<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">TEL</journal-id><journal-title-group><journal-title>Theoretical Economics Letters</journal-title></journal-title-group><issn pub-type="epub">2162-2078</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/tel.2012.21004</article-id><article-id pub-id-type="publisher-id">TEL-17351</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Business&amp;Economics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Exponential Ergodicity and β-Mixing Property for Generalized Ornstein-Uhlenbeck Processes
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>esook</surname><given-names>Lee</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Statistics, Ewha Womans University, Seoul, Korea (South)</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>oslee@ewha.ac.kr</email></corresp></author-notes><pub-date pub-type="epub"><day>23</day><month>02</month><year>2012</year></pub-date><volume>02</volume><issue>01</issue><fpage>21</fpage><lpage>25</lpage><history><date date-type="received"><day>November</day>	<month>29,</month>	<year>2011</year></date><date date-type="rev-recd"><day>January</day>	<month>13,</month>	<year>2012</year>	</date><date date-type="accepted"><day>January</day>	<month>20,</month>	<year>2012</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The generalized Ornstein-Uhlenbeck process is derived from a bivariate L&#233;vy process and is suggested as a continuous time version of a stochastic recurrence equation [1]. In this paper we consider the generalized Ornstein-Uhlenbeck process and provide sufficient conditions under which the process is exponentially ergodic and hence holds the expo-nentially β-mixing property. Our results can cover a wide variety of areas by selecting suitable L&#233;vy processes and be used as fundamental tools for statistical analysis concerning the processes. Well known stochastic volatility models in finance such as L&#233;vy-driven Ornstein-Uhlenbeck process is examined as a special case.
 
</p></abstract><kwd-group><kwd>β-Mixing; Generalized Ornstein-Uhlenbeck Process; Exponential Ergodicity; L&#233;vy Driven       Ornstein-Uhlenbeck Process</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Many continuous time processes are suggested and studied as a natural continuous time generalization of a random recurrence equation, for example, diffusion model of Nelson [<xref ref-type="bibr" rid="scirp.17351-ref2">2</xref>], continuous time GARCH (COGARCH) (1,1) process of Kl&#252;ppelberg et al. [<xref ref-type="bibr" rid="scirp.17351-ref3">3</xref>] and L&#233;vy-driven Ornstein-Uhlenbeck (OU) process of Barndorff-Nielsen and Shephard [<xref ref-type="bibr" rid="scirp.17351-ref4">4</xref>] etc. Continuous time processes are particularly appropriate models for irregularly spaced and high frequency data [<xref ref-type="bibr" rid="scirp.17351-ref5">5</xref>]. We consider the generalized Ornstein-Uhlenbeck (GOU) process <img src="4-1500079\994b8794-4b37-43fb-bc87-3b425b18598d.jpg" /> which is defined by</p><disp-formula id="scirp.17351-formula91989"><label>(1)</label><graphic position="anchor" xlink:href="4-1500079\2ce5c078-8a0f-4fb1-9a98-8edcba86cdf4.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="4-1500079\c0b9a0a2-13f4-4968-b8c6-8fa910d68668.jpg" /> is a two-dimensional L&#233;vy process and the starting random variable <img src="4-1500079\d6c8ba32-6e8f-4e0e-9b67-ee012220f289.jpg" /> is independent of<img src="4-1500079\c1a7da6c-f398-4682-b1d2-4de690ff9123.jpg" />. L&#233;vy processes are a class of continuous time processes with independent and stationary increments and continuous in probability. Since L&#233;vy processes <img src="4-1500079\b32365d8-569f-47c1-886a-b03e713ba3c0.jpg" /> and <img src="4-1500079\262daeb5-241e-464e-9e1b-2c7486c6a92c.jpg" /> are semimartingales, stochastic integral in Equation (1) is well defined.</p><p>The GOU process is a continuous time version of a stochastic recurrence equation derived from a bivariate L&#233;vy process (de Haan and Karandikar [<xref ref-type="bibr" rid="scirp.17351-ref1">1</xref>]). The GOU process has recently attracted attention, especially in the financial modelling area such as option pricing, insurance and perpetuities, or risk theory. Stationarity, moment condition and autocovariance function of the GOU process are studied in Lindner and Maller [<xref ref-type="bibr" rid="scirp.17351-ref6">6</xref>]. Fasen [<xref ref-type="bibr" rid="scirp.17351-ref7">7</xref>] obtain the results for asymptotic behavior of extremes and sample autocovariance function of the GOU process. For related results, we may consult, e.g. Masuda [<xref ref-type="bibr" rid="scirp.17351-ref8">8</xref>], Kl&#252;ppelberg et al. [3,9], Maller et al. [<xref ref-type="bibr" rid="scirp.17351-ref5">5</xref>] and Lindner [<xref ref-type="bibr" rid="scirp.17351-ref10">10</xref>] etc.</p><p>Mixing property of a stochastic process describes the temporal dependence in data and is used to prove consistency and asymptotic normality of estimators. For a stationary process <img src="4-1500079\77c2af84-5fb6-4725-88f6-584633f4e416.jpg" /> and<img src="4-1500079\57fff4b6-74bf-4d5e-abfd-08ab1170eb3d.jpg" />, let</p><p><img src="4-1500079\2e58b245-8685-453b-a5c0-79deb48c5088.jpg" /></p><p>where the supremum takes over <img src="4-1500079\1f381d2d-1ff9-4781-9c27-5e6837042232.jpg" /></p><p><img src="4-1500079\74407984-b2be-4592-8e3e-00131c47818b.jpg" /></p><p>if <img src="4-1500079\bfa11f94-18b1-4e52-a8a9-0834dfaaa45b.jpg" /> and<img src="4-1500079\0f9ea162-1877-4ae5-a3ee-f86f1f04334b.jpg" />. If <img src="4-1500079\80b19dc8-5b15-4e30-a55f-bbc805d3d144.jpg" /> as<img src="4-1500079\ca8033bb-bee7-47ad-8087-6bbafe65f8bc.jpg" />, then <img src="4-1500079\6faf9197-8e32-42fe-98a9-ac3072157a28.jpg" /> is called β-mixing. <img src="4-1500079\a0f80bff-17a6-4999-bd10-bd78770d67f8.jpg" />is called exponentially β-mixing if <img src="4-1500079\7573cac2-9fda-48b8-8fda-26cfb9e630b0.jpg" /> for some <img src="4-1500079\079f2cee-511b-4c0f-bbc2-0e4f51fcb41b.jpg" /> and all<img src="4-1500079\f7ccf75a-dad2-47e9-b7e5-4d1ba4b51f4a.jpg" />.</p><p>In this paper we prove the exponential ergodicity and exponentially β-mixing property of the GOU process</p><p><img src="4-1500079\e15dae03-3b30-4f03-ab13-438ad668b4c2.jpg" />of Equation (1) and obtain the β-mixing property of the L&#233;vy-driven OU process as a special case.</p><p>For more information on Markov chain theory, we refer to Meyn and Tweedie [<xref ref-type="bibr" rid="scirp.17351-ref11">11</xref>]. We refer to Bertoin [<xref ref-type="bibr" rid="scirp.17351-ref12">12</xref>] and Sato [<xref ref-type="bibr" rid="scirp.17351-ref13">13</xref>] for basic results and representations concerning L&#233;vy processes.</p></sec><sec id="s2"><title>2. Exponential Ergodicity of <img src="4-1500079\a2cc5eda-fe6e-4acb-9c80-990f7d714552.jpg" /></title><sec id="s2_1"><title>2.1. The Model</title><p>A bivariate L&#233;vy process <img src="4-1500079\5ec52116-82b4-4bec-8291-3878b92fb585.jpg" /> defined on a complete probability space <img src="4-1500079\3ead96a8-b20a-4c31-9c98-07d05a48d446.jpg" /> is a stochastic process in<img src="4-1500079\d2c16601-5a98-4843-ae72-bf09ce975867.jpg" />, with c&#224;dl&#224;g paths, <img src="4-1500079\09499b14-5d5a-4173-a69e-9ada5b5ec2ce.jpg" />and stationary independent increments, which is continuous in probability.</p><p>Consider the GOU process <img src="4-1500079\be550942-b65a-4637-8398-a8923199d3c7.jpg" /> given by</p><p><img src="4-1500079\aef26cb3-1f7f-4ee2-975a-08d0b696e954.jpg" /></p><p>Assume that <img src="4-1500079\8311eec8-ae2c-4edd-b466-c573786370ae.jpg" /> is independent of<img src="4-1500079\a6b9c197-fec8-429e-b2d3-a11e66fc5c63.jpg" />. Let</p><disp-formula id="scirp.17351-formula91990"><label>(2)</label><graphic position="anchor" xlink:href="4-1500079\bb2c3d60-99aa-4188-81f0-50aa03b9dbd0.jpg"  xlink:type="simple"/></disp-formula><p>Then we have that</p><disp-formula id="scirp.17351-formula91991"><label>(3)</label><graphic position="anchor" xlink:href="4-1500079\9c250528-fed8-4605-ac38-175f39264b0a.jpg"  xlink:type="simple"/></disp-formula><p>Let n denote an integer and <img src="4-1500079\0c6c3e49-5020-45d8-8a05-5ac568acbf4e.jpg" /> a real number. We can easily show that <img src="4-1500079\ff58a528-beec-4d0a-9b83-4f6d0637d0ea.jpg" />in Equation (2) is a sequence of independent and identically distributed random vectors and <img src="4-1500079\589d5433-d509-4e9d-a60b-26f34e18fdb4.jpg" /> in Equation (1) is a time homogeneous Markov process with t-step transition probability function</p><p><img src="4-1500079\a0aafb64-9c26-42fc-94b5-b811579fa242.jpg" /></p><p>where <img src="4-1500079\b5d3990f-94cf-460a-8623-2ad4a6a48723.jpg" /> is a Borel σ-field of subsets of real numbers R.</p><p>We temporally assume that <img src="4-1500079\945a1024-d239-41cf-8b34-a22c35660035.jpg" /> is fixed. <img src="4-1500079\e06ed648-6ff4-402b-aec7-685bb1c3069e.jpg" />in Equation (3) can be considered as a discrete time Markov process with n-step transition probability function<img src="4-1500079\fe8c1dd2-de2b-4a46-bcae-03d1c1c2f591.jpg" />. <img src="4-1500079\2e8ae22a-b3b1-4d30-bd09-6ed028f3b222.jpg" />is called the h-skeleton chain of<img src="4-1500079\fef8b1a7-0491-4d4a-af9a-e666ad444caf.jpg" />. A Markov process <img src="4-1500079\f4d3b0b3-56d7-439e-8298-b344283a7d49.jpg" /> is <img src="4-1500079\c79d419e-d146-4f08-9f93-61ad586db948.jpg" />-irreducible if, for some <img src="4-1500079\c833e96a-a9c3-4570-adfb-6fd0fcf574c7.jpg" />-finite measure<img src="4-1500079\04855f01-5c67-4ce6-bee8-e5dbee670326.jpg" />, <img src="4-1500079\6bdb7d33-c1b9-48c2-9e0f-fbac959d7c8b.jpg" />for all <img src="4-1500079\20165b7b-fb5d-4d64-8060-bf5d50d0d0f9.jpg" /> whenever<img src="4-1500079\7aacfbf4-3efa-4ee8-b493-7b5efc812ce2.jpg" />. <img src="4-1500079\229f839c-aecd-4e6c-8c39-bc86bdafb974.jpg" />is said to be simultaneously <img src="4-1500079\0cc0c38b-0125-4760-a2d1-654047c5e2dd.jpg" />-irreducible if any h-skeleton chain is <img src="4-1500079\76d66863-086a-42b8-b32c-f7d15505a28e.jpg" />-irreducible. It is known that if <img src="4-1500079\dd3dbc26-3311-4fbf-a7af-4626e8042613.jpg" /> is simultaneously <img src="4-1500079\3bf0549d-50e2-4b9c-9526-a6393580e068.jpg" />-irreducible, then any h-skeleton chain is aperiodic (Proposition 1.2 of Tuominen and Tweedie [<xref ref-type="bibr" rid="scirp.17351-ref14">14</xref>]).</p><p>For fixed<img src="4-1500079\ab2e1803-81a0-4392-a4d7-475bd28dc6b4.jpg" />, we make the following assumptions:</p><p>(A1) <img src="4-1500079\f934a77e-2d9b-4d1d-ad2b-4393bb298f49.jpg" />and<img src="4-1500079\e3403b0b-2b36-49db-8717-4d55e3e5d182.jpg" />.</p><p>(A2) <img src="4-1500079\d5e14cf9-1a90-435c-a13d-2d15a3145682.jpg" />for some <img src="4-1500079\cc034f44-4f4f-4795-94cb-c38cb1e42b1d.jpg" /></p><p>Theorem 2.1 Under the assumption (A1), <img src="4-1500079\b9e16711-6801-4ac8-9071-c86de62aea7c.jpg" />defined by Equation (3) converges in distribution to a probability measure <img src="4-1500079\3e6bc18b-0786-4938-ac9b-1082f435dbbe.jpg" /> which does not depend on<img src="4-1500079\b69a5466-4b43-45ca-ab7a-f7ca1e0aa0b6.jpg" />. Further, <img src="4-1500079\f6dc2e6b-bfdd-42b3-a898-4b4bbda22276.jpg" />is the unique invariant initial distribution for<img src="4-1500079\ff881a45-d923-4ad6-81e9-9699f28f2b3c.jpg" />.</p><p>Proof. The conclusion follows from Theorem 3.1 and Theorem 3.4 in de Haan and Karandikar [<xref ref-type="bibr" rid="scirp.17351-ref1">1</xref>]. Note that if the assumption (A1) holds, then it is obtained that</p><p><img src="4-1500079\6c12f5c0-5ef3-4141-923b-f81a13caab24.jpg" />and<img src="4-1500079\f90ab32d-280d-4dff-967e-8f3012ca04c1.jpg" />.<img src="4-1500079\62d73b17-7337-4e56-a747-8897328852a8.jpg" /></p><p>Remark 1 Assume that<img src="4-1500079\3e8bb9e2-9bd0-4cb4-b741-b015fe8b4365.jpg" />. Then <img src="4-1500079\e5f72590-ab17-40ad-9d96-8438a5d86c41.jpg" /> is also necessary for the existence of a strictly stationary solution. (See Theorem 2.1 in Lindner and Maller [<xref ref-type="bibr" rid="scirp.17351-ref6">6</xref>].)</p><p>Remark 2 Suppose that there exist <img src="4-1500079\cdc23e35-a30d-4a7d-a813-834729d643b5.jpg" /> and <img src="4-1500079\d65956b3-e0b6-4f2a-a668-b22984282774.jpg" /> with <img src="4-1500079\99d4011f-b69c-47ff-a541-6be1a69770c4.jpg" /> such that</p><p><img src="4-1500079\bc0c49e8-fa3d-4753-856c-da26901e4609.jpg" /></p><p>where <img src="4-1500079\a51e55c2-73fb-4d1a-96c3-d3d61e5d32c9.jpg" /> denotes the L&#233;vy exponent of the L&#233;vy process<img src="4-1500079\e727defc-9746-4e1b-9662-daab2475ba0d.jpg" />: <img src="4-1500079\72fe850a-8e11-4b54-9f67-4bc7390d460c.jpg" />If in addition, <img src="4-1500079\ff8fd0da-e2db-4011-bd76-38d84511d593.jpg" />then assumptions (A1) and (A2) hold (Proposition 4.1 in Lindner and Maller [<xref ref-type="bibr" rid="scirp.17351-ref6">6</xref>]).</p></sec><sec id="s2_2"><title>2.2. Drift Condition for <img src="4-1500079\5a96cb80-63ec-470d-9c36-b6f6c1518357.jpg" /></title><p>A discrete time Markov process <img src="4-1500079\6f46ceac-8239-4d50-9eb2-f958b2fb4cdd.jpg" /> is said to hold the drift condition if there exist a positive function g on R, a compact set K, and constants <img src="4-1500079\e1fcc458-4216-4e38-bc41-5bcf4a8142c2.jpg" /> and <img src="4-1500079\e7cead50-5303-408c-bb70-3b5a939b6daa.jpg" /> such that</p><p><img src="4-1500079\e1c81df7-61a4-472d-95d6-e900b790ffb5.jpg" /></p><p>and &#160;&#160;&#160;&#160;&#160;&#160;&#160;&#160;<img src="4-1500079\8240ce04-58d5-413c-a3d1-189d3b2deea2.jpg" /></p><p>Theorem 2.2 Under the assumptions (A1) and (A2), <img src="4-1500079\92dd99fb-6c3f-405e-beec-0d81a65c3bb8.jpg" />given in Equation (3) satisfies the drift condition.</p><p>Proof. For notational simplicity, let<img src="4-1500079\0d8afa30-bb79-400a-b213-71e672d4a4be.jpg" />. From assumptions, we have that <img src="4-1500079\655e60d7-a501-4ed3-9783-f51a354e2532.jpg" /> and <img src="4-1500079\8bc59426-81d4-46a9-a5ed-7aa6b0097d80.jpg" /> for some<img src="4-1500079\14761d02-1e23-4d68-bbc3-83633d147fa1.jpg" />. Then</p><p><img src="4-1500079\7da92b74-6bee-4616-aa88-76375f4786ee.jpg" /></p><p>as <img src="4-1500079\6b26a90f-b5bd-492a-a6d2-e3365a9a4ce6.jpg" /> ( Hardy et al. [<xref ref-type="bibr" rid="scirp.17351-ref15">15</xref>]). Here <img src="4-1500079\13ba59aa-8885-4ba0-94cf-875246c961ef.jpg" /> implies the existence of<img src="4-1500079\f52b54e4-8c74-47f2-a9b2-caf9c21584f5.jpg" />, <img src="4-1500079\178ca271-50d7-4bc5-bd80-0bd66b280a99.jpg" />such that<img src="4-1500079\02373e4f-9d11-432f-82b8-673df34632f5.jpg" />. Now define a nonnegative test function g on R by<img src="4-1500079\1223be0c-30df-470a-9f14-9bbac1ddf074.jpg" />. Then we have that</p><disp-formula id="scirp.17351-formula91992"><label>(4)</label><graphic position="anchor" xlink:href="4-1500079\3f6d11a1-a035-4624-90c8-5481a27678a1.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="4-1500079\65e26bc4-650f-41b8-b946-6c038a9071e7.jpg" />, by assumption (A2). Since <img src="4-1500079\c0598fc4-0549-4b49-8a45-bda9cc5d46ad.jpg" /> increases to <img src="4-1500079\a0171442-3e25-4737-890b-b5e1b2d5b41c.jpg" /> as <img src="4-1500079\2a1efa11-a2d1-4ddd-9405-b86d2507c512.jpg" /> increases to<img src="4-1500079\e5268a2e-4089-436d-9672-672ff1240196.jpg" />, for any<img src="4-1500079\b1770539-965b-4d5f-b3cc-ef75400be0e2.jpg" />, there exist <img src="4-1500079\a0755b81-9ae2-429c-985a-608de96438a8.jpg" /> and <img src="4-1500079\22a294a6-f3dd-44d2-918f-65fd955bd941.jpg" /> with<img src="4-1500079\c32f4c08-893b-4b81-bfd1-1d1a51a9b654.jpg" />, such that</p><disp-formula id="scirp.17351-formula91993"><label>(5)</label><graphic position="anchor" xlink:href="4-1500079\48c8caf7-bd0d-4688-ab27-7cebabb338b7.jpg"  xlink:type="simple"/></disp-formula><p>Clearly,</p><disp-formula id="scirp.17351-formula91994"><label>(6)</label><graphic position="anchor" xlink:href="4-1500079\74969856-163a-4609-94df-5b6756ca07da.jpg"  xlink:type="simple"/></disp-formula><p>Combining Equations (4)-(6), the drift condition for <img src="4-1500079\d36479b1-594b-43fc-ab1a-372dc9312e01.jpg" /> holds.<img src="4-1500079\905e4273-35eb-4e8a-bac4-d3d410747aa2.jpg" /></p></sec><sec id="s2_3"><title>2.3. Simultaneous <img src="4-1500079\14d6f68c-acf5-4ef2-b2a6-90e8e1b4ba53.jpg" />-Irreducibility of <img src="4-1500079\6c1fa377-03ad-4e93-9f5c-53bcf7f9567f.jpg" /></title><p>For reader’s convenience, we state the following theorems which play important roles to prove our main results.</p><p>Theorem 2.3 (Meyn and Tweedie [<xref ref-type="bibr" rid="scirp.17351-ref11">11</xref>]) Suppose that a Markov chain <img src="4-1500079\74beed70-6c67-4c48-b6da-be4201d740c0.jpg" /> has the Feller property. If <img src="4-1500079\7dca4238-f3ed-4c5d-883f-3d1491d44619.jpg" /> satisfies the drift condition for a compact set</p><p><img src="4-1500079\4664c6b8-e29e-4cac-a7c8-e021e6dc0180.jpg" />, then there exists an invariant probability measure. In addition, if the process is <img src="4-1500079\dcc1eae2-365c-4ad1-b3a1-26341cd552cb.jpg" />-irreducible and aperiodic, then the given process is geometrically ergodic.</p><p>Theorem 2.3 shows that the crucial step to prove the geometric ergodicity of a Markov process is to show that the given process is <img src="4-1500079\def70e48-ae57-417c-b0b1-0742986b610a.jpg" />-irreducible and holds the drift condition. In many cases, however, proving irreducibility of a Markov process is an awkward task. Consulting the following Theorem 2.4, irreducibility of the process can be derived from connection between <img src="4-1500079\208d8bca-d2e7-4bc3-a680-6c2147c1a79f.jpg" />-irreducibility and the uniform countable additivity condition. A Markov chain <img src="4-1500079\53fae8d6-7bb6-450f-944d-d7efa8021589.jpg" /> is said to hold the uniform countable additivity condition (Liu and Susko [<xref ref-type="bibr" rid="scirp.17351-ref16">16</xref>]) if its one-step transition probability function satisfies that for any decreasing sequence <img src="4-1500079\4c77897d-259a-4ee6-8b8a-117e0872841f.jpg" /> inside compact sets,</p><p><img src="4-1500079\ab04eb4a-a495-4aa7-8e2d-5a6c9793cb71.jpg" /></p><p>Theorem 2.4 (Tweedie [<xref ref-type="bibr" rid="scirp.17351-ref17">17</xref>]) Suppose that the drift condition holds with a test set K and the uniform countable additivity condition holds for the same set K. Then there is a unique invariant measure for <img src="4-1500079\14d764dd-76c1-4af7-96a6-6f79939739d5.jpg" /> if and only if <img src="4-1500079\761112f4-3a7e-44e8-907c-ee4fbbfb673c.jpg" /> is <img src="4-1500079\06c1f373-4116-4655-b4cd-27189e4bda9f.jpg" />-irreducible.</p><p>Let <img src="4-1500079\13982836-b98c-4457-a91b-285846edd737.jpg" /> be the compact set defined in the proof of Theorem 2.2.</p><p>Theorem 2.5 Under the assumptions (A1) and (A2), <img src="4-1500079\1f01cbe1-1dba-4fb1-a1ab-4f3f2db742f7.jpg" />is simultaneously π-irreducible if for any<img src="4-1500079\93d8e930-3d44-40f9-b621-3baff4b66fb7.jpg" />,</p><p><img src="4-1500079\6990b53c-bae5-4743-bd46-e090fa303df4.jpg" />has a probability density function <img src="4-1500079\b3a1dac3-90f5-403e-8a12-5b163c9079b5.jpg" /></p><p>(with respect to the Lebesgue measure<img src="4-1500079\dd8e2e56-5f98-4a66-82ad-4da71058c407.jpg" />), which is uniformly bounded on compacts for<img src="4-1500079\34b2e178-1e68-4f44-b9bc-777ce14f18bf.jpg" />.</p><p>Proof. Let <img src="4-1500079\bdb3c034-6ab8-4308-a679-7a28ba725868.jpg" /> be any decreasing sequence inside compact sets with<img src="4-1500079\d838cef8-c491-4ec3-8721-9acf8eae4e4d.jpg" />. Then</p><disp-formula id="scirp.17351-formula91995"><label>(7)</label><graphic position="anchor" xlink:href="4-1500079\945ef172-7ff4-4d56-bd30-27e6d608e950.jpg"  xlink:type="simple"/></disp-formula><p>where &#160;&#160;<img src="4-1500079\d8a2448c-bbfe-4649-b35b-40b3c3f68c82.jpg" />.</p><p>The inequality in Equation (7) and the condition that <img src="4-1500079\1d737e6b-4cd9-41ed-afe2-c7ce5c48d67c.jpg" /> is any sequence inside compact sets in <img src="4-1500079\8d343070-dc8d-43c5-80c5-97c49a528fdc.jpg" /> with <img src="4-1500079\61ac2f3d-5b7a-437e-98e0-e4317ba0af1f.jpg" /> imply that</p><p><img src="4-1500079\649158ed-a40b-4cf6-a6d2-94542f6a94a9.jpg" />.</p><p>Therefore the uniform countable additivity condition holds for the compact set K. Theorem 2.4 and the existence of a unique invariant initial distribution for</p><p><img src="4-1500079\3d8d6b2f-a3fb-445b-bbd0-200bb54c405a.jpg" />yield the <img src="4-1500079\aeb09514-6799-4645-b7ad-27477b9811fb.jpg" />-irreducibility of any h-skeleton chain<img src="4-1500079\0d4da8ab-c353-4a1f-8958-9f2e947f486e.jpg" />.</p><p>To complete the proof, we need to show that the assumption (A1) and (A2) hold for all<img src="4-1500079\c40ec57e-aef0-4957-afc5-4d58737e2f12.jpg" />. Since L&#233;vy processes have stationary and independent increments, it is easy to show that the assumption (A1) and <img src="4-1500079\c74f2e08-76ed-4a38-9593-77b1159cc974.jpg" /></p><p>hold for all<img src="4-1500079\25ff6def-d9ae-427f-8f63-90187cb1ac4d.jpg" />. It remains to prove that</p><p><img src="4-1500079\6d155232-f2a6-4af3-9163-814bfd0281cf.jpg" /></p><p>for all <img src="4-1500079\33ba2076-b13f-4974-8505-94c19911f7bc.jpg" /> with some<img src="4-1500079\7f6d50b0-ff75-4a4c-88ae-f3c8031ca9c2.jpg" />. We first define a finite L&#233;vy process <img src="4-1500079\739ed80c-3d1a-44d9-9cb0-d7a40b265d20.jpg" /> as follows:</p><p><img src="4-1500079\9be38ff1-632b-4902-97c3-e63a35122a6a.jpg" /></p><p>Then it is shown that<img src="4-1500079\628eb8d3-a5eb-45ff-a5c6-955b02cf1fa2.jpg" />,</p><p><img src="4-1500079\709b8564-392e-481a-9a0b-52fd4ad6b433.jpg" /></p><p>(See Proposition 2.3 in Lindner and Maller [<xref ref-type="bibr" rid="scirp.17351-ref6">6</xref>]). Without loss of generality, we may assume that<img src="4-1500079\10c2d1ba-0380-4bed-8585-f70d70b0ac7a.jpg" />. Choose any<img src="4-1500079\7613cffb-147a-463b-a062-7e7881663144.jpg" />. Then<img src="4-1500079\da583a66-60bc-4923-b242-f307972ca649.jpg" />, where n is a nonnegative integer, <img src="4-1500079\e3e62373-ba8a-426b-95c0-28df333c8b3d.jpg" />and <img src="4-1500079\52378d12-8085-45cb-a59e-6095862fd2e0.jpg" /> is in the assumptions (A1) and (A2), we have that</p><disp-formula id="scirp.17351-formula91996"><label>(8)</label><graphic position="anchor" xlink:href="4-1500079\09f587e6-c4d6-4827-bb6b-a635f4a44ead.jpg"  xlink:type="simple"/></disp-formula><p>The first inequality in Equation (8) follows from stationary and independent increments property of L&#233;vy processes <img src="4-1500079\ce265091-24bf-4d2c-8591-ab178953f35d.jpg" /> and<img src="4-1500079\854645a9-4a45-4f4e-a0de-8bd2aca9a538.jpg" />.</p><p>Therefore for any<img src="4-1500079\58653c02-adf5-4868-9980-8cbdea1168aa.jpg" />, h-skeleton chain <img src="4-1500079\5f6a58bb-869c-446d-bb82-44f4cdd0477c.jpg" /> is <img src="4-1500079\d7a925b7-7bfc-405d-b573-874dbac9652c.jpg" />-irreducible and hence <img src="4-1500079\2b62f715-8a19-4780-be76-9b8a9a115708.jpg" /> is simultaneously <img src="4-1500079\7fccef54-74a5-420a-b45d-88960730c9cf.jpg" />-irreducible and <img src="4-1500079\4946b80b-5661-4421-a037-f72a5b6e2af3.jpg" /> is aperiodic.</p></sec><sec id="s2_4"><title>2.4. Exponential Ergodicity of <img src="4-1500079\32ee6c72-75d4-4b5c-9d7f-6ff1d18affcb.jpg" /></title><p>The next theorem is our main result.</p><p>Theorem 2.6 Suppose that the assumptions of Theorem 2.5 hold. Then the GOU process <img src="4-1500079\1cebbfa8-4ddd-4d9c-8a6f-ab62ed886b46.jpg" /> in Equation (1) is exponentially ergodic and holds the exponentially <img src="4-1500079\43bed62f-6cfa-430f-b637-16c86083a93f.jpg" />-mixing property.</p><p>Proof. Theorem 2.5 shows that any h-skeleton chain</p><p><img src="4-1500079\70a4fdd0-6e19-4740-bad2-f2b97faea3aa.jpg" />is <img src="4-1500079\e087e51d-15e4-4ea6-8f2a-cdee06326b18.jpg" />-irreducible and aperiodic. Note that <img src="4-1500079\893cccc1-df0c-4fa0-a4c8-1af8eb45d8c9.jpg" /> is a Feller chain, that is, <img src="4-1500079\2cac8a6b-6499-4af8-9c5a-4485d5a5da45.jpg" /></p><p>is a continuous function of x whenever f is continuous and bounded. Therefore any nontrivial compact set is a small set. Theorem 2.2 ensures that <img src="4-1500079\24720faa-2877-4b94-ab5a-748e0830eb54.jpg" /> holds the drift condition and hence Theorem 2.5 and Theorem 2.3 imply that <img src="4-1500079\d79241a5-750e-4e1e-b4b7-25be53564c35.jpg" /> is geometrically ergodic, that is, there exists a constant <img src="4-1500079\0951d0d7-ab7d-4f82-b5d1-bd83207fb516.jpg" /> such that</p><disp-formula id="scirp.17351-formula91997"><label>(9)</label><graphic position="anchor" xlink:href="4-1500079\0f665c7f-b3b7-487c-bb29-50bd7e5474d4.jpg"  xlink:type="simple"/></disp-formula><p><img src="4-1500079\52312154-c873-4183-888e-040b247077ae.jpg" />-a.a. x as<img src="4-1500079\93f9d176-7368-49cd-ac57-eaf320d2d01d.jpg" />, where <img src="4-1500079\8e63b51a-4ddb-48aa-afa7-52ca90396cf5.jpg" /> denotes the total variation norm. Under simultaneous <img src="4-1500079\ee8f73f8-64cb-46ac-bd8a-25859fefd6e5.jpg" />-irreducibility condition of<img src="4-1500079\08963c2b-ead6-4ff7-b2c8-ebb23bbe1231.jpg" />, Equation (9) and Theorem 5 in Tuominen and Tweedie [<xref ref-type="bibr" rid="scirp.17351-ref14">14</xref>] guarantee the exponential ergodicity of <img src="4-1500079\88e8a7c5-4042-4b4e-ae57-0efddadc8711.jpg" /> in the following sense:</p><p><img src="4-1500079\69136178-f39a-4738-8b9e-c5d3282cfed3.jpg" /></p><p>as<img src="4-1500079\e2021141-1c15-4640-837a-7ec536ba2a6c.jpg" />, for some <img src="4-1500079\bcdc46f9-d46a-4b00-b225-e6442cf6fed2.jpg" /> and <img src="4-1500079\82980e0b-f30b-4f28-b986-34348b662c95.jpg" />-a.a. x. <img src="4-1500079\41e8e1c5-c9b7-41ed-a5bd-1f5c8ce095ee.jpg" />-mixing property for the continuous time GOU process <img src="4-1500079\0391f97e-c4c0-4eb7-a594-a36edc4900e7.jpg" /> is also obtained.</p></sec><sec id="s2_5"><title>2.5. Examples</title><p>In this example, we assume that<img src="4-1500079\7bf4d42a-1017-442e-a391-3d3836ffd49e.jpg" />. If <img src="4-1500079\aa100eb3-6f02-46e0-bd77-b9854d704009.jpg" /> is any L&#233;vy process, then <img src="4-1500079\5748fb44-c03d-4c3f-bc2e-2d3c2124cdd0.jpg" /> in Equation (1) is the L&#233;vydriven OU process which is studied by Barndorff-Nielsen and Shephard [<xref ref-type="bibr" rid="scirp.17351-ref4">4</xref>]. In particular, if <img src="4-1500079\efea9f11-c38f-417b-91f1-9fc159836eda.jpg" /> is a subordinator, that is, <img src="4-1500079\3e774501-a95e-4b8d-852b-96421ac4cae9.jpg" />has nondecreasing sample path, finite variation with nonnegative drift and L&#233;vy measure concentrated on<img src="4-1500079\f9232fe1-b774-42b2-9aa9-e1f42227dd4b.jpg" />, then <img src="4-1500079\559502ee-2306-4eca-a2ab-b2da6289bdf9.jpg" /> is called the L&#233;vy-driven stochastic volatility model. For the case that <img src="4-1500079\3e15ed14-f507-4a90-8043-77db617c2657.jpg" /> is a Brownian motion, <img src="4-1500079\947f81dd-93a2-4c39-bf95-ca9aab4ff3a7.jpg" />is the classical OU process. Let <img src="4-1500079\51951a25-afa3-46bd-b738-9cedfdb8918c.jpg" /> be the L&#233;vy measure for the process <img src="4-1500079\05d5e50a-5950-47c2-82c9-d34e6e421e64.jpg" /> and assume that <img src="4-1500079\45e10241-eab1-4cc5-b218-4ce80b8e3788.jpg" /> for some <img src="4-1500079\68d57f99-245f-4507-bb2c-1fed7701fb20.jpg" /> and<img src="4-1500079\f5fe2c6f-8c65-448b-9209-c6b198e2c237.jpg" />.</p><p>Then<img src="4-1500079\9f03fc3f-790f-48ca-8bf1-b3874747eaa8.jpg" />. Here we can easily show that the assumptions (A1)and (A2) hold. Theorem 2.2 implies that <img src="4-1500079\0cb41c2a-4090-4cd4-a871-f97c1363dc80.jpg" /> holds the drift condition. Moreover, it is known that <img src="4-1500079\02088ffa-4737-45a8-80af-67e3949ed3f3.jpg" /> admits a <img src="4-1500079\d1f2319e-6888-4790-b9da-9d31068b67f8.jpg" /> density <img src="4-1500079\d0c187c0-fe4c-45f6-a514-8469d96e2e9a.jpg" /> for each <img src="4-1500079\78face0d-c904-49c6-8ce6-369b1b6b20ae.jpg" /> (Sato and Yamazato [<xref ref-type="bibr" rid="scirp.17351-ref18">18</xref>]) and by Theorem 2.5, <img src="4-1500079\015b4340-4d99-4344-916f-4d6cbd587284.jpg" />is <img src="4-1500079\103e6596-0157-41fd-a383-007abaf07ef6.jpg" />-irreducible. Above statements hold for any <img src="4-1500079\b881d890-1f92-4324-ae9b-153b313d5fd1.jpg" /> and hence <img src="4-1500079\733b7a23-7707-449e-b298-d5d6d263f983.jpg" /> is simultaneously <img src="4-1500079\94952f9d-4e6b-436a-9acd-63ae47de9151.jpg" />-irreducible. Therefore exponential ergodicity and exponential <img src="4-1500079\78b13631-973d-4a8e-b8ca-4d84b1461dae.jpg" />-mixing property of <img src="4-1500079\88915e17-216f-4979-8914-f28cf99dd9fb.jpg" /> follow from Theorem 2.6.</p></sec></sec><sec id="s3"><title>3. Conclusion</title><p>Recently, time series models in finance and econometrics are suggested as continuous time models which are particularly appropriate for irregularly spaced and high frequency data. The GOU process is a continuous time stochastic process driven by a bivariate L&#233;vy process. The stationarity, moment conditions, autocovariance function and asymptotic behavior of extremes of the process are studied in [6,7], but exponential ergodicity does not seem to have been investigated as yet. In this paper, we give sufficient conditions under which the process is exponentially ergodic and <img src="4-1500079\f5b9e786-587b-47ce-8876-caba07a7ef36.jpg" />-mixing. The drift condition and the simultaneous <img src="4-1500079\a4dd24d5-230a-4f4d-b014-5347efac68c4.jpg" />-irreducibility of the process that is induced from uniform countable additivity condition play a crucial role to prove the results. Our results are used to show, in particular, consistency and asymptotic normality of estimators.</p></sec><sec id="s4"><title>4. Acknowledgements</title><p>This research was supported by KRF grant 2010- 0015707.</p></sec><sec id="s5"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.17351-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">L. de Haan and R. L. Karandikar, “Embedding a Stochastic Difference Equation in a Continuous Time Process,” Stochastic Processes and Their Applications, Vol. 32, No. 2, 1989, pp. 225-235.  
doi:10.1016/0304-4149(89)90077-X</mixed-citation></ref><ref id="scirp.17351-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">D. B. Nelson, “ARCH Models as Diffusion Approximations,” Journal of Econometrics, Vol. 45, No. 1-2, 1990, pp. 7-38. doi:10.1016/0304-4076(90)90092-8</mixed-citation></ref><ref id="scirp.17351-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">C. Klüppelberg, A. Lindner and R. A. Maller, “A Continuous Time GARCH Process Driven by a Levy Process: Stationarity and Second Order Behavior,” Journal of Applied Probability, Vol. 41, No. 3, 2004, pp. 601-622.  
doi:10.1239/jap/1091543413</mixed-citation></ref><ref id="scirp.17351-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">O. E. Barndorff-Nielsen and N. Shephard, “Non-Gaussian Ornstein-Uhlenbeck Based Models and Some of Their Uses in Financial Economics (with dis-cussion),” Journal of Royal Statistical Society, Series B, Vol. 63, No. 2, 2001, pp. 167-241. doi:10.1111/1467-9868.00282</mixed-citation></ref><ref id="scirp.17351-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">R. A. Maller, G. Müller and A. Szimayer, “GARCH Modeling in Continuous Time for Irregularly Spaced Time Series Data,” Bernoulli, Vol. 14, No. 2, 2008, pp. 519-542. doi:10.3150/07-BEJ6189</mixed-citation></ref><ref id="scirp.17351-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">A. Lindner and R. A. Maller, “Levy Integrals and the Stationarity of Generalized Ornstein-Uhlenbeck Processes,” Stochastic Processes and Their Applications, Vol. 115, No. 10, 2005, pp. 1701-1722.  
doi:10.1016/j.spa.2005.05.004</mixed-citation></ref><ref id="scirp.17351-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">V. Fasen, “Asymptotic Results for Sample Auto-covariance Functions and Extremes of Integrated Generalized Ornstein-Uhlenbeck Processes,” 2010. 
http://www.ma.tum.de/stat/</mixed-citation></ref><ref id="scirp.17351-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">H. Masuda, “On Multidimen-sional Ornstein-Uhlenbeck Processes Driven by a General Levy Process,” Bernoulli, Vol. 10, No. 1, 2004, pp. 97-120.  
doi:10.3150/bj/1077544605</mixed-citation></ref><ref id="scirp.17351-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">C. Klüppelberg, A. Lindner and R. A. Maller, “Continuous Time Volatility Modeling: COGARCH versus Ornstein-Uhlenbeck Models,” In: Y. Ka-banov, R. Liptser, and J. Stoyanov, Eds., Stochastic Calculus to Mathematical Finance, The Shiryaev Festschrift, Springer, Berlin, 2006, pp. 393-419.  
doi:10.1007/978-3-540-30788-4_21</mixed-citation></ref><ref id="scirp.17351-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">A. Lindner, “Continuous Time Approximations to GARCH and Stochastic Volatility Models,” In: T. G. Andersen, R. A. Davis, J. P. Krei and T. Mikosch, Eds., Handbook of Financial Time Series, Springer, Berlin, 2010.</mixed-citation></ref><ref id="scirp.17351-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">S. P. Meyn and R. L. Tweedie, “Markov Chain and Stochastic Stability,” Springer-Verlag, Berlin, 1993.</mixed-citation></ref><ref id="scirp.17351-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">J. Bertoin, “Lévy Processes,” Cambridge University Press, Cambridge, 1996.</mixed-citation></ref><ref id="scirp.17351-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">K. Sato, “Levy Processes and Infinitely Divisible Distributions,” Cambridge University Press, Cambridge, 1999.</mixed-citation></ref><ref id="scirp.17351-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">P. Tuominen and R. L. Tweedie, “Exponential Decay and Ergodicity of General Markov Processes and Their Discrete Skeletons,” Advances in Applied Probability, Vol. 11, 1979, pp.784-803. doi:10.2307/1426859 </mixed-citation></ref><ref id="scirp.17351-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">G. H. Hardy, J. E. Littlewood and G. Pólya, “Inequalities,” Cambridge University Press, Cambridge, 1952.</mixed-citation></ref><ref id="scirp.17351-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">J. Liu and E. Susko, “On Strict Stationarity and Ergodicity of a Nonlinear ARMA Model,” Journal of Applied Probability, Vol. 29, 1992, pp. 363-373.  
doi:10.2307/3214573</mixed-citation></ref><ref id="scirp.17351-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">R. L. Tweedie, “Drift Conditions and Invariant Measures for Markov Chains,” Stochastic Processes and their Applications, Vol. 92, No. 2, 2001, pp. 345-354.  
doi:10.1016/S0304-4149(00)00085-5</mixed-citation></ref><ref id="scirp.17351-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">K. Sato and M. Yamazato, “Operator-self Decomposable Distributions as Limit Distributions of Processes of Ornstein-Uhlenbeck Type,” Stochastic Processes and Their Applications, Vol. 17, No. 1, 1984, pp. 73-100.  
doi:10.1016/0304-4149(84)90312-0</mixed-citation></ref></ref-list></back></article>