A ring coded‐aperture microscope for high‐resolution imaging of high‐energy x rays

1992 ◽  
Vol 63 (10) ◽  
pp. 5086-5088 ◽  
Author(s):  
D. Ress ◽  
D. R. Ciarlo ◽  
J. E. Stewart ◽  
P. M. Bell ◽  
D. R. Kania
Author(s):  
G.J.F. Legge ◽  
J.S. Laird ◽  
L.M. Mason ◽  
A. Saint ◽  
M. Cholewa ◽  
...  

2002 ◽  
Vol 73 (3) ◽  
pp. 1640-1642 ◽  
Author(s):  
C. G. Schroer ◽  
B. Benner ◽  
T. F. Günzler ◽  
M. Kuhlmann ◽  
C. Zimprich ◽  
...  

Science ◽  
1982 ◽  
Vol 215 (4529) ◽  
pp. 150-152 ◽  
Author(s):  
A. Robinson

Author(s):  
Charles W. Allen ◽  
Kenneth H. Westmacotp

With the development of the Atomic Resolution Microscope (JEOL ARM-1000) about a decade ago and the current availability of new ultra high resolution HVEMs, the important role of HVEM in high resolution imaging has been well achieved. Higher spatial resolution imaging is attainable with higher energy electrons without sacrificing sample tilting capability by virtue of a smaller CSλ value. When commercial HVEMs first became available in the mid 1960's, however, it was not the prospect of high resolution imaging which seemed most important but rather the fact that, for a given material, significantly thicker specimens could be examined.The microstructures (ultrastructures) and physical behavior of these foils (up to 15 μm thick) would be more representative of those for the bulk material. And especially for materials science applications two other factors were also of paramount importance: (1) the controlled generation of vacancy-interstitial (Frenkel) pairs in crystalline pure elements and alloys by high energy electron irradiation became possible and (2) the increased working space in the objective lens region allowed some miniaturized experimental apparatus to be incorporated.


2008 ◽  
Author(s):  
Brian Rodricks ◽  
Boyd Fowler ◽  
Chiao Liu ◽  
John Lowes ◽  
Dean Haeffner ◽  
...  

2003 ◽  
Vol 35 (3-4) ◽  
pp. 253-271 ◽  
Author(s):  
H. J. Bunge ◽  
H. Klein ◽  
L. Wcislak ◽  
U. Garbe ◽  
W. Weiß ◽  
...  

In order to describe texture and microstructure of a polycrystalline material completely, crystal orientation g={ϕ1Φϕ2} must be known in all points x={x1 x2 x3} of the material. This can be achieved by locationresolved diffraction of high-energy, i.e. short-wave, X-rays from synchrotron sources. Highest resolution in the orientation- as well as the location-coordinates can be achieved by three variants of a detector “sweeping” technique in which an area detector is continuously moved during exposure. This technique results in two-dimensionally continuous images which are sections and projections of the six-dimensional “orientation– location” space. Further evaluation of these images depends on whether individual grains are resolved in them or not. Because of the high penetration depth of high-energy synchrotron radiation in matter, this technique is also, and particularly, suitable for the investigation of the interior of big samples.


2021 ◽  
Author(s):  
Nicolas Bertaux ◽  
Marc Allain ◽  
John Weizeorick ◽  
Jun-Sang Park ◽  
Peter Kenesei ◽  
...  

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