POLARIZATION OF ELASTICALLY SCATTERED 1.33-MeV PHOTONS

1965 ◽  
Vol 43 (6) ◽  
pp. 1078-1087 ◽  
Author(s):  
R. A. Williams ◽  
K. G. McNeill

Measurements have been made as a function of angle of the polarization of 1.33-MeV gamma rays elastically scattered by lead. The analysis of the experimental data included the contribution of the L-shell electrons to inelastic Compton scattering. The results show no apparent deviation from the polarizations expected on the basis of Rayleigh and Thomson scattering.

2018 ◽  
Vol 13 (0) ◽  
pp. 2404066-2404066
Author(s):  
Shuji MIYAMOTO ◽  
Akinori TAKEMOTO ◽  
Masashi YAMAGUCHI ◽  
Kento SUGITA ◽  
Satoshi HASHIMOTO ◽  
...  

2014 ◽  
Vol 61 (3) ◽  
pp. 1252-1258 ◽  
Author(s):  
Hiroaki Utsunomiya ◽  
Tatsushi Shima ◽  
Keiji Takahisa ◽  
Dan Mihai Filipescu ◽  
Ovidiu Tesileanu ◽  
...  

2020 ◽  
Vol 27 (3) ◽  
pp. 737-745
Author(s):  
Zhijun Chi ◽  
Yingchao Du ◽  
Wenhui Huang ◽  
Chuanxiang Tang

A Thomson scattering X-ray source can provide quasi-monochromatic, continuously energy-tunable, polarization-controllable and high-brightness X-rays, which makes it an excellent tool for X-ray fluorescence computed tomography (XFCT). In this paper, we examined the suppression of Compton scattering background in XFCT using the linearly polarized X-rays and the implementation feasibility of linearly polarized XFCT based on this type of light source, concerning the influence of phantom attenuation and the sampling strategy, its advantage over K-edge subtraction computed tomography (CT), the imaging time, and the potential pulse pile-up effect by Monte Carlo simulations. A fan beam and pinhole collimator geometry were adopted in the simulation and the phantom was a polymethyl methacrylate cylinder inside which were gadolinium (Gd)-loaded water solutions with Gd concentrations ranging from 0.2 to 4.0 wt%. Compared with the case of vertical polarization, Compton scattering was suppressed by about 1.6 times using horizontal polarization. An accurate image of the Gd-containing phantom was successfully reconstructed with both spatial and quantitative identification, and good linearity between the reconstructed value and the Gd concentration was verified. When the attenuation effect cannot be neglected, one full cycle (360°) sampling and the attenuation correction became necessary. Compared with the results of K-edge subtraction CT, the contrast-to-noise ratio values of XFCT were improved by 2.03 and 1.04 times at low Gd concentrations of 0.2 and 0.5 wt%, respectively. When the flux of a Thomson scattering light source reaches 1013 photons s−1, it is possible to finish the data acquisition of XFCT at the minute or second level without introducing pulse pile-up effects.


2006 ◽  
Vol 643 (2) ◽  
pp. 1081-1097 ◽  
Author(s):  
Charles D. Dermer ◽  
Markus Bottcher

2019 ◽  
Vol 4 (1) ◽  
pp. 24 ◽  
Author(s):  
Mihael Makek ◽  
Damir Bosnar ◽  
Luka Pavelić

The Compton scattering of gamma rays is commonly detected using two detector layers, the first for detection of the recoil electron and the second for the scattered gamma. We have assembled detector modules consisting of scintillation pixels, which are able to detect and reconstruct the Compton scattering of gammas with only one readout layer. This substantially reduces the number of electronic channels and opens the possibility to construct cost-efficient Compton scattering detectors for various applications such as medical imaging, environment monitoring, or fundamental research. A module consists of a 4 × 4 matrix of lutetium fine silicate scintillators and is read out by a matching silicon photomultiplier array. Two modules have been tested with a 22 Na source in coincidence mode, and the performance in the detection of 511 keV gamma Compton scattering has been evaluated. The results show that Compton events can be clearly distinguished with a mean energy resolution of 12.2% ± 0.7% in a module and a coincidence time resolution of 0 . 56 ± 0 . 02 ns between the two modules.


2008 ◽  
Author(s):  
Takehito Hayakawa ◽  
Ryoichi Hajima ◽  
Sergei V. Bulanov ◽  
H. Daido

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