scholarly journals 50-nm-resolution full-field X-ray microscope without chromatic aberration using total-reflection imaging mirrors

2017 ◽  
Vol 7 (1) ◽  
Author(s):  
Satoshi Matsuyama ◽  
Shuhei Yasuda ◽  
Jumpei Yamada ◽  
Hiromi Okada ◽  
Yoshiki Kohmura ◽  
...  
2013 ◽  
Vol 463 ◽  
pp. 012017 ◽  
Author(s):  
S Matsuyama ◽  
Y Emi ◽  
Y Kohmura ◽  
K Tamasaku ◽  
M Yabashi ◽  
...  
Keyword(s):  

2017 ◽  
Vol 24 (2) ◽  
pp. 392-401 ◽  
Author(s):  
Hugh Simons ◽  
Sonja Rosenlund Ahl ◽  
Henning Friis Poulsen ◽  
Carsten Detlefs

A comprehensive optical description of compound refractive lenses (CRLs) in condensing and full-field X-ray microscopy applications is presented. The formalism extends ray-transfer matrix analysis by accounting for X-ray attenuation by the lens material. Closed analytical expressions for critical imaging parameters such as numerical aperture, spatial acceptance (vignetting), chromatic aberration and focal length are provided for both thin- and thick-lens imaging geometries. These expressions show that the numerical aperture will be maximized and chromatic aberration will be minimized at the thick-lens limit. This limit may be satisfied by a range of CRL geometries, suggesting alternative approaches to improving the resolution and efficiency of CRLs and X-ray microscopes.


2015 ◽  
Vol 23 (8) ◽  
pp. 9746 ◽  
Author(s):  
Satoshi Matsuyama ◽  
Yoji Emi ◽  
Hidetoshi Kino ◽  
Yoshiki Kohmura ◽  
Makina Yabashi ◽  
...  

2019 ◽  
Vol 27 (13) ◽  
pp. 18318 ◽  
Author(s):  
Satoshi Matsuyama ◽  
Jumpei Yamada ◽  
Yoshiki Kohmura ◽  
Makina Yabashi ◽  
Tetsuya Ishikawa ◽  
...  

Author(s):  
Werner P. Rehbach ◽  
Peter Karduck

In the EPMA of soft x rays anomalies in the background are found for several elements. In the literature extremely high backgrounds in the region of the OKα line are reported for C, Al, Si, Mo, and Zr. We found the same effect also for Boron (Fig. 1). For small glancing angles θ, the background measured using a LdSte crystal is significantly higher for B compared with BN and C, although the latter are of higher atomic number. It would be expected, that , characteristic radiation missing, the background IB (bremsstrahlung) is proportional Zn by variation of the atomic number of the target material. According to Kramers n has the value of unity, whereas Rao-Sahib and Wittry proposed values between 1.12 and 1.38 , depending on Z, E and Eo. In all cases IB should increase with increasing atomic number Z. The measured values are in discrepancy with the expected ones.


2003 ◽  
Vol 107 ◽  
pp. 203-206 ◽  
Author(s):  
M. Bounakhla ◽  
A. Doukkali ◽  
K. Lalaoui ◽  
H. Aguenaou ◽  
N. Mokhtar ◽  
...  
Keyword(s):  

2016 ◽  
Vol 88 (7) ◽  
pp. 3826-3835 ◽  
Author(s):  
Bernhard Hesse ◽  
Murielle Salome ◽  
Hiram Castillo-Michel ◽  
Marine Cotte ◽  
Barbara Fayard ◽  
...  

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