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Full characterization of an old HPGe detector (GEROS)
V. Angelopoulou E. Kouvaris V. Lagaki T.J. Mertzimekis P. Papagiannis
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Outline: Story of GEROS Motivation Characterization Techniques
Simulations Conclusion
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What is GEROS GEROS stands for Germanium for Environmental
RadiOactivity Studies An old, p-type, 20% HPGe detector, coaxial crystal geometry Has already been used for some environmental γ-ray spectroscopy
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Why ? Only information available:
A full characterization was needed before putting it back to operation 14 mm 53.6 mm 48.6 mm 53.4 mm
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At 15 cm : Sources 60Co 137Cs 152Eu 226Ra
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Fit with 2nd order polynomial E = A+B(chn)+C(chn)2
Linearity: 152Eu, 15 cm Parameters Curve fit A 9.2 B 0.6435 C 9.2∙10-8 Resolution (FWHM):
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IAEA Ref.154, C. Potiriadis Weight (g) Element Energy (keV) ε (%)
δε (%) 3.245 137Cs 661.75 2.78 0.04 40Κ 2.03 2.956 661.38 1.96 1.43 19.781 661.68 1.427 0.012 0.361 0.007 32.736 661.7 1.192 0.009 0.228 0.004 92.48 661.71 1.155 0.011 0.125 IAEA Ref.154, C. Potiriadis
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The experimental setup
Liquid N2 Dewar container Alignment laser Pb collimator 134Cs source Shield consists of four 5-cm thick Pb bricks: 2 used for vertical dimension and 2 for parallel 3 x 3 mm2 collimation hole X-Y motion platform
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The 134Cs spectrum (t1/2 = 2.0652 y) Δt = 10 min
The energy spectrum of 134Cs, from GEROS, taken at (x,y)=(0,0) position More than 700 spectra were collected and analyzed Δt = 10 min SpectrW, C.Kalfas
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Results of gamma ray tomography
Diagrams of counts in a vertical scanning, for fixed x position x = -9 mm x = -3 mm x = 0 mm x = 3 mm x = 6 mm x = 9 mm Diagrams of counts in a horizontal scanning, for fixed y position y = -12mm y = -6 mm y = -3 mm y = 0 mm y = 3 mm y = 9 mm
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Reconstructed 3D model
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Study of the results Estimation of the center of the crystal : (0, -2)
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The crystal appears to be tilted
25 mm mm 18 mm mm
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Estimation of the crystal’s diameter
Int. Diam.: 8 ± 1.5 mm Int. Diam.: 12 ± 3 mm Ext. Diam.: 46 ± 1.5 mm Ext. Diam.: 48 ± 3 mm
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Can we confirm this? GEROS was CT scanned (X-ray Computed Tomography)
Front view GEROS was CT scanned (X-ray Computed Tomography) Side view Full view
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MCNP simulation Eu keV
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Conclusions An old HPGe detector was put back
to operation and fully characterized From γ-ray and CT tomographies the exact geometry was deduced and fully reconstructed in 3D The detector has suffered some loss of efficiency due to prolonged inactivity (dead layer built up) MCNP simulations have been performed and found to agree well with the experimental data Efficiencies for several bulk sample geometries were estimated by means of an IAEA reference material Overall the detector can be used for γ-ray spectroscopy and educational activities at UoA
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Thanks to The TANDEM accelerator staff, and especially Dr. M.Axiotis
The Lefkos Stavros hospital and staff Dr. C.Potiriadis for the IAEA reference material Dr. C.Kalfas for SpectrW licences
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Thank you for your attention!
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Additional slide The inside-out of the detector
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