{"title":"McKean-Vlasov型非线性SDEs的解析逼近","authors":"E. Gobet, S. Pagliarani","doi":"10.2139/ssrn.2868660","DOIUrl":null,"url":null,"abstract":"Abstract We provide analytical approximations for the law of the solutions to a certain class of scalar McKean–Vlasov stochastic differential equations (MKV-SDEs) with random initial datum. “Propagation of chaos“ results ( [15] ) connect this class of SDEs with the macroscopic limiting behavior of a particle, evolving within a mean-field interaction particle system, as the total number of particles tends to infinity. Here we assume the mean-field interaction only acting on the drift of each particle, this giving rise to a MKV-SDE where the drift coefficient depends on the law of the unknown solution. By perturbing the non-linear forward Kolmogorov equation associated to the MKV-SDE, we perform a two-steps approximating procedure that decouples the McKean–Vlasov interaction from the standard dependence on the state-variables. The first step yields an expansion for the marginal distribution at a given time, whereas the second yields an expansion for the transition density. Both the approximating series turn out to be asymptotically convergent in the limit of short times and small noise, the convergence order for the latter expansion being higher than for the former. Concise numerical tests are presented to illustrate the accuracy of the resulting approximation formulas. The latter are expressed in semi-closed form and can be then regarded as a viable alternative to the numerical simulation of the large-particle system, which can be computationally very expensive. Moreover, these results pave the way for further extensions of this approach to more general dynamics and to high-dimensional settings.","PeriodicalId":320844,"journal":{"name":"PSN: Econometrics","volume":"41 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2017-08-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"14","resultStr":"{\"title\":\"Analytical Approximations of Non-Linear SDEs of McKean-Vlasov Type\",\"authors\":\"E. Gobet, S. Pagliarani\",\"doi\":\"10.2139/ssrn.2868660\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Abstract We provide analytical approximations for the law of the solutions to a certain class of scalar McKean–Vlasov stochastic differential equations (MKV-SDEs) with random initial datum. “Propagation of chaos“ results ( [15] ) connect this class of SDEs with the macroscopic limiting behavior of a particle, evolving within a mean-field interaction particle system, as the total number of particles tends to infinity. Here we assume the mean-field interaction only acting on the drift of each particle, this giving rise to a MKV-SDE where the drift coefficient depends on the law of the unknown solution. By perturbing the non-linear forward Kolmogorov equation associated to the MKV-SDE, we perform a two-steps approximating procedure that decouples the McKean–Vlasov interaction from the standard dependence on the state-variables. The first step yields an expansion for the marginal distribution at a given time, whereas the second yields an expansion for the transition density. Both the approximating series turn out to be asymptotically convergent in the limit of short times and small noise, the convergence order for the latter expansion being higher than for the former. Concise numerical tests are presented to illustrate the accuracy of the resulting approximation formulas. The latter are expressed in semi-closed form and can be then regarded as a viable alternative to the numerical simulation of the large-particle system, which can be computationally very expensive. Moreover, these results pave the way for further extensions of this approach to more general dynamics and to high-dimensional settings.\",\"PeriodicalId\":320844,\"journal\":{\"name\":\"PSN: Econometrics\",\"volume\":\"41 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2017-08-31\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"14\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"PSN: Econometrics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.2139/ssrn.2868660\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"PSN: Econometrics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.2139/ssrn.2868660","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 14
摘要
摘要本文给出了一类具有随机初始基准的标量McKean-Vlasov随机微分方程(MKV-SDEs)的解律的解析近似。“混沌传播”(Propagation of chaos)的结果([15])将这类sde与粒子的宏观极限行为联系起来,当粒子总数趋于无穷大时,粒子在平均场相互作用粒子系统中演化。这里我们假设平均场相互作用只作用于每个粒子的漂移,这就产生了MKV-SDE,其中漂移系数取决于未知解的定律。通过扰动与MKV-SDE相关的非线性前向Kolmogorov方程,我们执行了一个两步逼近过程,将McKean-Vlasov相互作用与对状态变量的标准依赖解耦。第一步得到给定时间的边际分布的展开式,而第二步得到跃迁密度的展开式。两种近似级数在短时间和小噪声极限下都是渐近收敛的,后者的收敛阶高于前者。给出了简明的数值试验来说明所得近似公式的准确性。后者以半封闭形式表示,可以被视为大颗粒系统的数值模拟的可行替代方案,这在计算上非常昂贵。此外,这些结果为进一步将该方法扩展到更一般的动力学和高维设置铺平了道路。
Analytical Approximations of Non-Linear SDEs of McKean-Vlasov Type
Abstract We provide analytical approximations for the law of the solutions to a certain class of scalar McKean–Vlasov stochastic differential equations (MKV-SDEs) with random initial datum. “Propagation of chaos“ results ( [15] ) connect this class of SDEs with the macroscopic limiting behavior of a particle, evolving within a mean-field interaction particle system, as the total number of particles tends to infinity. Here we assume the mean-field interaction only acting on the drift of each particle, this giving rise to a MKV-SDE where the drift coefficient depends on the law of the unknown solution. By perturbing the non-linear forward Kolmogorov equation associated to the MKV-SDE, we perform a two-steps approximating procedure that decouples the McKean–Vlasov interaction from the standard dependence on the state-variables. The first step yields an expansion for the marginal distribution at a given time, whereas the second yields an expansion for the transition density. Both the approximating series turn out to be asymptotically convergent in the limit of short times and small noise, the convergence order for the latter expansion being higher than for the former. Concise numerical tests are presented to illustrate the accuracy of the resulting approximation formulas. The latter are expressed in semi-closed form and can be then regarded as a viable alternative to the numerical simulation of the large-particle system, which can be computationally very expensive. Moreover, these results pave the way for further extensions of this approach to more general dynamics and to high-dimensional settings.