亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        THE CONVERGENCE OF NONHOMOGENEOUS MARKOV CHAINS IN GENERAL STATE SPACES BY THE COUPLING METHOD?

        2021-10-28 05:45:28ZhifengZHU朱志鋒

        Zhifeng ZHU(朱志鋒)

        School of Mathematics and Statistics,Hubei Engineering University,Xiaogan 432000,China Hubei Province Key Laboratory of Systems Science in Metallurgical Process(Wuhan University of Science and Technology),Wuhan 430081,China

        E-mail:376574200@qq.com

        Shaoyi ZHANG(張紹義)Fanji TIAN(田范基)?

        Hubei Key Laboratory of Applied Mathematics,School of Mathematics and Statistics,Hubei University,Wuhan 430062,China

        E-mail:zhshaoyi@aliyun.com;tianfj1837@sina.com

        Abstract We investigate the convergence of nonhomogeneous Markov chains in general state space by using the f norm and the coupling method,and thus,a sufficient condition for the convergence of nonhomogeneous Markov chains in general state space is obtained.

        Key words f norm;coupling;nonhomogeneous Markov chains;convergence

        1 Introduction

        Because of the requirement of the application of Markov chains in the Monte Carlo method(MCMC),the ergodicity of time-homogeneous Markov chains has attracted considerable interest in the statistical community.The convergence of Markov chains was introduced in Meyn and Tweedie[1],Kartashov[2],Mukhamedov[3],Mukhamedov[4].Currently there already exist mature results on the convergence of the time-homogeneous Markov process in which Probabilistic Distance has been widely employed;see,for example,Theorem 5.22 and Theorem 5.23 of Chen[5].However,the ergodicity of time-homogeneous Markov chains is not enough in the application of MCMC.Therefore,it is necessary to discuss convergence of nonhomogeneous Markov chains.

        Since non-homogeneous Markov chains are an extremely difficult aspect in the study of Markov processes,judging the convergence of Markov chains has been the pursuit of many scholars.The Dobrushin-Isaacson-Madsen theorem studies Markov chains in terms of finite state space(Gong and Qian[6]).In this paper,a conclusion about the convergence of nonhomogeneous Markov chains is drawn for general state space.Theorem 1.1(Dobrushin-Isaacson-Madsen theorem)is a special case of Theorem 1.2.The following Dobrushin-Isaacson-Madsen theorem gives a sufficient condition for the convergence of nonhomogeneous Markov chains in finite state space.

        De finition

        Let v be the signed measure on

        B

        (X),and let g and f be measurable functions on

        B

        (X).De fine

        and

        De finition

        The Markovprocess{Φ,t∈R}is called ergodic if there is a unique invariant measure π that satis fies

        De finition

        Let f be measurable function on

        B

        (X).The Markov process{Φ,t∈R}is called f-ergodic if f≥1 satis fies that

        (i) Φis a positive Harris recurrent and has an invariant measure π;

        (ii) π(f)<∞;

        (iii)for any initial state of x,

        If f≡1,the f norm becomes the total variation norm,and accordingly,the f-ergodic becomes ergodic.

        Theorem 1.1

        (Dobrushin-Isaacson-Madsen Theorem[6]) Let X={X,X,···,X,···}be a non-homogeneous Markov chain in the finite state space S,and let Pbe the transfer probability matrix of its n-th step.Assume that

        (A.1)there is a stationary distribution πwhen Pis a homogeneous transfer matrix;

        (A.3)these either satisfy the Isaacson-Madsen condition,that for any probability distribution vectorμ,ν on S and with positive integer j,we always get

        or they satisfy the Dobrushin condition,that for any integer j,if we let P=(P···P)=(P),C(P),i.e.,the contraction coefficient of P,we have

        where

        Then,there is a probability measure π on S such that

        (1)‖π?π‖→0,n→∞;

        (2)for any arbitrary initial distributionμ,the distributionμof the nonhomogeneous Markov chains always has a limit

        where‖v‖is the total variation norm of the signed measure v on S.

        We extend Theorem 1.1 from the finite state space S to the generalPolish space(X,ρ,

        B

        (X)).Let(X,

        B

        (X))be a Polish space,where

        B

        (X)is an σ algebra generated by a countable subset of X.Throughout the paper,we denote by g a measurable function on X.by v the signed measure on

        B

        (X),and by K a measurable nuclear on(X,

        B

        (X)).We de fine

        De finition

        Let v be the signed measure on

        B

        (X),and let g and f be measurable functions on

        B

        (X).De fine

        and

        Let ?(x,y):=d(x,y)[f(x)+f(y)],where

        Let Φ={Φ,Φ,···,Φ,···}be a nonhomogeneous Markov chain in(X,ρ,

        B

        (X)),where the transfer probability of its n-th step can be written as P(Φ∈A|Φ=x}:=P(x,A).Furthermore,if P=P=···=P,then we call Φ a time-homogeneous Markov chain.Moreover,let us de fine

        P

        (X)as the all probability measures on X,and xas any given point on X,and also set

        M

        ={μ∈

        P

        (X):R?(x,x)μ(dx)<∞}.

        Theorem 1.1 introduces the convergence of nonhomogeneous Markov chains in the finite state space.In practice,however,this is not enough.Zhang[7]introduced the existence of Markov chains coupling.Zhu and Zhang[8]studied the convergenceof nonhomogeneous Markov chains in general state space using Probabilistic Distance and the coupling method.Now,we will study the convergence of nonhomogeneous Markov chains in general state space using the f norm and the coupling method.

        Theorem 1.2

        Let(X,

        B

        (X))be a Polish space,and let Φ={Φ,Φ,···,Φ,···}be a nonhomogeneous Markov chain on X.Furthermore,let{P;n=1,2,···}be the corresponding sequence of probability kernel of Φ.Assume that

        Then,there exists a probability measure π in

        M

        such that,for a probability measureμin

        M

        ,we have

        Remark 1

        In general,the condition in the theorem(iv)is easily veri fiable.In particular,this condition is automatically satis fied when ? is a bounded distance.

        Remark 2

        When f≡1,the f norm becomes the total variation norm,in which case Theorem 1.2 is considered,like Theorem 1.1,a general state.

        2 Preliminaries

        We denote by K(μ,μ)all coupling ofμandμ.

        De finition

        Lettingμandμbe probability measures in the Polish space(X,ρ,

        B

        (X)),

        Lemma 2.1

        (Lindvall[9]) Letμandμbe probability measures on

        B

        (X),and let

        Then,we have the following:

        1.0 ≤γ≤1;

        2.vand vare two probability measures on

        B

        (X);3.Q is a probability measure on

        B

        (X)×

        B

        (X).

        Furthermore,let

        Lemma 2.2

        Letμ,μbe probability measures.Hence,we obtain

        Therefore,‖μ?μ‖∈

        M

        .

        Lemma 2.4

        Letμ,μbe probability measures,and let Pbe a probability kernel on Polish space(X,ρ,

        B

        (X)).Assume that

        Proof

        From(2.2),we obtain that

        As the years passed, other occasions--birthdays, recitals13, awards, graduations--were marked with Dad s flowers. My emotions continued to seesaw14 between pleasure and embarrassment.

        which means that

        Now we only need to prove that

        Therefore{μ:n≥1}is a Cauchy sequence.

        3 Proof of the Main Result

        Next,we use three steps to prove The theorem 1.2:

        (a)For?μ,μ∈

        M

        and any positive integer j,we have

        (b)There exists a probability measure π∈

        M

        such that

        Lemma 2.7 implies that{

        M

        ,W}is a complete metric space.Lemma 2.8 implies that{π:n≥1}is a Cauchy sequence on{

        M

        ,W}.Then there exists π∈

        M

        such that‖π?π‖→0,n→∞.Thus(b)holds.

        (c)We will prove that for?ε>0,?N∈zsuch that for n>N we have that

        For any positive integer j≤n,by triangle inequality we have

        Applying the condition πP=πrepeatedly to the second item above,we can deduce that

        We again apply(3.9)and(3.10)to(3.4),and thus(3.3)holds.The proof of Theorem 1.2 is completed.

        4 Remark on Theorem 1.2

        Remark 1

        The condition(ii)can be replaced by the following:there is cuncorrelated with x,y that satis fies 0≤c≤1 such tha,t for?μ,μ∈

        M

        ,

        Remark 2

        The condition(ii)can be replaced by the following:there is cuncorrelated with x,y that satis fies 0≤c≤1 such that

        where ?(x,y):=d(x,y)[f(x)+f(y)],and f≥1 is a measurable function.

        Remark 3

        The condition(iv)can be replaced by P∈

        M

        .

        For P∈

        M

        ,μ∈

        M

        ,

        Thus,

        Therefore,μP∈

        M

        .

        欲香欲色天天综合和网| 久久综合给合久久狠狠狠97色69| 毛片毛片免费看| 久久综合激激的五月天| 日韩一区二区av极品| 波多野42部无码喷潮在线| 人妻去按摩店被黑人按中出 | 开心五月激情综合婷婷| 国产午夜精品福利久久| 亚洲av日韩av天堂久久不卡| 蓝蓝的天空,白白的云| 久久精品国产亚洲av果冻传媒| 老司机在线精品视频网站| 亚洲a人片在线观看网址| 国产av精选一区二区| 免费无码不卡视频在线观看| 亚洲美国产亚洲av| 亚洲色无码中文字幕| 国内免费自拍9偷1拍| 国模无码一区二区三区| 亚洲激情成人| 少妇高潮太爽了免费网站| 欧美牲交a欧美牲交| 久久av高潮av无码av喷吹| 亚洲精品国产品国语在线app | 亚洲精品av一区二区| 女人高潮被爽到呻吟在线观看| 夜夜爽无码一区二区三区| 亚洲一区二区三区最新视频| 18禁在线永久免费观看| 亚洲av无码第一区二区三区| 一区二区三区免费视频网站 | 色综合天天综合网国产成人网| 亚洲av永久无码精品国产精品| 日韩av一区二区三区四区av| 国产3p一区二区三区精品| 久久久久人妻一区精品| 在线观看91精品国产免费免费| 视频一区二区不中文字幕| 妺妺窝人体色www在线| 大地资源在线播放观看mv|