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首页> 外文期刊>Surface & Coatings Technology >Morphology of Si surfaces sputter-eroded by low-energy Xe-ions at glancing incident angle
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Morphology of Si surfaces sputter-eroded by low-energy Xe-ions at glancing incident angle

机译:低能Xe离子在掠射角处溅射腐蚀的Si表面的形貌

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Sputter erosion of Si generates nanoscale ripple patterns which are stable at ambient conditions and which may serve as an experimental test of ripple formation theories. Up to now, almost all studies on ripple formation of Si-surface have been carried Out with large ion-fluence (varying from 10(17) ions/cm(2) to 10(22) ions/cm(2)) and shown the ripple-pattern orientated in the direction perpendicular to the ion-beam. The present reports on the evolution of Si surfaces after low-energy (5 keV) Xe+ ion irradiation at room temperature with low ion-fluences of 1 X 10(14) -3 x 10(17) ions /cm(2) at glancing incident angles theta up to 85 degrees. The purpose is to focus on the critical angle 0, of the ripple rotation from perpendicular to parallel orientation to the ion beam. It is found that the nanometer ripple formations occurred for theta > 70 degrees with an orientation perpendicular (for 80 degrees > theta >= 70 degrees) or parallel (for theta>80 degrees) to the ion-beam direction. At the critical angle theta(c) = 80 degrees ion-bombardment produced two-dimensional nanopatterns with tile-like laminas. The size of the laminas increase by raising the ion-fluences. The surface roughness obeys an exponential function (omega similar to exp (R-k . Phi) for ion-fluences Phi < 1.5 x 10(16) ions/cm(2), while for larger ion-fluences the roughness nearly reaches saturation and only increases slowly according to a power law function omega similar to Phi(beta) with beta approximate to 0.34.
机译:Si的溅射腐蚀会产生在环境条件下稳定的纳米级波纹图案,可作为波纹形成理论的实验测试。到目前为止,几乎所有关于硅表面波纹形成的研究都是通过较大的离子通量(从10(17)离子/ cm(2)到10(22)离子/ cm(2)变化)进行的,并且显示了波纹图案的方向垂直于离子束。本报告报道了在室温下低能量(5 keV)Xe +离子辐照后,低离子通量为1 X 10(14)-3 x 10(17)离子/ cm(2)时Si表面的演变入射角θ可达85度。目的是关注从垂直到平行于离子束取向的波纹旋转的临界角0。已经发现,对于θ> 70度发生了纳米波纹形成,其取向与离子束方向垂直(对于80度>θ> = 70度)或平行于(对于θ> 80度)取向。在临界角theta(c)= 80度时,离子轰击产生了带有瓦状薄片的二维纳米图案。层的大小通过提高离子通量而增加。对于离子通量Phi <1.5 x 10(16)ions / cm(2),表面粗糙度服从指数函数(类似于exp(Rk。Phi)的Ω),而对于较大的离子通量,粗糙度几乎达到饱和并且仅增加缓慢地根据幂律函数ω类似于Phiβ,β大约为0.34。

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