Calculating off-axis efficiency of coaxial HPGe detectors by Monte Carlo simulation
In beam geometries where a directed γ-ray beam hits the surface of a coaxial high purity germanium detector (HPGe), the detector efficiency is sensitive to the position where γ-rays initially hit the detector surface because the structure of the detector is nonuniform. This may cause inaccuracy of t...
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Veröffentlicht in: | Radiation physics and chemistry (Oxford, England : 1993) England : 1993), 2022-09, Vol.198, p.110241, Article 110241 |
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Sprache: | eng |
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Zusammenfassung: | In beam geometries where a directed γ-ray beam hits the surface of a coaxial high purity germanium detector (HPGe), the detector efficiency is sensitive to the position where γ-rays initially hit the detector surface because the structure of the detector is nonuniform. This may cause inaccuracy of the detector efficiency when measured using standard sources that are point-like sources emitting γ-rays isotropically. Obtaining a precise estimation of the full energy peak efficiency of the coaxial HPGe detector in the beam geometry for on-axis and off-axis measurements requires a Monte Carlo simulation. We performed Monte Carlo simulations that calculate the detector efficiency in the beam geometry. The effects of the off-axis distance and γ-ray beam size on the efficiency are quantitatively analyzed. We found that the intrinsic efficiency in the beam geometry is maximized when the beam hits the detector at specific off-axis distances. Our Monte Carlo calculations have been supported by nuclear resonance fluorescence experiments using laser Compton scattering γ-ray beams.
•Calculating efficiency of coaxial HPGe detector for directed γ-ray beams by Geant4.•Revealing the sensitivity of efficiency to γ-ray beam size and off-axis distance.•Off-axis efficiency is higher than on-axis efficiency, depending on γ-ray energy.•Maximizing efficiency by selecting the optimum off-axis distance.•LCS γ-ray beams up to 3 MeV validate calculations experimentally. |
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ISSN: | 0969-806X 1879-0895 |
DOI: | 10.1016/j.radphyschem.2022.110241 |