Total-electron-yield x-ray standing-wave measurements of multilayer x-ray mirrors for the interface structure evaluation

Author(s):  
Y. Muramatsu ◽  
L. Takenaka ◽  
E.M. Gullikson ◽  
R.C.C. Perera
2002 ◽  
Vol 41 (Part 1, No. 6B) ◽  
pp. 4250-4252 ◽  
Author(s):  
Yasuji Muramatsu ◽  
Hisataka Takenaka ◽  
Eric M. Gullikson ◽  
Rupert C. C. Perera

1985 ◽  
Vol 24 (Part 2, No. 6) ◽  
pp. L475-L477 ◽  
Author(s):  
Toshiaki Ohta ◽  
Hideo Sekiyama ◽  
Yoshinori Kitajima ◽  
Haruo Kuroda ◽  
Toshio Takahashi ◽  
...  

2005 ◽  
Vol 144-147 ◽  
pp. 897-899 ◽  
Author(s):  
Takeo Ejima ◽  
Atsushi Yamazaki ◽  
Takanori Banse ◽  
Tadashi Hatano

2018 ◽  
Vol 25 (5) ◽  
pp. 1433-1443
Author(s):  
C. Jansing ◽  
H. Wahab ◽  
H. Timmers ◽  
A. Gaupp ◽  
H.-C. Mertins

The complex refractive index of many materials is poorly known in the soft X-ray range across absorption edges. This is due to saturation effects that occur there in total-electron-yield and fluorescence-yield spectroscopy and that are strongest at resonance energies. Aiming to obtain reliable optical constants, a procedure that reconciles electron-yield measurements and reflection spectroscopy by correcting these saturation effects is presented. The procedure takes into account the energy- and polarization-dependence of the photon penetration depth as well as the creation efficiency for secondary electrons and their escape length. From corrected electron-yield spectra the absorption constants and the imaginary parts of the refractive index of the material are determined. The real parts of the index are subsequently obtained through a Kramers–Kronig transformation. These preliminary optical constants are refined by simulating reflection spectra and adapting them, so that measured reflection spectra are reproduced best. The efficacy of the new procedure is demonstrated for graphite. The optical constants that have been determined for linearly polarized synchrotron light incident with p- and s-geometry provide a detailed and reliable representation of the complex refractive index of the material near π- and σ-resonances. They are also suitable for allotropes of graphite such as graphene.


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