{"title":"具有跳跃的交互无限马尔可夫粒子系统","authors":"Seiji Hiraba","doi":"10.21099/TKBJM/1373893404","DOIUrl":null,"url":null,"abstract":"In [2] we investigated independent infinite Markov particle systems as measure-valued Markov processes with jumps, and we gave sample path properties and martingale characterizations. In particular, we investigated the exponent of Hölder-right continuity in case that the motion process is absorbing a-stable motion on ð0;yÞ with 0 < a < 2, that is, time-changed absorbing Brownian motions on ð0;yÞ by the increasing a=2-stable Lévy processes. In the present paper we shall extend the results to the case of simple interactive infinite Markov particle systems. We also consider the absorbing stable motion on a half space H 1⁄4 R 1 ð0;yÞ as a motion process. 1. Settings and Previous Results In this section we give the general settings and the known results which are given in [2] in order to describe the main results in § 3 and § 4. Let S be a domain of R . Let ðwðtÞ;PxÞtb0;x AS be a S-valued Markov process having life time zðwÞ A ð0;y such that w A Dð1⁄20; zðwÞÞ ! SÞ, i.e., w : 1⁄20; zðwÞÞ ! S is right continuous and has left-hand limits. For convenience, we fix an extra point D B S and set wðtÞ 1⁄4 D if tb zðwÞ. Moreover we shall extend functions f on S to on fDg by f ðDÞ 1⁄4 0, if necessary. We use the following notations: Let SHR be a domain. If x 1⁄4 ðx1; . . . ; xdÞ A R , then q i1 ik 1⁄4 q k=ðqxi1 qxik Þ, q i 1⁄4 q =ðqxk i Þ and qi 1⁄4 q i for each k 1⁄4 0; 1; . . . , i 1⁄4 1; . . . ; d. Moreover qt 1⁄4 q=qt for time tb 0. 2000 Mathematics Subject Classification: Primary 60G57; Secondary 60G75.","PeriodicalId":44321,"journal":{"name":"Tsukuba Journal of Mathematics","volume":"37 1","pages":"27-50"},"PeriodicalIF":0.3000,"publicationDate":"2013-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.21099/TKBJM/1373893404","citationCount":"0","resultStr":"{\"title\":\"Interactive infinite Markov particle systems with jumps\",\"authors\":\"Seiji Hiraba\",\"doi\":\"10.21099/TKBJM/1373893404\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In [2] we investigated independent infinite Markov particle systems as measure-valued Markov processes with jumps, and we gave sample path properties and martingale characterizations. In particular, we investigated the exponent of Hölder-right continuity in case that the motion process is absorbing a-stable motion on ð0;yÞ with 0 < a < 2, that is, time-changed absorbing Brownian motions on ð0;yÞ by the increasing a=2-stable Lévy processes. In the present paper we shall extend the results to the case of simple interactive infinite Markov particle systems. We also consider the absorbing stable motion on a half space H 1⁄4 R 1 ð0;yÞ as a motion process. 1. Settings and Previous Results In this section we give the general settings and the known results which are given in [2] in order to describe the main results in § 3 and § 4. Let S be a domain of R . Let ðwðtÞ;PxÞtb0;x AS be a S-valued Markov process having life time zðwÞ A ð0;y such that w A Dð1⁄20; zðwÞÞ ! SÞ, i.e., w : 1⁄20; zðwÞÞ ! S is right continuous and has left-hand limits. For convenience, we fix an extra point D B S and set wðtÞ 1⁄4 D if tb zðwÞ. Moreover we shall extend functions f on S to on fDg by f ðDÞ 1⁄4 0, if necessary. We use the following notations: Let SHR be a domain. If x 1⁄4 ðx1; . . . ; xdÞ A R , then q i1 ik 1⁄4 q k=ðqxi1 qxik Þ, q i 1⁄4 q =ðqxk i Þ and qi 1⁄4 q i for each k 1⁄4 0; 1; . . . , i 1⁄4 1; . . . ; d. Moreover qt 1⁄4 q=qt for time tb 0. 2000 Mathematics Subject Classification: Primary 60G57; Secondary 60G75.\",\"PeriodicalId\":44321,\"journal\":{\"name\":\"Tsukuba Journal of Mathematics\",\"volume\":\"37 1\",\"pages\":\"27-50\"},\"PeriodicalIF\":0.3000,\"publicationDate\":\"2013-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.21099/TKBJM/1373893404\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Tsukuba Journal of Mathematics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.21099/TKBJM/1373893404\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"MATHEMATICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Tsukuba Journal of Mathematics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.21099/TKBJM/1373893404","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"MATHEMATICS","Score":null,"Total":0}
引用次数: 0
摘要
在[2]中,我们研究了独立无限马尔可夫粒子系统作为具有跳变的测量值马尔可夫过程,并给出了样本路径的性质和鞅刻画。特别地,我们研究了当运动过程吸收了1 -稳定的运动在ð0;yÞ上且0 < a < 2时的Hölder-right连续性指数,即通过增加a=2-稳定的l杂变过程吸收了1 -稳定的布朗运动在ð0;yÞ上。在本文中,我们将结果推广到简单交互无限马尔可夫粒子系统的情况。我们还将半空间H 1⁄4 R 1 ð0;yÞ上的吸收稳定运动视为一个运动过程。1. 在本节中,为了描述§3和§4中的主要结果,我们给出了在[2]中给出的一般设置和已知结果。设S是R的定义域。设ðwðtÞ;PxÞtb0;x为寿命为zðwÞ a ð0;y的s值马尔可夫过程,使得w a Dð1⁄20;zðwÞÞ!SÞ,即w: 1 / 20;zðwÞÞ!S是右连续的,有左极限。为方便起见,我们固定一个额外的点D B S,设wðtÞ 1⁄4 D为zðwÞ。此外,如有必要,我们将函数f on S扩展到on fDg,并将其扩展f ðDÞ 1 / 4 0。我们使用以下符号:设SHR为一个域。如果x1⁄4 × x1;……;xdÞ A R,则qi1 ik 1⁄4 qk = / qxi1 qxik Þ, qi1⁄4 q = / qxk i Þ, qi 1⁄4 qi每k 1⁄4 0;1;……, I 1 / 4 1;……;d.此外,qt 1 / 4 q=qt时间t0。2000数学学科分类:小学60G57;二次60 g75。
Interactive infinite Markov particle systems with jumps
In [2] we investigated independent infinite Markov particle systems as measure-valued Markov processes with jumps, and we gave sample path properties and martingale characterizations. In particular, we investigated the exponent of Hölder-right continuity in case that the motion process is absorbing a-stable motion on ð0;yÞ with 0 < a < 2, that is, time-changed absorbing Brownian motions on ð0;yÞ by the increasing a=2-stable Lévy processes. In the present paper we shall extend the results to the case of simple interactive infinite Markov particle systems. We also consider the absorbing stable motion on a half space H 1⁄4 R 1 ð0;yÞ as a motion process. 1. Settings and Previous Results In this section we give the general settings and the known results which are given in [2] in order to describe the main results in § 3 and § 4. Let S be a domain of R . Let ðwðtÞ;PxÞtb0;x AS be a S-valued Markov process having life time zðwÞ A ð0;y such that w A Dð1⁄20; zðwÞÞ ! SÞ, i.e., w : 1⁄20; zðwÞÞ ! S is right continuous and has left-hand limits. For convenience, we fix an extra point D B S and set wðtÞ 1⁄4 D if tb zðwÞ. Moreover we shall extend functions f on S to on fDg by f ðDÞ 1⁄4 0, if necessary. We use the following notations: Let SHR be a domain. If x 1⁄4 ðx1; . . . ; xdÞ A R , then q i1 ik 1⁄4 q k=ðqxi1 qxik Þ, q i 1⁄4 q =ðqxk i Þ and qi 1⁄4 q i for each k 1⁄4 0; 1; . . . , i 1⁄4 1; . . . ; d. Moreover qt 1⁄4 q=qt for time tb 0. 2000 Mathematics Subject Classification: Primary 60G57; Secondary 60G75.