2005
DOI: 10.1007/s10967-005-0692-y
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Calculation of peak-to-total ratios for high purity germanium detectors using Monte-Carlo modeling

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Cited by 19 publications
(9 citation statements)
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“…Semiconductor radiation detectors for high-energy-photon detection require materials with a large detecting volume to intercept radiation, a large linear attenuation coefficient, large and balanced electron and hole mobility (µ)-charge carrier lifetime (τ ) product (µτ product) for efficient charge collection, and finally, high resistivity and low charge trap density to avoid charge trapping under singleevent analysis 4 . Among the semiconductors with relatively strong attenuation, high-purity germanium (HPGe) that was developed in the 1970s gives a γ-ray detector the best resolution, which however needs liquid nitrogen cooling due to its small bandgap 5 . Zinc-alloyed CdTe (Cd 1−x Zn x Te, denoted CZT for 0 < x < 0.2) single crystals with a large bandgap of above 1.6 eV possess a high resistivity up to 10 8 ∼ 10 9 cm at room temperature as well as a large µτ product, and thus produce the best resolution γ-ray spectrum among non-cooled semiconductor radiation detectors [6][7][8] .…”
mentioning
confidence: 99%
“…Semiconductor radiation detectors for high-energy-photon detection require materials with a large detecting volume to intercept radiation, a large linear attenuation coefficient, large and balanced electron and hole mobility (µ)-charge carrier lifetime (τ ) product (µτ product) for efficient charge collection, and finally, high resistivity and low charge trap density to avoid charge trapping under singleevent analysis 4 . Among the semiconductors with relatively strong attenuation, high-purity germanium (HPGe) that was developed in the 1970s gives a γ-ray detector the best resolution, which however needs liquid nitrogen cooling due to its small bandgap 5 . Zinc-alloyed CdTe (Cd 1−x Zn x Te, denoted CZT for 0 < x < 0.2) single crystals with a large bandgap of above 1.6 eV possess a high resistivity up to 10 8 ∼ 10 9 cm at room temperature as well as a large µτ product, and thus produce the best resolution γ-ray spectrum among non-cooled semiconductor radiation detectors [6][7][8] .…”
mentioning
confidence: 99%
“…Analysis of the spectra was made using Canberra Genie 2000 software with efficiency models created using ISOCS (Venkataraman et al, 1999(Venkataraman et al, , 2005. The method should be regarded here as semi-quantitative, although the patterns of radionuclide concentration with depth have been verified by analysis of depth slices from cores using conventional low background laboratory gamma spectrometry with a HPGe detector.…”
mentioning
confidence: 99%
“…The GEB can be used to better simulate a physical radiation detector in which energy peaks exhibit Gaussian energy broadening. According to the MCNPX manual the tallied energy is broadened by sampling from the Gaussian [ 21 , 22 ]: where E = the broadened energy, E 0 = the unbroadened energy of the tally, C = a normalization constant, and A = the Gaussian width. The Gaussian width is related to the full width half maximum (FWHM) by The desired FWHM is specified by the user-provided constants, a , b , and c , where The FWHM is defined as where is such that , and is the maximum value of .…”
Section: Resultsmentioning
confidence: 99%