Development of a 3-D X-Ray Micro-tomography System and its Application to Trabecular Bone/Cement Interface

2004 ◽  
Vol 41 (sup4) ◽  
pp. 369-4
Author(s):  
Yong Ki Chi ◽  
Gyuseong Cho
2003 ◽  
Vol 58 (2) ◽  
pp. 177-181 ◽  
Author(s):  
P.M. Jenneson ◽  
W.B. Gilboy ◽  
E.J. Morton ◽  
P.J. Gregory

1994 ◽  
Vol 5 (9-10) ◽  
pp. 644-646
Author(s):  
L. Savarino ◽  
S. Stea ◽  
D. Granchi ◽  
M. E. Donati ◽  
G. Paganetto ◽  
...  

2004 ◽  
Vol 49 (17) ◽  
pp. 3889-3902 ◽  
Author(s):  
In Kon Chun ◽  
Myung Hye Cho ◽  
Sang Chul Lee ◽  
Min Hyoung Cho ◽  
Soo Yeol Lee

Author(s):  
W. Brünger

Reconstructive tomography is a new technique in diagnostic radiology for imaging cross-sectional planes of the human body /1/. A collimated beam of X-rays is scanned through a thin slice of the body and the transmitted intensity is recorded by a detector giving a linear shadow graph or projection (see fig. 1). Many of these projections at different angles are used to reconstruct the body-layer, usually with the aid of a computer. The picture element size of present tomographic scanners is approximately 1.1 mm2.Micro tomography can be realized using the very fine X-ray source generated by the focused electron beam of a scanning electron microscope (see fig. 2). The translation of the X-ray source is done by a line scan of the electron beam on a polished target surface /2/. Projections at different angles are produced by rotating the object.During the registration of a single scan the electron beam is deflected in one direction only, while both deflections are operating in the display tube.


1997 ◽  
Vol 503 ◽  
Author(s):  
B. L. Evans ◽  
J. B. Martin ◽  
L. W. Burggraf

ABSTRACTThe viability of a Compton scattering tomography system for nondestructively inspecting thin, low Z samples for corrosion is examined. This technique differs from conventional x-ray backscatter NDI because it does not rely on narrow collimation of source and detectors to examine small volumes in the sample. Instead, photons of a single energy are backscattered from the sample and their scattered energy spectra are measured at multiple detector locations, and these spectra are then used to reconstruct an image of the object. This multiplexed Compton scatter tomography technique interrogates multiple volume elements simultaneously. Thin samples less than 1 cm thick and made of low Z materials are best imaged with gamma rays at or below 100 keV energy. At this energy, Compton line broadening becomes an important resolution limitation. An analytical model has been developed to simulate the signals collected in a demonstration system consisting of an array of planar high-purity germanium detectors. A technique for deconvolving the effects of Compton broadening and detector energy resolution from signals with additive noise is also presented. A filtered backprojection image reconstruction algorithm with similarities to that used in conventional transmission computed tomography is developed. A simulation of a 360–degree inspection gives distortion-free results. In a simulation of a single-sided inspection, a 5 mm × 5 mm corrosion flaw with 50% density is readily identified in 1-cm thick aluminum phantom when the signal to noise ratio in the data exceeds 28.


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