María Fernanda Moreno-López, Angel Joel Lara-Martinez, Astrid Maritza Gonzalez-Zapata, Alejandro Silva-Juarez, Luis Gerardo de la Fraga, Esteban Tlelo-Cuautle
{"title":"FPGA Implementation of PRNGs Based on Chaotic Systems Optimized by DE, GWO, and PSO","authors":"María Fernanda Moreno-López, Angel Joel Lara-Martinez, Astrid Maritza Gonzalez-Zapata, Alejandro Silva-Juarez, Luis Gerardo de la Fraga, Esteban Tlelo-Cuautle","doi":"10.1002/cta.4435","DOIUrl":null,"url":null,"abstract":"<div>\n \n <p>The optimization of chaotic systems remains a challenge because the search space of the design parameters can have several orders of magnitude, causing that the corresponding eigenvalues can be very sparse, thus producing unnecessary long simulation times. This imposes the need of estimating the step-size \n<span></span><math>\n <mi>h</mi></math> of the numerical method that discretizes the ordinary differential equations. In this manner, the proposed work shows the optimization of chaotic systems, by applying differential evolution (DE), grey wolf optimization (GWO), and particle swarm optimization (PSO) algorithms. Within the optimization loop, \n<span></span><math>\n <mi>h</mi></math> is estimated taking into account the inverse of the highest eigenvalue, and the total time simulation is estimated by taking the inverse of the lowest eigenvalue. The constraints consider that a chaotic system is simulated only if there exist two complex eigenvalues and if the Fourier transform of the chaotic time series has a spectrum area in a certain threshold. A single-objective function is associated to maximize the Kaplan–Yorke dimension \n<span></span><math>\n <msub>\n <mrow>\n <mi>D</mi>\n </mrow>\n <mrow>\n <mi>K</mi>\n <mi>Y</mi>\n </mrow>\n </msub></math>, and then PSO, DE, and GWO are executed with the same number of runs, generations, and population individuals. Their performances are compared by Wilcoxon and Levene tests. The best solutions obtained for each optimization algorithm and for each chaotic system are used to implement pseudo-random number generators (PRNG). Finally, the PRNGs that passed NIST and TestU01 tests are implemented into a field-programmable gate array.</p>\n </div>","PeriodicalId":13874,"journal":{"name":"International Journal of Circuit Theory and Applications","volume":"53 10","pages":"5875-5892"},"PeriodicalIF":1.6000,"publicationDate":"2025-01-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Circuit Theory and Applications","FirstCategoryId":"5","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/cta.4435","RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
Abstract
The optimization of chaotic systems remains a challenge because the search space of the design parameters can have several orders of magnitude, causing that the corresponding eigenvalues can be very sparse, thus producing unnecessary long simulation times. This imposes the need of estimating the step-size
of the numerical method that discretizes the ordinary differential equations. In this manner, the proposed work shows the optimization of chaotic systems, by applying differential evolution (DE), grey wolf optimization (GWO), and particle swarm optimization (PSO) algorithms. Within the optimization loop,
is estimated taking into account the inverse of the highest eigenvalue, and the total time simulation is estimated by taking the inverse of the lowest eigenvalue. The constraints consider that a chaotic system is simulated only if there exist two complex eigenvalues and if the Fourier transform of the chaotic time series has a spectrum area in a certain threshold. A single-objective function is associated to maximize the Kaplan–Yorke dimension
, and then PSO, DE, and GWO are executed with the same number of runs, generations, and population individuals. Their performances are compared by Wilcoxon and Levene tests. The best solutions obtained for each optimization algorithm and for each chaotic system are used to implement pseudo-random number generators (PRNG). Finally, the PRNGs that passed NIST and TestU01 tests are implemented into a field-programmable gate array.
混沌系统的优化仍然是一个挑战,因为设计参数的搜索空间可能有几个数量级,导致相应的特征值可能非常稀疏,从而产生不必要的长仿真时间。这就要求对离散常微分方程的数值方法的步长h进行估计。通过这种方式,提出的工作展示了混沌系统的优化,通过应用微分进化(DE),灰狼优化(GWO)和粒子群优化(PSO)算法。在优化回路中,考虑最高特征值的倒数来估计h,考虑最低特征值的倒数来估计总仿真时间。该约束条件考虑了混沌系统只有在存在两个复特征值且混沌时间序列的傅里叶变换在一定阈值范围内具有谱域时才能被模拟。将单目标函数关联到最大化Kaplan-Yorke维D K Y,然后使用相同数量的运行、代和种群个体执行PSO、DE和GWO。采用Wilcoxon和Levene检验对其性能进行比较。利用各优化算法和混沌系统的最优解实现伪随机数生成器。最后,通过NIST和test01测试的prng被实现到一个现场可编程门阵列中。
期刊介绍:
The scope of the Journal comprises all aspects of the theory and design of analog and digital circuits together with the application of the ideas and techniques of circuit theory in other fields of science and engineering. Examples of the areas covered include: Fundamental Circuit Theory together with its mathematical and computational aspects; Circuit modeling of devices; Synthesis and design of filters and active circuits; Neural networks; Nonlinear and chaotic circuits; Signal processing and VLSI; Distributed, switched and digital circuits; Power electronics; Solid state devices. Contributions to CAD and simulation are welcome.