Fast single scan derivation of the PSF resolution model on the TruePoint PET/CT using a printed point source array

Author(s):  
F A Kotasidis ◽  
J C Matthews ◽  
G I Angelis ◽  
P J Noonan ◽  
P J Markiewicz ◽  
...  
2013 ◽  
Vol 33 (12) ◽  
pp. 1222003 ◽  
Author(s):  
沈华 Shen Hua ◽  
李嘉 Li Jia ◽  
朱日宏 Zhu Rihong ◽  
荣四海 Rong Sihai

Geophysics ◽  
1995 ◽  
Vol 60 (4) ◽  
pp. 1058-1069 ◽  
Author(s):  
Tien‐Chang Lee ◽  
Brian N. Damiata

Owing to the proximity of an insulating ground surface, normal resistivity logging at shallow depths (less than 30 m) can yield an apparent resistivity that exceeds 200% of the formation resistivity for a homogeneous medium. The distortion is more acute for long‐normal than for short‐normal logging. Three examples from a landfill site in southern California are presented to show such distortion. The patterns of distortion are similar for logging devices consisting of either two point‐source electrodes or one point‐source and one finite length, line‐source electrode. The former electrode array is a generally accepted approximation of the latter. However, the simulated apparent resistivity for the line‐source array is greater than that for the point‐source array at any given depth. A resistivity contrast between the formation and the borehole fluid can shift the magnitude of the background apparent resistivity but does not significantly alter the pattern of distortion. The magnitude of the distortion can be reduced by placing the reference‐ground potential electrode at a radial distance that is about equal to the spacing between the downhole upper potential electrode and the upper current electrode. It can also be removed by including the radial distance in an array‐dependent geometric factor that accounts for the resistivity of the borehole fluid and the proximity of the logging device to the ground surface.


2008 ◽  
Vol 25 (2) ◽  
pp. 586-588 ◽  
Author(s):  
An Kang ◽  
Shen Yong ◽  
Ou Da-Yi
Keyword(s):  

2018 ◽  
Vol 417 ◽  
pp. 67-75 ◽  
Author(s):  
Jia Li ◽  
Hua Shen ◽  
Rihong Zhu ◽  
Jinming Gao ◽  
Yue Sun ◽  
...  

2017 ◽  
Vol 56 (11) ◽  
pp. 1 ◽  
Author(s):  
Donghui Zheng ◽  
Lei Chen ◽  
Yu Ding ◽  
Qinyuan Sun ◽  
Wenhua Zhu ◽  
...  

Author(s):  
Fotis A. Kotasidis ◽  
Georgios I. Angelis ◽  
Julian C. Matthews ◽  
William R. Lionheart ◽  
Andrew J. Reader

2018 ◽  
Vol 57 (21) ◽  
pp. 5929
Author(s):  
Yu Ding ◽  
Lei Chen ◽  
Lu Kong ◽  
Ying Yang ◽  
Zhiyuan Liu ◽  
...  

Author(s):  
D. A. Carpenter ◽  
Ning Gao ◽  
G. J. Havrilla

A monolithic, polycapillary, x-ray optic was adapted to a laboratory-based x-ray microprobe to evaluate the potential of the optic for x-ray micro fluorescence analysis. The polycapillary was capable of collecting x-rays over a 6 degree angle from a point source and focusing them to a spot approximately 40 µm diameter. The high intensities expected from this capillary should be useful for determining and mapping minor to trace elements in materials. Fig. 1 shows a sketch of the capillary with important dimensions.The microprobe had previously been used with straight and with tapered monocapillaries. Alignment of the monocapillaries with the focal spot was accomplished by electromagnetically scanning the focal spot over the beveled anode. With the polycapillary it was also necessary to manually adjust the distance between the focal spot and the polycapillary.The focal distance and focal spot diameter of the polycapillary were determined from a series of edge scans.


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