{"title":"无网格加权粒子法在Vlasov-Poisson方程中的应用","authors":"Yoann Le Henaff","doi":"10.1007/s00211-023-01378-4","DOIUrl":null,"url":null,"abstract":"We study a grid-free particle method based on following the evolution of the characteristics of the Vlasov–Poisson system, and we show that it converges for smooth enough initial data. This method is built as a combination of well-studied building blocks—mainly time integration and integral quadratures—and allows to obtain arbitrarily high orders. By making use of the Non-Uniform Fast Fourier Transform, the overall computational complexity is $$ {\\mathcal {O}}(P \\log P + K^d \\log K^d) $$ , where $$ P $$ is the total number of particles and where we only keep the Fourier modes $$ k \\in ({\\mathbb {Z}}^d)^* $$ such that $$ k_1^2 + \\dots + k_d^2 \\le K^2 $$ . Some numerical results are given for the Vlasov–Poisson system in the one-dimensional case.","PeriodicalId":2,"journal":{"name":"ACS Applied Bio Materials","volume":null,"pages":null},"PeriodicalIF":4.6000,"publicationDate":"2023-10-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Grid-free weighted particle method applied to the Vlasov–Poisson equation\",\"authors\":\"Yoann Le Henaff\",\"doi\":\"10.1007/s00211-023-01378-4\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We study a grid-free particle method based on following the evolution of the characteristics of the Vlasov–Poisson system, and we show that it converges for smooth enough initial data. This method is built as a combination of well-studied building blocks—mainly time integration and integral quadratures—and allows to obtain arbitrarily high orders. By making use of the Non-Uniform Fast Fourier Transform, the overall computational complexity is $$ {\\\\mathcal {O}}(P \\\\log P + K^d \\\\log K^d) $$ , where $$ P $$ is the total number of particles and where we only keep the Fourier modes $$ k \\\\in ({\\\\mathbb {Z}}^d)^* $$ such that $$ k_1^2 + \\\\dots + k_d^2 \\\\le K^2 $$ . Some numerical results are given for the Vlasov–Poisson system in the one-dimensional case.\",\"PeriodicalId\":2,\"journal\":{\"name\":\"ACS Applied Bio Materials\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":4.6000,\"publicationDate\":\"2023-10-26\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"ACS Applied Bio Materials\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1007/s00211-023-01378-4\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, BIOMATERIALS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"ACS Applied Bio Materials","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1007/s00211-023-01378-4","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, BIOMATERIALS","Score":null,"Total":0}
引用次数: 0
摘要
我们研究了一种基于跟踪Vlasov-Poisson系统特征演变的无网格粒子方法,并证明了它在足够光滑的初始数据下是收敛的。这种方法是建立在一个充分研究的构建模块的组合-主要是时间积分和积分正交-并允许获得任意高阶。通过使用非均匀快速傅里叶变换,总的计算复杂度是$$ {\mathcal {O}}(P \log P + K^d \log K^d) $$,其中$$ P $$是粒子的总数我们只保留傅里叶模式$$ k \in ({\mathbb {Z}}^d)^* $$这样$$ k_1^2 + \dots + k_d^2 \le K^2 $$。给出了一维情况下Vlasov-Poisson系统的一些数值结果。
Grid-free weighted particle method applied to the Vlasov–Poisson equation
We study a grid-free particle method based on following the evolution of the characteristics of the Vlasov–Poisson system, and we show that it converges for smooth enough initial data. This method is built as a combination of well-studied building blocks—mainly time integration and integral quadratures—and allows to obtain arbitrarily high orders. By making use of the Non-Uniform Fast Fourier Transform, the overall computational complexity is $$ {\mathcal {O}}(P \log P + K^d \log K^d) $$ , where $$ P $$ is the total number of particles and where we only keep the Fourier modes $$ k \in ({\mathbb {Z}}^d)^* $$ such that $$ k_1^2 + \dots + k_d^2 \le K^2 $$ . Some numerical results are given for the Vlasov–Poisson system in the one-dimensional case.