磁性材料及器件
磁性材料及器件
자성재료급기건
JOURNAL OF MAGNETIC MATERIALS AND DEVICES
2013年
5期
15-18,53
,共5页
刘艳芬%刘晓华%孙为民%刘晓军%林方婷
劉豔芬%劉曉華%孫為民%劉曉軍%林方婷
류염분%류효화%손위민%류효군%림방정
Fe/Ni体系超晶格%推迟模式%禁带宽度%体极化子
Fe/Ni體繫超晶格%推遲模式%禁帶寬度%體極化子
Fe/Ni체계초정격%추지모식%금대관도%체겁화자
Fe/Ni superlattice%retarded modes%forbidden bandwidth%bulk polaron
基于等效介质理论计算了半无限侧向 Fe/Ni 体系超晶格的体模式,通过对体极化子禁带宽度的讨论给出了自旋波在该体系下传播区域的改变。外场较小时磁性层的磁比例因子与外场对禁带宽度的影响规律性较强,Ni层越厚、外场越大禁带宽度越大。外场增大使趋肤效应与涡流损耗效应增强,导致自旋波衰减,禁带宽度变化情况复杂化。讨论结果与J.Barnas利用传输矩阵方法算出的磁性/非磁性超晶格推迟模式的体极化子的色散曲线很相似。对比发现,等效介质理论更具简便性,在所研究体系中第二种磁性介质的饱和磁化强度趋于0时即为J.Barnas的磁性/非磁性超晶格。
基于等效介質理論計算瞭半無限側嚮 Fe/Ni 體繫超晶格的體模式,通過對體極化子禁帶寬度的討論給齣瞭自鏇波在該體繫下傳播區域的改變。外場較小時磁性層的磁比例因子與外場對禁帶寬度的影響規律性較彊,Ni層越厚、外場越大禁帶寬度越大。外場增大使趨膚效應與渦流損耗效應增彊,導緻自鏇波衰減,禁帶寬度變化情況複雜化。討論結果與J.Barnas利用傳輸矩陣方法算齣的磁性/非磁性超晶格推遲模式的體極化子的色散麯線很相似。對比髮現,等效介質理論更具簡便性,在所研究體繫中第二種磁性介質的飽和磁化彊度趨于0時即為J.Barnas的磁性/非磁性超晶格。
기우등효개질이론계산료반무한측향 Fe/Ni 체계초정격적체모식,통과대체겁화자금대관도적토론급출료자선파재해체계하전파구역적개변。외장교소시자성층적자비례인자여외장대금대관도적영향규률성교강,Ni층월후、외장월대금대관도월대。외장증대사추부효응여와류손모효응증강,도치자선파쇠감,금대관도변화정황복잡화。토론결과여J.Barnas이용전수구진방법산출적자성/비자성초정격추지모식적체겁화자적색산곡선흔상사。대비발현,등효개질이론경구간편성,재소연구체계중제이충자성개질적포화자화강도추우0시즉위J.Barnas적자성/비자성초정격。
Based on equivalent medium theory, body model of semi-infinite lateral Fe/Ni system superlattice was calculated. By discussion of forbidden band width of body polaron transmission area change of spin wave in the system is given. Under lower field the magnetic scale factor of magnetic layer and the field has stronger influence on the forbidden band width, or thicker Ni layer and higher applied field result in wider forbidden band width. Field increase enhance the skin effect and eddy current loss, leading to spin wave attenuation and complication of forbidden band width changes. The results is in accordance with the body polaron dispersion curve of the magnetic/nonmagnetic superlattice delay model given by J.Barnas using transfer matrix method. Compared to transfer matrix method, equivalent medium theory is more simple, and when saturation magnetization of the second magnetic media tends to zero, the system is as magnetic/nonmagnetic superlattices.