稀有金属材料与工程
稀有金屬材料與工程
희유금속재료여공정
RARE METAL MATERIALS AND ENGINEERNG
2009年
z2期
987-990
,共4页
刘晓芳%龚维幂%潘崇超%杨松林%贺博%于荣海
劉曉芳%龔維冪%潘崇超%楊鬆林%賀博%于榮海
류효방%공유멱%반숭초%양송림%하박%우영해
稀磁半导体%纳米棒%Co掺杂SnO_2%铁磁性
稀磁半導體%納米棒%Co摻雜SnO_2%鐵磁性
희자반도체%납미봉%Co참잡SnO_2%철자성
diluted magnetic semiconductor%nanorods%Co-doped SnO_2%ferromagnetism
采用水热法制备了Co掺杂的SnO_2纳米棒.随着Co掺杂浓度的增加,样品的室温铁磁性先增加后降低,当Co掺杂浓度为4%时,样品的饱和磁化强度达到最大值.纳米棒呈花簇状生长,单根纳米棒长度约300 nm,为单晶金红石型SnO_2相.X射线光电子能谱和X射线近边结构谱分析表明,Co在SnO_2样品中以+2价态存在,替代了Sn~(4+)离子的位置,并未与其它元素形成杂质相,从而证明室温铁磁性为Sn_(1-x)Co_xO_2纳米棒的本征性能.同时,采用自旋分裂杂质带模型,解释了Co掺杂浓度对样品室温铁磁性的调节作用.
採用水熱法製備瞭Co摻雜的SnO_2納米棒.隨著Co摻雜濃度的增加,樣品的室溫鐵磁性先增加後降低,噹Co摻雜濃度為4%時,樣品的飽和磁化彊度達到最大值.納米棒呈花簇狀生長,單根納米棒長度約300 nm,為單晶金紅石型SnO_2相.X射線光電子能譜和X射線近邊結構譜分析錶明,Co在SnO_2樣品中以+2價態存在,替代瞭Sn~(4+)離子的位置,併未與其它元素形成雜質相,從而證明室溫鐵磁性為Sn_(1-x)Co_xO_2納米棒的本徵性能.同時,採用自鏇分裂雜質帶模型,解釋瞭Co摻雜濃度對樣品室溫鐵磁性的調節作用.
채용수열법제비료Co참잡적SnO_2납미봉.수착Co참잡농도적증가,양품적실온철자성선증가후강저,당Co참잡농도위4%시,양품적포화자화강도체도최대치.납미봉정화족상생장,단근납미봉장도약300 nm,위단정금홍석형SnO_2상.X사선광전자능보화X사선근변결구보분석표명,Co재SnO_2양품중이+2개태존재,체대료Sn~(4+)리자적위치,병미여기타원소형성잡질상,종이증명실온철자성위Sn_(1-x)Co_xO_2납미봉적본정성능.동시,채용자선분렬잡질대모형,해석료Co참잡농도대양품실온철자성적조절작용.
SnO_2 nanorods with different concentration of Co dopants were prepared by hydrothermal method. With the increase in the concentration of Co, room temperature ferromagnetism of the samples initially increases and then decreases. The highest value of saturated magnetization occurs in the sample with the Co concentration of 4%. Morphology analyses indicate that the nanorods grow in flower cluster, and the length of single nanorod is approximate 300 nm. XPS and XANES techniques reveal a solid solution of Co dopants in SnO_2 lattice, where Co is in 2+ oxidation state substituting for Sn~(4+). Due to the elimination of impurity phases, it is confirmed that the observed ferromagnetism is the intrinsic nature of the system. Using impurity band model, we demonstrate the dependence of ferromagnetism on Co concentration and elucidate the origin of ferromagnetism.