Tani K, Nanjyo T, Masui S, Saisho H
Ricoh R & D Center, Tsuzuki-ku, Yokohama 224, Japan.
J Synchrotron Radiat. 1998 May 1;5(Pt 3):1144-5. doi: 10.1107/S0909049597017597.
The reflectivity of TiSi(2) films was measured as a function of photon energy E at the Ti K-edge region at a glancing angle theta close to the critical angle theta(C) of total reflection. TiSi(2) silicide films (about 30 nm thickness) were prepared by silicidation of Ti thin films deposited on Si(001) substrates. Since the Fresnel reflectivity R(theta,E) is a function of the dispersion delta(E) and of the absorption beta(E), the absorption beta(E) which carries the XAFS signal can be solved as beta(theta,delta,R) for observed reflectivity R and for estimated delta. The dispersion delta(E) is related to the absorption beta(E) by the Kramers-Kronig (K-K) relations since the refractive index is n(E) = 1 - delta(E) - ibeta(E). beta(E) was calculated from the observed reflectivity R(theta,E) using theoretical values for initial delta(E). Titanium K-edge XAFS for TiSi(2) was extracted from the reflectivity by 'ReflXAFS'.
在接近全反射临界角θ(C)的掠射角θ下,测量了TiSi(2)薄膜在Ti K边区域的反射率随光子能量E的变化。通过对沉积在Si(001)衬底上的Ti薄膜进行硅化处理,制备了厚度约为30 nm的TiSi(2)硅化物薄膜。由于菲涅耳反射率R(θ,E)是色散δ(E)和吸收β(E)的函数,对于观测到的反射率R和估计的δ,携带XAFS信号的吸收β(E)可以求解为β(θ,δ,R)。由于折射率为n(E)=1-δ(E)-iβ(E),色散δ(E)通过克莱默斯-克勒尼希(K-K)关系与吸收β(E)相关。利用初始δ(E)的理论值,从观测到的反射率R(θ,E)计算出β(E)。通过“ReflXAFS”从反射率中提取了TiSi(2)的钛K边XAFS。