Information driven localisation of a radiological point source
Introduction
Since the end of the Cold War, the risk of nuclear proliferation has increased dramatically due to the relative ease of acquiring radioactive materials [19]. Of growing concern is that numerous accidents have already been reported involving a loss or theft of radioactive sources, which could potentially be used to improvise nuclear devices for high-impact spectacular attacks [19]. A dirty bomb, for example, is a radiological weapon which consists of a conventional explosive packaged with radioactive materials, aimed to kill or injure through the initial blast of the conventional explosive and by airborne radiation and contamination.
This paper proposes a sequential Monte Carlo technique for detection and a subsequent information driven control of the observer for the purpose of parameter estimation of an unaccounted point source of relatively low-level gamma radiation. The search for nuclear materials in a similar context has been considered earlier in [7], [9]. In [7], the authors apply a sequence of statistical hypothesis tests for a survey on a predetermined route. Our goal, however, is to perform an on-line feedback of detection and estimation results into the search plan and thus control the observer motion and the radiation exposure times. Another fundamental difference between our problem formulation and those presented in [7], [9] is that we exploit prior knowledge of the propagation properties of gamma radiation, experimentally verified to obey the inverse distance square law.
The problem can be described informally as follows. Suppose that based on an intelligence report, an area has been identified where an unaccounted radiological source is likely to be found. Our goal is twofold. First, by searching the area, the presence of the source has to be firmly established (this is the detection part). Second, if the source has been detected, it has to be localised in an optimal manner (for example, by minimising the number of measurement acquisition steps, or by minimising the total search time). This second part involves both estimation and resource allocation strategies. Our study is restricted to the case where the point source, to be detected and localised, is static and placed in an open field.
The paper is organised as follows. A formal problem description is presented in Section 2. Section 3 describes the conceptual solution based on the particle filter, for detection and estimation, and the information gain control of the observer. Section 4 details two versions of the particle filter. Section 5 is devoted to the observer control for the purpose of fast, accurate and safe estimation of the source parameters. The numerical simulation results are presented in Section 6 and the findings of this study are summarised in Section 7.
Section snippets
Problem formulation
Suppose an area has been identified in which the potential presence of a radiological point source has to be confirmed. For simplicity, let us assume that this area is flat and rectangular with limits xmin and xmax along axis x and similarly ymin and ymax along axis y.
Equipped with a radiation survey instrument, mounted on a vehicle or carried by a person, the task is to quickly confirm the presence of the source and in the case of positive detection, estimate its location and its level of
Conceptual solution
Let us for a moment disregard the sensor control aspect of the problem (i.e. how the measurements of radiation intensity are collected). The goal is to jointly detect and estimate the source parameter vector using a cumulative set of recorded measurements. The problem has many similarities to the recursive track-before-detect described in [21, Chapter 11], except that the likelihood functions are different and, more importantly, here we treat the problem as a static parameter estimation
Particle filter for integrated detection and estimation
The recursive Bayesian hybrid state estimator, which performs jointly detection and parameter estimation (Steps 5.d and 5.f.(i.)), is implemented as a particle filter (PF). The main idea of the PF is to represent the posterior distribution p(x, E∣Zk) through a finite set of random samples (particles). When a new observation zk+1 is received, the particles are updated in order to represent the new posterior p(x, E∣Zk+1). An additional problem in our context is that both x and E are static
Sensor control
The radiological survey instrument is controlled automatically for the purpose of detection and parameter estimation of a radioactive source. While Pk is below a certain threshold value P∗, in the absence of any prior information on the source location, the measurements are taken along a predefined path that scans the area in a uniform manner (known as the parallel sweeps search [10]). An example of a path scanning the area is shown in Fig. 1, where Δ is the distance between consecutive
Simulation parameters
A radiological point source of an equivalent intensity Is = 18 × 103 cts/s is placed at xs = 240 m, ys = 532 m in a 2D Cartesian plane. Our prior knowledge is as follows: xmin = 100 m, xmax = 600 m, ymin = 300 m, ymax = 800 m, Imin = 8 × 103 cts/s and Imax = 33 × 103 cts/s. The mean count-rate of the background radiation is μb = 1 cts/s. The count measurements were generated using a Poisson random number generator and the propagation model (4).
The parameters of the proposed algorithm are: Np = N/10, N = 30,000, h = 0.005, P∗ = 0.75, Δ = 50
Summary
The paper presented an algorithm for joint detection and parameter estimation of a radiological point source, where the emphasis was on post-detection observer control by maximisation of the Fisher information gain. The numerical simulations show a remarkably good performance of the algorithm under various conditions in the open field environment. There are many possibilities for future research and improvements of the basic algorithm described in this paper. First, a more efficient
Acknowledgments
The authors thank the anonymous reviewers for valuable comments and Mark Rutten (DSTO) and Mark Morelande (The University of Melbourne) for useful technical discussions.
References (26)
- et al.
Optimising the receiver maneuvers for bearings-only tracking
Automatica
(1999) - et al.
Optimal observer motion for localisation with bearings measurements
Comput. Math. Appl.
(1989) - et al.
Improved particle filter for non-linear problems
IEE Proc. F
(1999) - et al.
Novel approach to nonlinear/non-Gaussian Bayesian state estimation
IEE Proc. F
(1993) - A. Gunatilaka, B. Ristic, R. Gailis, On localisation of a radiological point source, in: Proceedings of the...
- J.P. Helferty, D.R. Mudgett. Optimal observer trajectories for bearings-only tracking by minimizing the trace of the...
- et al.
Statistical data evaluation in mobile gamma spectrometry: an optimisation of on-line search strategies in the scenario of lost point sources
Health Phys.
(2001) Monte Carlo filter and smoother for non-Gaussian non-linear state space models
J. Comput. Graphical Stat.
(1996)- et al.
Efficient strategies for low-level nuclear searches
IEEE Trans. Nucl. Sci.
(2006) Search and Scanning
(1980)
A particle algorithm for sequential Bayesian parameter estimation and model selection
IEEE Trans. Signal Process.
Combined parameter and state estimation in simulation-based filtering
Sequential Monte Carlo methods for dynamical systems
J. Am. Stat. Assoc.
Cited by (30)
Multi-robot collaborative radioactive source search based on particle fusion and adaptive step size
2022, Annals of Nuclear EnergyCitation Excerpt :Ristic et al. (2007), Ristic and Gunatilaka (2008) established the posterior probability distribution function (PDF) of the radioactive source parameter vector according to Bayesian theory, which was approximated by particle filters (Ristic et al., 2007; Ristic and Gunatilaka, 2008; Morelande and Ristic, 2009; Huo et al., 2020; Xu et al., 2021) and Monte Carlo methods (Hite et al., 2019; Meutter and Hoffma, 2020). Then, the robot could gradually search for the radioactive source based on the information gain (Ristic et al., 2007; Ristic and Gunatilaka, 2008), information entropy (Xu et al., 2021; Masson et al., 2009), artificial Potential Field (Lin and Tzeng, 2014), Partially Observable Markov Decision Process (POMDP) (Huo et al., 2020) and other methods. Compared with a single robot, multiple robots can take advantage of the synergistic effect in searching for unknown radioactive source in the environment, introducing efficient search time, robustness, and fault tolerance.
A deep reinforcement learning based searching method for source localization
2022, Information SciencesMulti-sensing paradigm based urban air quality monitoring and hazardous gas source analyzing: a review
2021, Journal of Safety Science and ResilienceRegularized Particle Filter based algorithm for the state estimation of orphan gamma source in real time using a backpack gamma spectrometry system
2021, Applied Radiation and IsotopesCitation Excerpt :This methodology could estimate the source activity and source location within 51% and 29% of the actual values, respectively. Sequential Monte Carlo technique for detection and information driven localisation and quantification of an unaccounted point source of relatively low-level gamma radiation has been proposed by Ristic and Gunatilaka (2008). Multiple versions of particle filter can be found in Literature (Ristic et al., 2004) such as Sequential Importance Resampling (SIR) Filter, Auxiliary SIR Filter, Regularized Particle Filter (RPF) etc.
Entrotaxis as a strategy for autonomous search and source reconstruction in turbulent conditions
2018, Information FusionCitation Excerpt :Observations are fused with meteorological data and a dispersion model in order to gain a point estimate or posterior probability density function of source parameters through optimisation [26,27] or Bayesian inference [28] algorithms. The cognitive search formulation has enabled information-driven control for source estimation using a mobile sensor [29]. This paper proposes an alternative cognitive search and source term estimation strategy, termed as Entrotaxis.