Quantum efficiency measurement of the x-ray CCD camera (XIS) for the ASTRO-E mission in the soft-x-ray band

1999 ◽  
Author(s):  
Takayoshi Kohmura ◽  
Kazunori Katayama ◽  
Haruyoshi Katayama ◽  
Makoto Shouho ◽  
Hiroshi Tsunemi ◽  
...  
Author(s):  
Neil J. Murray ◽  
Andrew D. Holland ◽  
David R. Smith ◽  
Jason P. Gow ◽  
Peter J. Pool ◽  
...  

1999 ◽  
Vol 320 (4-5) ◽  
pp. 373-373
Author(s):  
T. Kohmura ◽  
K. Katayama ◽  
H. Katayama ◽  
M. Shouho ◽  
H. Tsunemi ◽  
...  
Keyword(s):  

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.


Author(s):  
A. V. Ermachikhin ◽  
◽  
Yu. V. Vorobyov ◽  
V. O. Sazonov ◽  
◽  
...  

1994 ◽  
Author(s):  
Vincent D. Rose ◽  
Kathryn A. Flanagan ◽  
Joshua Lessing ◽  
D. Kearns ◽  
Stephen S. Murray ◽  
...  

2021 ◽  
Author(s):  
Jesse Tanguay ◽  
Devon Richtsmeier ◽  
Christopher Dydula ◽  
James A. Day ◽  
Kris Iniewski ◽  
...  

1998 ◽  
Vol 5 (3) ◽  
pp. 642-644 ◽  
Author(s):  
J. Y. Huang ◽  
I. S. Ko

A diagnostic beamline is being constructed in the PLS storage ring for measurement of electron- and photon-beam properties. It consists of two 1:1 imaging systems: a visible-light imaging system and a soft X-ray imaging system. In the visible-light imaging system, the transverse beam size and beam position are measured with various detectors: a CCD camera, two photodiode arrays and a photon-beam position monitor. Longitudinal bunch structure is also investigated with a fast photodiode detector and a picosecond streak camera. On the other hand, the soft X-ray imaging system is under construction to measure beam sizes with negligible diffraction-limited error. The X-ray image optics consist of a flat cooled mirror and two spherical focusing mirrors.


Sign in / Sign up

Export Citation Format

Share Document