Development of Hard X-ray Imaging Optics with Two Pairs of Elliptical and Hyperbolic Mirrors

2010 ◽  
Author(s):  
S. Matsuyama ◽  
M. Fujii ◽  
T. Wakioka ◽  
H. Mimura ◽  
S. Handa ◽  
...  
Keyword(s):  
X Ray ◽  
2007 ◽  
Author(s):  
Tomasz Jannson ◽  
Michael Gertsenshteyn ◽  
Victor Grubsky ◽  
Pauline Amouzou ◽  
Richard Koziol

1992 ◽  
Author(s):  
Takeshi Namioka ◽  
Koujun Yamashita ◽  
Masaki Yamamoto ◽  
Tadashi Matsushita ◽  
Sadao Aoki ◽  
...  
Keyword(s):  
X Ray ◽  
Title X ◽  

2012 ◽  
Vol 20 (9) ◽  
pp. 10310 ◽  
Author(s):  
Satoshi Matsuyama ◽  
Naotaka Kidani ◽  
Hidekazu Mimura ◽  
Yasuhisa Sano ◽  
Yoshiki Kohmura ◽  
...  

1981 ◽  
Vol 20 (6) ◽  
pp. 1080 ◽  
Author(s):  
P. A. J. de Korte ◽  
R. Giralt ◽  
J. N. Coste ◽  
C. Ernu ◽  
S. Frindel ◽  
...  
Keyword(s):  
X Ray ◽  

2001 ◽  
Vol 40 (Part 1, No. 3A) ◽  
pp. 1499-1503 ◽  
Author(s):  
Akihisa Takeuchi ◽  
Kentaro Uesugi ◽  
Yoshio Suzuki ◽  
Sadao Aoki
Keyword(s):  
X Ray ◽  

Author(s):  
M.G. Baldini ◽  
S. Morinaga ◽  
D. Minasian ◽  
R. Feder ◽  
D. Sayre ◽  
...  

Contact X-ray imaging is presently developing as an important imaging technique in cell biology. Our recent studies on human platelets have demonstrated that the cytoskeleton of these cells contains photondense structures which can preferentially be imaged by soft X-ray imaging. Our present research has dealt with platelet activation, i.e., the complex phenomena which precede platelet appregation and are associated with profound changes in platelet cytoskeleton. Human platelets suspended in plasma were used. Whole cell mounts were fixed and dehydrated, then exposed to a stationary source of soft X-rays as previously described. Developed replicas and respective grids were studied by scanning electron microscopy (SEM).


Author(s):  
James F. Mancuso ◽  
William B. Maxwell ◽  
Russell E. Camp ◽  
Mark H. Ellisman

The imaging requirements for 1000 line CCD camera systems include resolution, sensitivity, and field of view. In electronic camera systems these characteristics are determined primarily by the performance of the electro-optic interface. This component converts the electron image into a light image which is ultimately received by a camera sensor.Light production in the interface occurs when high energy electrons strike a phosphor or scintillator. Resolution is limited by electron scattering and absorption. For a constant resolution, more energy deposition occurs in denser phosphors (Figure 1). In this respect, high density x-ray phosphors such as Gd2O2S are better than ZnS based cathode ray tube phosphors. Scintillating fiber optics can be used instead of a discrete phosphor layer. The resolution of scintillating fiber optics that are used in x-ray imaging exceed 20 1p/mm and can be made very large. An example of a digital TEM image using a scintillating fiber optic plate is shown in Figure 2.


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