys. 89 7428
[25] Sheng P, Abeles B and Arie Y 1973 Phys. Rev. B 31 44
[26] Raychaudhuri P, Sheshadri K, Taneja P, Bandyopadhyay S, Ayyub P, Nigam A K and Pinto R 1998 J. Appl. Phys. 84 2048
[27] Dey P and Nath T K 2006 Phys. Rev. B 73 214425