Abstract
In the work, we studied the influences of dead layer thickness on the whole gamma spectrum response for HPGe detector by using Monte Carlo simulation. From the simulated relation of the FEPEs and the dead layer thicknesses, the dead layer thickness of 0.567 mm was derived which increased compared with the nominal value of 0.46 mm from manufacturer after 4 years of operation. The multiple scattering region and peak decreased with different rates and the valley region of the forward-scattering photon increased quickly when the dead layer thickness increased. The energy dependence of the P/T and the general range was also carried out. The results showed that the effect of the increase in dead layer thickness on regions in the spectrum was not the same. Through this study, among several scintillators, it was possible to find a HPGe detector suitable for the purpose of the study.
Similar content being viewed by others
References
N Q Huy Nucl. Instrum. Meth. A 621 390 (2010)
T T H Loan, V N Ba, T H N Thy and H T Y Hong J. Rad. Nucl. Chem. 315 95 (2017)
P Dryak and P Kovar Appl. Radiat. Isot. 64 1346 (2006)
J Boson, G Agren and L A Johansson Nucl. Instrum. Meth. A. 587 304 (2008)
A Elanique, A Marzocchi, O Leone, D Hegenbart, L Breustedt, B Oufni and L Dead Appl. Radiat. Isot. 70 538 (2012)
E Andreotti, M Hult, G Marissens, G Lutter, A Garfagnini, S Hemmer and K Von Sturm Appl. Radiat. Isot. 87 331 (2014)
V N Ba, L T H Giang, B N Thien, T T H Loan and N Q Huy Appl. Radiat. Isot 163 109229 (2020)
N Q Huy and D Q Binh Instrum. Meth. A. 573 384 (2007)
J Rodenas and A Pascual J. Ballesteros. Nucl. Instrum. Meth. A 496 390 (2003)
F Courtine, T Pilleyre, S Sanzelle and D Nucl Instrum. Meth. A 596 229 (2008)
W I Zidan J. Nucl. Part. Phys. 5 30–37 (2015)
W I J. Nucl. Part. Phys. 5 30 (2015)
R J Friedman, M C Reichard, T E Blue and A S Brown Health Phys. 80 53 (2001)
R Berndt and P Mortreau Nucl. Instrum Meth. A 694 341 (2012)
A Caciolli et al Sci. Total. Environ. 414 639 (2012)
T Watanabe, Y Oi, M Taki, K Kawasaki and M Yoshida Appl. Radiat. Isot. 50 1057 (1999)
E Sahiner and N A Radiat Phys. Chem. 96 50 (2014)
X-5 Monte Carlo Team Los Alamos National Laboratory. LA-UR-03-1987 (2005)
Z Wang, B Kahn and J D Valentine IEEE Trans. Nucl. Sci. 49 1925 (2002)
P Zombori, A Andrasi and I Nemeth Report KFKI-1992-20/K, IAEA INIS, Hungary (1992)
S I Kafala J. Rad. Nucl. Chem. 191 105 (1995)
A Cesana and M Terrani Nucl. Instrum. Meth. A. 281 172 (1989)
R Venkataraman, R S Croft and W R Russ J. Rad. Nucl. Chem. 264 183 (2005)
Acknowledgements
Our Nuclear Technique Laboratory (NTLab) was invested by Vietnam National University of Ho Chi Minh City, Viet Nam.
Author information
Authors and Affiliations
Corresponding author
Additional information
Publisher's Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Rights and permissions
Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.
About this article
Cite this article
Dao, N.Q., Ba, V.N. & Loan, T.T.H. The effects of the dead layer thickness increase to the regions in the spectrum response for a coaxial HPGe detector. Indian J Phys (2023). https://doi.org/10.1007/s12648-023-03037-8
Received:
Accepted:
Published:
DOI: https://doi.org/10.1007/s12648-023-03037-8