An analytical X-ray CdTe detector response matrix for incomplete charge collection correction for photon energies up to 300 keV

2018 ◽  
Vol 146 ◽  
pp. 26-33 ◽  
Author(s):  
Dana Kurková ◽  
Libor Judas
Author(s):  
RunLong Gao ◽  
Yang Liu ◽  
XiaoPing Ouyang ◽  
Jing Chen ◽  
Xiao Ouyang

2016 ◽  
Vol 587 ◽  
pp. A151 ◽  
Author(s):  
J. S. Kaastra ◽  
J. A. M. Bleeker
Keyword(s):  
X Ray ◽  

2010 ◽  
Vol 57 (4) ◽  
pp. 2400-2404 ◽  
Author(s):  
Jeffrey W. Keister ◽  
John Smedley ◽  
Dimitre Dimitrov ◽  
Richard Busby
Keyword(s):  

2020 ◽  
Vol 38 ◽  
pp. 93-99
Author(s):  
Hiroshi Sakurai ◽  
Kazushi Hoshi ◽  
Yosuke Harasawa ◽  
Daiki Ono ◽  
Kun Zhang ◽  
...  

We developed the photon counting CT system by using a conventional laboratory X-ray source and a CdTe line sensor. Attenuation coefficients were obtained from the measured CT image data. Our suggested method for deriving the electron density and effective atomic number from the measured attenuation coefficients was tested experimentally. The accuracy of the electron densities and effective atomic numbers are about <5 % (the averages of absolute values are 2.6 % and 3.1 %, respectively) for material of 6< Z and Zeff <13. Our suggested simple method, in which we do not need the exact source X-ray spectrum and detector response function, achieves comparable accuracy to the previous reports.


2019 ◽  
Vol 199 (3-4) ◽  
pp. 1046-1054 ◽  
Author(s):  
G. C. O’Neil ◽  
P. Szypryt ◽  
E. Takacs ◽  
J. N. Tan ◽  
S. W. Buechele ◽  
...  

1997 ◽  
Vol 163 ◽  
pp. 709-710 ◽  
Author(s):  
J. Greiner ◽  
B.A. Harmon ◽  
W.S. Paciesas ◽  
E.H. Morgan ◽  
R.A. Remillard

After the discovery of GRS 1915+105 (Castro-Tirado et al. 1992) we obtained pointed ROSAT observations every six months (12 until now). The flux in the ROSAT (0.1–2.4 keV) band is strikingly different from the simultaneous BATSE (25–50 keV) flux which was obtained by integrating the best fit power law (Fig. 1). Motivated by the different intensity evolution in the soft and hard X-ray band we have selected BATSE monitoring data collected simultaneously to ROSATdata and performed joint spectral fitting with XSPEC. As a result, we never got an acceptable fit (see Fig. 2): The BATSE power law (upper dotted line) is too steep to match the ROSAT band, and even allowing for an increased absorbing column (lower dotted line) does not solve the problem. Alternatively, neither a thermal bremsstrahlung fit (solid line) nor a power law fit (lower dash-dot line) to the ROSAT data match the BATSE flux. The upper dash-dot line is a -2.5 powerlaw which would match the BATSE data while giving too much 1–2 keV emission. A similar, but less stringent result is obtained when folding the best fit BATSE power law models with the HRI detector response to compare the expected count rate with the observed one. We therefore conclude that the spectrum during all simultaneous ROSAT/BATSE observations seemingly consists of two different spectral components.


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