X-ray crystal spectrometer with a charge-coupled-device detector for ion temperature measurements in the Large Helical Device

2003 ◽  
Vol 74 (4) ◽  
pp. 2375-2387 ◽  
Author(s):  
Shigeru Morita ◽  
Motoshi Goto
1997 ◽  
Vol 68 (6) ◽  
pp. 2387-2392 ◽  
Author(s):  
Michel Koenig ◽  
Jean Michel Boudenne ◽  
P. Legriel ◽  
A. Benuzzi ◽  
T. Grandpierre ◽  
...  

1998 ◽  
Vol 69 (12) ◽  
pp. 4054-4060 ◽  
Author(s):  
L. M. Logory ◽  
D. R. Farley ◽  
A. D. Conder ◽  
E. A. Belli ◽  
P. M. Bell ◽  
...  

2003 ◽  
Vol 74 (4) ◽  
pp. 2388-2408 ◽  
Author(s):  
R. Barnsley ◽  
N. J. Peacock ◽  
J. Dunn ◽  
I. M. Melnick ◽  
I. H. Coffey ◽  
...  

2000 ◽  
Vol 71 (12) ◽  
pp. 4449 ◽  
Author(s):  
K. Sato ◽  
Y. Hasegawa ◽  
K. Kondo ◽  
K. Miyazaki ◽  
T. Matsushita ◽  
...  

2006 ◽  
Vol 39 (5) ◽  
pp. 767-770
Author(s):  
Hiroshi Abe ◽  
Hiroyuki Saitoh ◽  
Hironori Nakao ◽  
Kazuki Ito ◽  
Ken-ichi Ohshima

A charge-coupled device (CCD) X-ray detector for inelastic X-ray scattering was installed at beamline BL-4C of the Photon Factory at the High Energy Accelerator Research Organization in Japan. A wavelength-dispersive X-ray spectrometer was mounted on a six-circle diffractometer. Energy spectra were obtained by the CCD X-ray detector and a curved highly oriented pyrolytic graphite analyser. By the combination of energy spectroscopy and diffraction, simultaneous real-time data acquisition of both the momentum and the energy transfer was performed.


1994 ◽  
Vol 38 ◽  
pp. 503-510 ◽  
Author(s):  
S. Hanna ◽  
A.H. Windle

Abstract We describe a new X-ray fibre diffractometer, consisting of a commercial X-ray sensitive video camera coupled to a conventional 3-circle goniometer in place of a more traditional single-point detector. The active element of the video camera is a charge-coupled device (CCD). Diffraction images, obtained at various goniometer settings, are transformed into reciprocal space, and combined to give a complete section through the origin and parallel to the symmetry axis of cyiindrically averaged reciprocal space. A greater density of measurements is needed in the vicinity of the reciprocal fibre axis in order to avoid information loss due to the curvature of the Ewald sphere. The pros and cons of using CCD's as X-ray detectors are discussed and sample results from polymer fibres are shown.


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