Enhanced Ferromagnetism and Microwave Dielectric Properties of Bi0.95Y0.05FeO3 Nanocrystals
HOU Zhi-Ling1**, ZHOU Hai-Feng1, YUAN Jie2, KANG Yu-Qing2, YANG Hui-Jing2, JIN Hai-Bo2, CAO Mao-Sheng2**
1School of Science, Beijing University of Chemical Technology, Beijing 100029 2School of Materials Science and Engineering, Beijing Institute of Technology, Beijing 100081
Enhanced Ferromagnetism and Microwave Dielectric Properties of Bi0.95Y0.05FeO3 Nanocrystals
HOU Zhi-Ling1**, ZHOU Hai-Feng1, YUAN Jie2, KANG Yu-Qing2, YANG Hui-Jing2, JIN Hai-Bo2, CAO Mao-Sheng2**
1School of Science, Beijing University of Chemical Technology, Beijing 100029 2School of Materials Science and Engineering, Beijing Institute of Technology, Beijing 100081
摘要Bi0.95Y0.05FeO3 nanocrystals are synthesized by a hydrothermal method, and are crystallized in a rhombohedrally distorted perovskite BiFeO3 structure in the R3c space, with compressive lattice distortion induced by the Y substitution at Bi sites from XRD study. Compared with BiFeO3 gained under similar conditions, the magnetic properties are greatly enhanced, with saturate magnetization of 2.3 emu/g at room temperature. Microwave dielectric properties of Bi0.95Y0.05FeO3 nanocrystals are investigated in the range of 2–18 GHz. The Y substitution results in the increase of permeability and decrease of permittivity, which are attributed to the enhanced spin relaxation of domain wall motion and the weakened electron-relaxation caused by decreasing Fe2+, respectively. The changes for microwave dielectric response could lead to the excellent microwave absorption due to the improvement of the impedance match between BiFeO3 and air.
Abstract:Bi0.95Y0.05FeO3 nanocrystals are synthesized by a hydrothermal method, and are crystallized in a rhombohedrally distorted perovskite BiFeO3 structure in the R3c space, with compressive lattice distortion induced by the Y substitution at Bi sites from XRD study. Compared with BiFeO3 gained under similar conditions, the magnetic properties are greatly enhanced, with saturate magnetization of 2.3 emu/g at room temperature. Microwave dielectric properties of Bi0.95Y0.05FeO3 nanocrystals are investigated in the range of 2–18 GHz. The Y substitution results in the increase of permeability and decrease of permittivity, which are attributed to the enhanced spin relaxation of domain wall motion and the weakened electron-relaxation caused by decreasing Fe2+, respectively. The changes for microwave dielectric response could lead to the excellent microwave absorption due to the improvement of the impedance match between BiFeO3 and air.
[1] Wang K F, Liu J M and Ren Z F 2009 Adv. Phys. 58 321
[2] Tokunaga Y, Furukawa N, Sakai H, Taguchi Y, Arima T H and Tokura Y 2009 Nature Mater. 8 558
[3] Liu J M, Chan-Wong L W and Choy C L 2009 Chin. Phys. Lett. 26 087501
[4] Feng H J and Liu F M 2008 Chin. Phys. Lett. 25 671
[5] Huang N X, Zhao L F, Xu J Y, Chen J L and Zhao Y 2010 Chin. Phys. Lett. 27 027704
[6] Wang J, Li M Y, Liu X L, Pei L, Liu J, Yu B F and Zhao X Z 2009 Chin. Phys. Lett. 26 117301
[7] Rovillain P, de Sousa R, Gallais Y, Sacuto A, Measson M A, Colson D, Forget A, Bibes M, Barthelemy A and Cazayous M 2010 Nature Mater. 9 975
[8] Fischer P, Polomska M, Sosnowska I and Szymanski M 1980 J. Phys. C: Solid State Physics 13 1931
[9] Zhang Q, Kim C H, Jang Y H, Hwang H J and Cho J H 2010 Appl. Phys. Lett. 96 152901
[10] Xu Q Y, Zai H F, Wu D, Qiu T and Xu M X 2009 Appl. Phys. Lett. 95 112510
[11] Troyanchuk I O, Chobot A N, Mantytskaya O S and Tereshko N V 2010 Inorg. Mater. 46 424 1
[12] Hojamberdiev M, Xu Y, Wang F, Liu W and Wang J 2009 Inorg. Mater. 45 1183
[13] Qian F Z, Jiang J S, Guo S Z, Jiang D M and Zhang W G 2009 J. Appl. Phys. 106 084312
[14] Uniyal P and Yadav K L 2009 J. Appl. Phys. 105 07D914
[15] Zhang Y J, Zhang H G, Yin J H, Zhang H W, Chen J L, Wang W Q and Wu G H 2010 J. Magn. Magn. Mater. 322 2251
[16] Li J B, Rao G H, Xiao Y, Liang J K, Luo J, Liu G Y and Chen J R 2010 Acta Materialia 58 3701
[17] Lin Y H, Jiang Q H, Wang Y, Nan C W, Chen L and Yu J 2007 Appl. Phys. Lett. 90 172507
[18] Liu J, Fang L, Zheng F G, Ju S and Shen M R 2009 Appl. Phys. Lett. 95 022511
[19] Li J B, Rao G H, Xiao Y G, Luo J, Liu G Y, Chen J R and Liang J K 2010 Chin. Phys. B 19 107505
[20] Du Y, Cheng Z X, Shahbazi M, Collings E W, Dou S X and Wang X L 2010 J. Alloys Compd. 490 637
[21] Thakuria P and Joy P A 2010 Appl. Phys. Lett. 97 162504
[22] Song W L, Cao M S, Hou Z L, Yuan J and Fang X Y 2009 Scripta Mater. 61 201
[23] Zhang X Y, Song Q, Xu F and Ong C K 2009 Appl. Phys. Lett. 94 022907
Ahad F B A, Hung D S, Yao Y D, Lee S F, Tu C S, Wang T H, Chen Y Y and Fu Y P 2009 J. Appl. Phys. 105 07D912
[24] Xu J H, Ke H, Jia D C, Wang W and Zhou Y 2009 Philos. Mag. Lett. 89 701
[25] Kang Y Q, Cao M S, Yuan J and Shi X L 2009 Mater. Lett. 63 1344
[26] Wen F S, Wang N and Zhang F 2010 Solid State Comm. 150 1888
[27] Mazumder R, Devi P S, Bhattacharya D, Choudhury P, Sen A and Raja M 2007 Appl. Phys. Lett. 91 062510
[28] Hunpratub S, Thongbai P, Yamwong T, Yimnirun R and Maensiri S 2009 Appl. Phys. Lett. 94 062904
[29] Lou Y H, Song G L, Chang F G and Wang Z K 2010 Chin. Phys. B 19 077702
[30] Hou Z L, Cao M S, Yuan J and Song W L 2010 Chin. Phys. B 19 017702
[31] Cao M S, Qin R R, Qiu C J and Zhu J 2003 Mater. Design 24 391