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The Feasibility Study for Multigeometries Identification of Uranium Components Using PCA-LSSVM Based on Correlation Measurements.

1. Introduction

The geometry of uranium components is one of the key characteristics and strictly confidential [1, 2]. As for uranium components, they are very difficult to be detected in passive measurements because of the low neutron yield and the weak energy of gamma ray. Uranium components can be shielded easily. Hence, the active method is considered and widely used.

Correlation measurements used for in the field of nuclear material identification have been developed in recent decades [3-11]. In active measurements, [sup.252]Cf sources-driven correlation measurement method is a popular one [12,13]. Based on this method, ORNL (Oak Ridge National Laboratory) had designed a nuclear material identification system (NMIS) aiming to verify the fissile material [14-16]. This method has been used successfully in the past to identify various uranium components, but nearly all of them focused on mass and enrichment [7, 17-19]. Indeed, geometric difference exists practically, but few studies have been done.

In this paper, the research work of the geometry identification to the metal uranium components has been conducted. The uranium components have the same mass, enrichment, and different geometry. Just because the uranium components only have geometric difference, the geometry identification is very difficult by the correlation functions simply. By analyzing the features and differences of the correlation functions, we proposed an identification method combining principal component analysis and least-square support vector machine (PCA-LSSVM) [20, 21] to build an identification model, and the uranium components with different geometries can be effectively distinguished.

2. Methodology

2.1. [sup.252]Cf Sources-Driven Correlation Measurement Method. In [sup.252]Cf sources-driven correlation measurement method, [sup.252]Cf is employed as an interrogating neutron source.[sup.252]Cf source, uranium component, neutron detectors, and relevant data acquisition and display system are included in the measurement setup. Figure 1 shows the flowchart of the verification system. What if the uranium component is irradiated by [sup.252]Cf source, 235U goes through fission readily within 10-14 seconds in average and emits gamma rays, neutrons, and photons [19]. The mutual effects between spontaneous fission neutrons and gamma rays from [sup.252]Cf source and the uranium component are chiefly in three possible processes: penetration, scattering, and induced fission. Then the neutrons and gamma rays are detected and recorded by the detector. This method takes advantage of innumerable neutron counts and makes inferences about the properties of uranium components observed by the correlation function between the [sup.252]Cf source and detector.

2.2. The Correlation Function. As shown in Figure 1, [sup.252]Cf source is placed in an ionization chamber called channel 1 (CH1). The chamber's operation mode is typically pulse mode so that individual source fission event is observable. Neutrons from the [sup.252]Cf source interacting with the uranium component are detected by a scintillator detector, which is placed straightly behind the uranium component and called channel 2 (CH2). The uranium component is placed between the [sup.252]Cf source and the scintillator detector.

Thus, we can obtain signals [X.sub.1](t), [X.sub.2](t + [tau]) from CH1 and CH2, respectively, and derive the correlation function between the two signals. The correlation function [C.sub.12]([tau]), which statistically reflects the correlation neutrons characteristics between two random signals, is defined as

[mathematical expression not reproducible], (1)

where [tau] is the delayed time and T is the observing time. The correlation functions can depict some properties of uranium components, such as enrichment and mass.

Figure 2 shows the correlation function between the [sup.252]Cf source and a detector measured by ORNL [22]. Figure 2 has several meaningful features marking as letters from (a) to (g). (a) denotes the emitting time of [sup.252]Cf spontaneous fission. (b) shows the directly transmitted gamma rays recorded by the detector. (c) means the scattered gamma rays and directly transmitted neutrons. (d) corresponds to the scattered neutrons, the neutrons, and gamma rays from induced fission that are detected lately (e). Some of these divisions are not distinct in time but overlap. For a long time, slow decay (f) will reduce to the background level (g).

2.3. PCA-LSSVM. Principal component analysis (PCA) is a powerful multivariate statistical technique which usually applied to data treatment of high dimensionality. It is based on the reduction of the variable numbers for a lower value of the p-original ones, in order to represent the characteristics of this data set, however, without loss of information. Therefore, it can cover the combination among the variables as well as grouping of samples. Least squares-support vector machine (LS-SVM) is a method based on the Statistical Learning Theory (SLT) that employs a least-square linear system as a cost function, resembling a regularized network. PCA-LSSVM deals with combination of the feature extraction and classification. Geometry identification of the uranium components is separated into two phases: (1) the feature extraction from the correlation functions and feature reduction by PCA and (2) the classification by LSSVM classifier.

3. Simulations, Results, and Discussion

3.1. Simulation Setup and Results. Considering high radioactivity of high-enrichment uranium components, the simulation method is commonly used in the first place instead of making some experiments. In fact, the simulation research will help us further improve the performance of real-data experiments. Correlation measurements were carried out by application of MC simulation. Figure 3 shows the structure of the simulation setup. The distance between the [sup.252]Cf source and the detector is fixed for all measurements.

The particle transport code, Geant 4, was used for all simulations. Figure 4 shows the correlation functions acquired by the MC simulation. In order to make the results more accurate, we remove the transmitted gamma rays by our proposed "rejecting window" method [23, 24]. When [sup.252]Cf spontaneous fission, directly transmitted neutrons, the scattered neutrons, and the neutrons from induced fission all are detected by the detector, the peaks appeared in the curve.

For the neutrons detected by our detectors, we choose part of them whose energy covers 0~20 MeV as the objects to be processed. The average energy of [sup.252]Cf source spontaneous fission neutron is 2.13 MeV. The average energy for the induced neutrons is about 2 MeV. Furthermore, neutron energy decreases when neutrons collide with uranium nuclei, which is beneficial to improving the probability of [sup.235]U fission reaction. Thus, neutrons with energy less than 2 MeV account for the vast majority. Neutrons with energy ranging 2~20 MeV are very few. Neutrons with energy larger than 20 MeV are rare. That is why we choose 0~20 MeV.

Compared with Figures 2 and 4, there are several differences: (1) due to eliminating the transmitted gamma rays, the feature (b) does not exist in Figure 4; (2) the experiment setups are different, such as the mass and enrichment of the uranium component. But beyond that, both results are consistent qualitatively in the total correlation functions. Thus it can be seen that the MC code is skilled in correctly simulating the correlation experiments between the [sup.252]Cf source and detector.

3.2. Geometry Identification Based on Correlation Measurements. Three kinds of uranium components with the same mass (16.9736 kg) and same enrichment (93.15%) but different geometry are used. Table 1 lists the parameters of 3 samples.

Figure 5 shows the correlation functions for the 3 uranium components in different energy intervals. Here we focus on neutron correlation events and remove the gamma rays firstly; there is no gamma peak in Figure 5. The directly transmitted neutrons are the first particles detected by CH2 and then the scattered neutrons and the fission neutrons induced from the uranium components. The correlation function distribution presents a wide range because neutrons move at different velocities. The distribution curves given in Figure 5 show that, as time goes on, the correlation function decreases with the neutron chain reaction progress. Considering the features of the correlation function and compared with the distribution curves after the neutron peak, Figure 5 shows inconsistently in different energy intervals and cannot realize effectively the geometry identification.

To analyze the parameters of 3 uranium components, which have the same enrichment, mass and volume, so they have the same neutron net production. The 3 samples have different geometry, so they have different superficial area. Different superficial areas lead to different neutron leakages. The bigger superficial area has more possibility of stimulating the heavy nuclei and to induce easily more fission. Considering the above, the geometry identification of the 3 samples is very difficult, because there are subtle differences in neutron signals. Even worse, the correlation functions include "real" coincidence and "accidental" coincidence as shown in Figure 6. It is worth noting in Figure 6 that the "accidental" coincidence is chiefly from scatter neutrons which is not conductive to the geometry identification. Unfortunately, the detector just records the neutron counts but cannot pick out the fission neutrons or scatter neutrons. So, the geometry identification is very difficult by the correlation functions simply.

3.3. Geometry Identification Model Based on PCA-LSSVM. In order to identify the geometry of uranium components efficiently, we proposed a method combined principal component analysis and least-square support vector machine (PCA-LSSVM) to build an identification model based on the correlation functions of the 3 different geometry properties. In the above research, the correlation functions were divided into different groups with an energy interval of 0.1 MeV. The sample number of each geometry property was 21. So 21 x 3 = 63 groups of correlation functions were obtained. The 63 groups of correlation functions were shown in Figure 7.

In Figure 7, with the increase of the energy, the correlation functions of the sphere in a high energy level were mixed with the correlation functions of the cylinder in a low level. The similar situation also existed in the correlation functions of cylinder and cuboid, which is consistent with the above results. The geometry property was unable to be identified directly with the correlation functions.

A geometry identification model based on PCA-LSSVM was constructed. Firstly, PCA was applied to extract the feature components from the 63 groups of correlation functions. The feature components were the linear combination of the correlation functions and they were able to characterize the original data well. According to the extraction through PCA, the redundant information was deleted and the dimension was reduced dramatically compared with the original data. The number of the feature components was related to the including information percentage. Normally, an information percentage of no less than 85% contained in feature components was acceptable. In the experiment, the information percentage was selected as 95% and 3 feature components were obtained. The coefficients of the first feature component were shown in Figure 8.

The coefficients of the first feature component were the weights in characterizing the geometry properties with the correlation functions. When building the identification model of the geometry properties, the feature components were applied to replace the correlation functions as the input of the identification model. The labels of the 3 geometry properties were sets 1, 2, and 3 as output of the model corresponding to sphere, cylinder, and cuboid, respectively. Then LSSVM was applied to train the identification model of the geometry properties. In the model training process, the correlation functions were divided into training set and test set with a proportion of 13:8. Radial basis function was selected as the kernel function. The regularization parameter c and kernel width [[sigma].sup.2] of the LSSVM were determined by particle swarm optimization (PSO) method. At last, the identification model was trained and shown in Figure 9. In Figure 9, the distributions of each sample in the principal component feature space were shown. Coordinate axis [X.sub.1] showed the value of first feature component of each sample while the [X.sub.2] showed the second. The identification model divided the space into three parts. Each part represented the region where the feature components of the corresponding geometry property distributed.

The training precision was 100% and the test precision was 95.83% of the identification model. The total precision of the identification model was 98.41%, which indicated that the identification model was an effective way to identify the geometry properties with the correlation functions. However, the number of the sample data shown in this paper was not rich enough. In the future work, more data is expected to be achieved to test the reliability and precision of the identification model. Moreover, the identification model can be optimized for the possibility of identifying the geometry properties with different uranium masses and enrichments.

4. Conclusions

This paper describes a set of simulation experiments for the 3 uranium samples which have the the same mass and enrichment but different geometry. The experiments were performed using [sup.252]Cf sources-driven correlation measurement method, based on the correlation functions. However, the correlation functions are disturbed by "accidental" coincidence chiefly from scatter neutrons and showed disagreement in different energy intervals. Therefore, we cannot realize the geometry identification by the correlation functions directly. We proposed further a method combined principal component analysis and least-square support vector machine (PCA-LSSVM). The results based on PCA-LSSVM showed that the training precision was 100% and the test precision was 95.83% of the identification model. The total precision of the identification model was 98.41%, which indicated that the identification model was an effective way to identify the geometry properties with the correlation functions. Obviously, this correlation function based identification method should be feasible not only for these three geometries but also for other geometries; it is one of our follow-up studies.

Conflicts of Interest

The authors declare that they have no conflicts of interest.


This work was partially supported by the National Natural Science Foundation of China (no. 11605017) and the Fundamental Research Funds for the Central Universities (no. 10611CDJXZ238826).


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Mi Zhou, (1,2) Peng Feng (ID), (1,3) Yixin Liu (ID), (4) and Biao Wei (ID) (1)

(1) Key Laboratory of Optoelectronic Technology and System, Ministry of Education, Chongqing University, Chongqing 400044, China

(2) School of Science, Chongqing University of Technology, Chongqing 400054, China

(3) Collaborative Innovation Center for Brain Science, Chongqing University, Chongqing 400044, China

(4) Department of Engineering Physics, Tsinghua University, Beijing 100084, China

Correspondence should be addressed to Peng Feng; and Biao Wei;

Received 7 December 2017; Accepted 24 January 2018; Published 1 March 2018

Academic Editor: Arkady Serikov

Caption: Figure 1: Flowchart of the proposed identification system.

Caption: Figure 2: Correlation function between [sup.252]Cf source and a detector ([tau] > 0).

Caption: Figure 3: Structure of the simulation setup.

Caption: Figure 4: Simulation results of the sphere uranium component.

Caption: Figure 5: Simulation results of neutron correlation function.

Caption: Figure 6: Simulation results of "real" and "accidental" coincidence.

Caption: Figure 7: 63 groups of correlation functions of 3 different geometry properties.

Caption: Figure 8: Coefficients of the first feature component.

Caption: Figure 9: Identification model of the geometry properties trained by LSSVM.
Table 1: Parameters of the 3 uranium components.

Geometry         Dimension              Volume

Sphere         Radius: 6 cm       9.05 x [10.sup.2]

Cylinder       Radius: 6 cm       9.05 x [10.sup.2]
               Height: 8 cm           [cm.sup.3]

Cuboid         Length: 10 cm      9.05 x [10.sup.2]
               Width: 10 cm           [cm.sup.3]
              Height: 9.05 cm

Geometry        Surface area

Sphere        452.39 [cm.sup.2]

Cylinder      527.79 [cm.sup.2]

Cuboid        561.91 [cm.sup.2]
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Title Annotation:Research Article
Author:Zhou, Mi; Feng, Peng; Liu, Yixin; Wei, Biao
Publication:Science and Technology of Nuclear Installations
Article Type:Report
Date:Jan 1, 2018
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