物理学报
物理學報
물이학보
2001年
5期
860-864
,共5页
王培录%刘仲阳%郑思孝%廖小东%杨朝文%唐阿友%师勉恭%杨百方%缪竞威
王培錄%劉仲暘%鄭思孝%廖小東%楊朝文%唐阿友%師勉恭%楊百方%繆競威
왕배록%류중양%정사효%료소동%양조문%당아우%사면공%양백방%무경위
氮团簇注入%表面特性
氮糰簇註入%錶麵特性
담단족주입%표면특성
用椭偏仪、傅氏变换红外吸收谱(FT-IR)、X射线光电子能谱(XPS)以及原子力显微镜(AFM)对N+1,N+2,N+10离子高剂量(1.7×1017 ions/cm2)注入Si(111)的表面进行测试分析,发现三种不同尺度的离子注入后,均使Si由复折射率变化为实折射率,表面出现含氮-硅键的介质层.但其表面形貌各异:N+1注入的表面除存在少量点蚀坑外,光洁度最高(平均粗糙度Ra≈4.2nm),接近未注入前的原始表面(Ra≈3.5nm);N+2注入的出现黑色枝状区域,光洁度次之(Ra≈16nm),而N+10注入的则出现“波纹”状结构,光洁度最差(Ra≈40nm).与低能团簇注入相反,在高能条件下,随着离子尺度和注量增加,材料表面的粗糙度也越严重.
用橢偏儀、傅氏變換紅外吸收譜(FT-IR)、X射線光電子能譜(XPS)以及原子力顯微鏡(AFM)對N+1,N+2,N+10離子高劑量(1.7×1017 ions/cm2)註入Si(111)的錶麵進行測試分析,髮現三種不同呎度的離子註入後,均使Si由複摺射率變化為實摺射率,錶麵齣現含氮-硅鍵的介質層.但其錶麵形貌各異:N+1註入的錶麵除存在少量點蝕坑外,光潔度最高(平均粗糙度Ra≈4.2nm),接近未註入前的原始錶麵(Ra≈3.5nm);N+2註入的齣現黑色枝狀區域,光潔度次之(Ra≈16nm),而N+10註入的則齣現“波紋”狀結構,光潔度最差(Ra≈40nm).與低能糰簇註入相反,在高能條件下,隨著離子呎度和註量增加,材料錶麵的粗糙度也越嚴重.
용타편의、부씨변환홍외흡수보(FT-IR)、X사선광전자능보(XPS)이급원자력현미경(AFM)대N+1,N+2,N+10리자고제량(1.7×1017 ions/cm2)주입Si(111)적표면진행측시분석,발현삼충불동척도적리자주입후,균사Si유복절사솔변화위실절사솔,표면출현함담-규건적개질층.단기표면형모각이:N+1주입적표면제존재소량점식갱외,광길도최고(평균조조도Ra≈4.2nm),접근미주입전적원시표면(Ra≈3.5nm);N+2주입적출현흑색지상구역,광길도차지(Ra≈16nm),이N+10주입적칙출현“파문”상결구,광길도최차(Ra≈40nm).여저능단족주입상반,재고능조건하,수착리자척도화주량증가,재료표면적조조도야월엄중.
The measurement and analysis were carried out on the Si(111) surface implanted by N+1,N+2,N+10 cluster ions with high doses (1.7×1017ions/cm2) at 76keV energy using ellipsometry,Fourier-transform infrared (FT-IR) absorption spectroscopy, X-ray photoelectron spectroscopy and atomic force microscopy.It was found that the medium layer containing Si_N bond on the surface appeared,and their complex refractive index turned into real;however,at the same implantation dose their surface morphologies were different from each other.Expect for a few pittings,the N+1-implanted surface had a best fineness (average roughness Ra≈4.2nm), close to the unimplanted original surface.The N+2-implanted surface had a black dendritic area,and had a poorer fineness (Ra≈16nm).While in the N+10-implanted surface appeared a ripple structure,with the poorest fineness (Ra≈40nm).It was indicated that the roughness of the material surface increased with the ion size and fluence at the high energy in contrast to the cluster implantation at the low energy.