Monte Carlo simulations to advance characterisation of landmines by pulsed fast/thermal neutron analysis
Introduction
Urged by the latest tragic events and their aftermath, the world's attention has been re-captured to detection and characterisation of narcotics, explosives, contraband, landmines and unexploded ordnance (Hussein and Waller, 2000; BBC, 2003). For these applications, the development of nuclear radiation–detection techniques has strongly been stimulated to provide elemental characterisation and “fingerprint” signature of inspected objects.
However, the actual quantities measured through nuclear techniques do not always correspond to the geological/material parameters desired, a difference that is important to understand. Thus, additional information is required to relate the measurements made with nuclear techniques to representative parameters. As the extent to which laboratory calibrations can mimic complex in situ conditions is limited, Monte Carlo (MC) simulations may significantly contribute to the solution of this problem.
Although MC-based techniques are becoming more and more a prelude to experimental and design work, their applications to humanitarian de-mining (HD) are only very recent. The MC code MCNP (Briesmeister, 1999) was applied on a simple idealised geometry of a land-mine detector exposed to a 241Am–Be neutron source (Hussein, 1999). The results provide some basic conclusions in terms of detector response for thermal and fast neutrons as well as γ-rays produced in activation and by scattering. Maučec and de Meijer (2002) have assessed the MCNP as a feasibility tool for quantification of a thermal-neutron backscattering-based detector system for detection of non-metallic landmines. Several other authors (e.g. ElAgib and Csikai, 1999; Hlaváč, 1999; Pesente et al., 2001; Tickner (1999), Tickner (2000)) reported on the application of MC simulations for design of probing tools and optimisation of detector responses using various codes. Maučec and de Meijer (2001) proposed further development of the perturbation MC method, to advance the data interpretation and elemental characterisation in HD. Recently, a project was funded by the International Atomic Energy Agency (IAEA) (Rigollet et al., 2003) aiming at the development of MC simulation techniques to optimise the performance of the bismuth–germanate (BGO) detector system of pulse-neutron elemental analysis (PELAN) (Vourvopoulos and Womble, 2001).
In this paper, a development of MC simulation techniques at Nuclear Geophysics Division of Kernfysisch Versneller Instituut, Groningen, the Netherlands (NGD/KVI), to enhance the data analysis and interpretation of a pulse-neutron-based system is outlined. The work is based on the MCNP calculation of BGO detector responses in mixed (n,γ) fields and set-up of a database of standard responses required for the Full Spectrum Analysis (FSA) of γ-ray spectra.
The MC modelling of a simplified land-mine detector set-up, using a 14 MeV pulse-neutron source is presented in Section 2. In Section 3 the computational methods, aiming at the assessment of the neutron-induced background in the BGO detector and the generation of standard detector responses to the elements relevant for application of nuclear methods in HD are described and followed by the discussion of the results in Section 4. The last section provides conclusions and some guidelines for the future work.
Section snippets
MC modelling aspects
The general-purpose MC code MCNP4C was used for modelling the pulse-neutron DT (deuterium–tritium; PNDT) system schematically depicted in Fig. 1. The ∼14 MeV neutron source (108 n/s), radiating “almost” isotropically, is located a few centimetres above the conical neutron shield. The exact energy-spatial distribution of the DT source applied in our simulations was taken from (IAEA, 1987) and shown in Fig. 2.
A cylindrical, 7.6 cm×∅5 cm, BGO detector (ρBGO=7.13 g/cm3, Z=84), with an energy resolution
Computational methods
Initially, the MC simulations of the PNDT tool for the elemental characterisation of explosives and landmines have combined the assessment of the neutron-induced background in the BGO detector and the calculation of standard responses of the BGO detector to γ-rays (i.e. standard spectra, per unit elemental concentration of specific element).
Results
Originally, the spectra, calculated by MCNP are given normalised per starting particle. The standard spectra in Fig. 6, Fig. 7, Fig. 8, Fig. 9 are given in counts per unit (atom) concentration and smoothed with 5-point running average. By applying MC computational techniques, as described in Section 3, it was possible to decompose the combined scintillation detector response to γ-rays on two components, induced by neutron inelastic scattering and capture events. However, before being used for
Conclusions and discussion
In this paper, the MC modelling of the simplified 14 MeV pulse-neutron source based system for characterisation of landmines is presented. The simulations indicate that the pulsed fast/thermal neutron analysis (PFTNA) technique requires relatively high concentrations (∼20%) of soil moisture, to efficiently moderate fast neutrons (∼14 MeV) to lower energies (∼1 eV), where they can induce the characteristic thermal neutron capture γ-rays, thus providing the information on elemental composition. This
Acknowledgements
The research work was performed under IAEA Co-ordinated Research Project (CRP) “The application of nuclear methods to Anti-Personnel Landmine detection”. The authors would like to acknowledge James Tickner, for his assistance in providing MCNP neutron cross-section data for Germanium isotopes and for valuable discussions on the simulations of neutron-induced scintillator responses.
References (21)
- et al.
Validation of neutron data libraries by backscattered spectra of Pu-Be neutrons
Nucl. Instrum. Methods A
(1999) - et al.
MCNP modelling of scintillation-detector gamma-ray spectra from natural radionuclides
Appl. Radiat. Isot.
(2002) - et al.
Landmine detectionthe problem and the challenge
Appl. Radiat. Isot.
(2000) - et al.
Monte Carlo simulations as a feasibility tool for non-metallic land-mine detection by thermal-neutron backscattering
Appl. Radiat. Isot.
(2002) - et al.
Effects of soil moisture on the detection of buried explosives by radiative neutron capture
Nucl. Instrum. Methods A
(2001) - et al.
Prompt gamma rays from radioactive capture of thermal neutrons by elements from hydrogen through zinc
At. Data Nucl. Data Tables
(2002) Determination of the spatial response of neutron based analysers using a monte carlo based method
Appl. Radiat. Isot.
(2000)- et al.
Pulsed fast/thermal neutron analysisa technique for explosive detection
Talanta
(2001) - BBC News, World Edition, 2003. Landmine stocks ‘over 200 million’....
- Briesmeister, J. (Ed.), 1999. MCNP4C, A Monte Carlo N-Particle Transport Code System. Report CCC-660, Los Alamos...
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