The X pinch as an x-ray source for point-projection radiography

Author(s):  
S. A. Pikuz ◽  
T. A. Shelkovenko ◽  
A. R. Mingaleev ◽  
V. M. Romanova ◽  
B. M. Song ◽  
...  
2018 ◽  
Vol 46 (11) ◽  
pp. 3815-3819
Author(s):  
Sergey A. Pikuz ◽  
Tatiana A. Shelkovenko ◽  
Ivan N. Tilikin ◽  
Egor V. Parkevich ◽  
Albert R. Mingaleev ◽  
...  

1997 ◽  
Vol 68 (1) ◽  
pp. 796-798 ◽  
Author(s):  
K. S. Budil ◽  
T. S. Perry ◽  
S. A. Alvarez ◽  
D. Hargrove ◽  
J. R. Mazuch ◽  
...  

2001 ◽  
Vol 72 (1) ◽  
pp. 667-670 ◽  
Author(s):  
T. A. Shelkovenko ◽  
D. B. Sinars ◽  
S. A. Pikuz ◽  
K. M. Chandler ◽  
D. A. Hammer

Radiology ◽  
1986 ◽  
Vol 161 (2) ◽  
pp. 533-535 ◽  
Author(s):  
H Nishitani ◽  
Y Umezu ◽  
K Ogawa ◽  
H Yuzuriha ◽  
H Tanaka ◽  
...  

2017 ◽  
Vol 53 (3) ◽  
pp. 227-230
Author(s):  
N. N. Potrakhov ◽  
A. A. Podymskii ◽  
V. B. Bessonov ◽  
A. V. Obodovskii ◽  
A. Y. Gryaznov ◽  
...  
Keyword(s):  
X Ray ◽  

Author(s):  
Daniel H. Morse ◽  
Arlyn J. Antolak ◽  
Bernice E. Mills

X-ray radiography has long been recognized as a valuable tool for detecting internal features and flaws. Recent developments in microfabrication and composite materials have extended inspection requirements to the resolution limits of conventional radiography. Our work has been directed toward pushing both detection and measurement capabilities to a smaller scale. Until recently, we have used conventional contact radiography, optimized to resolve small features. With the recent purchase of a nano-focus (sub-micron) x-ray source, we are now investigating projection radiography, phase contrast imaging and micro-computed tomography (μ-CT). Projection radiography produces a magnified image that is limited in spatial resolution mainly by the source size, not by film grain size or detector pixel size. Under certain conditions phase contrast can increase the ability to resolve small features such as cracks, especially in materials with low absorption contrast. Micro-computed tomography can provide three-dimensional measurements on a micron scale and has been shown to provide better sensitivity than simple radiographs. We have included applications of these techniques to small-scale measurements not easily made by mechanical or optical means. Examples include void detection in meso-scale nickel MEMS parts, measurement of edge profiles in thick gold lithography masks, and characterization of the distribution of phases in composite materials. Our work, so far, has been limited to film.


1999 ◽  
Vol 5 (S2) ◽  
pp. 352-353
Author(s):  
Sterling P. Newberry

Recent advances with the cone-beam approach to tomography at the Advanced Microscopy and Imaging Laboratory (AMIL) have opened the possibility of employing tomography with the Shadow Projection X-Ray Microscope routinely when the specimen properties require it. The AMIL approach has been tested on small objects, without magnification, using conventional dental x-ray sources and a modestly diverging beam angle. The shadow projection Microscope, by contrast has a tenfold greater divergence and magnifies the specimen from unity to three or more orders of magnitude in resolution beyond the previous tests. The reader is reminded of the simplicity of the xray projection method and of the clarity of its images in fig. 1 and 2. The microscope can be operated in any laboratory and readily transported to alternate locations. Now that the AMIL data base and algorithms for tomography can be handled by a Pentium II processor the data gathering and reconstructions can also be managed at any laboratory installation.


Author(s):  
S. Fletcher ◽  
R. S. Hannah ◽  
M. J. Hollenberg

The purpose of this study was to develop a functional microscope system to overcome the inherent disadvantages of using the light microscope/camera lucida system to reconstruct sections of biological material. The problem is perhaps most acute in the nervous system, where reconstruction of 3-dimensional neurons or the tracing of neuronal pathways over extensive distances must be attempted. The camera lucida system suffers from many inaccuracies and is an extremely time-consuming and tedious procedure. Point projection x-ray microscopy in the SEM, entails utilizing the primary electron beam in the spot mode to generate a point source of x-rays from a suitable target (Al, Cu, Au). This technique was first successfully demonstrated by Horn and Waltinger (1978).


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