<?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">JSS</journal-id><journal-title-group><journal-title>Open Journal of Social Sciences</journal-title></journal-title-group><issn pub-type="epub">2327-5952</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jss.2016.45010</article-id><article-id pub-id-type="publisher-id">JSS-66850</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><subject> Social Sciences&amp;Humanities</subject></subj-group></article-categories><title-group><article-title>
 
 
  Comovement of Stock Markets—An Analysis by Nonlinear Cointegration*
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kazumi</surname><given-names>Asako</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zhentao</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Institute for Financial and Accounting Studies, Xiamen University, Xiamen, China</addr-line></aff><aff id="aff1"><addr-line>Faculty of Economics, Rissho University, Tokyo, Japan</addr-line></aff><pub-date pub-type="epub"><day>31</day><month>05</month><year>2016</year></pub-date><volume>04</volume><issue>05</issue><fpage>64</fpage><lpage>75</lpage><history><date date-type="received"><day>19</day>	<month>April</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>13</month>	<year>May</year>	</date><date date-type="accepted"><day>16</day>	<month>May</month>	<year>2016</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>
 
 
   This paper proposes and estimates a statistical model of nonlinear cointegration, with applications to the stock markets of Japan and the United States. We define nonlinear cointegration as a long-run stable relationship between two time series variables even in the presence of temporary nonlinear divergence from this long-run relationship. More concretely, extending the bubble model of Asako and Liu (2013) [1] to stock price ratio variables, both upward and downward divergent bubble processes are estimated at a time. We conclude that, although two stock price indexes are not linearly cointegrated, they are considered to be cointegrated nonlinearly. 
 
</p></abstract><kwd-group><kwd>Booms and Busts</kwd><kwd> Stock Prices</kwd><kwd> Nonlinear Cointegration</kwd><kwd> Bayesian Estimation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In this paper we propose and develop the recursive estimation method of a nonlinear statistical model of speculative bubbles and utilize this model in establishing an idea of nonlinear cointegration. We then apply this idea to the stock market indexes of Japan and the United States, and we detect how these indexes commove in the long run although they deviate from the long-run relationship nonlinearly in the short run.</p><p>So far, whether stock markets of different countries commove together has mainly been tested by utilizing the linear cointegration relationship &#224; la Engle and Granger (1987) [<xref ref-type="bibr" rid="scirp.66850-ref2">2</xref>]. We owe the main idea of cointegration to this line of research. However, what we propose in this paper is a statistical model that incorporates latent cointegration relationship not linearly but nonlinearly. The nonlinearity here stems from the consideration of booms and busts in stock price indexes (and thereby the ratio of indexes of different markets). When bubbles are born and boom for certain periods only to crash in due course, time series of these events are hardly captured by linear models.</p><p>As empirical investigation of comovement of stock markets, there have been a number of research and the results vary depending on the countries and sample periods. Asako, Zhang and Liu (2014) [<xref ref-type="bibr" rid="scirp.66850-ref3">3</xref>] conduct linear cointegration test among any pair of Japan, the United States and China and reach the conclusion that the linear cointegration is rejected. This is the origin of our analysis here because our daily observation suggests that the worldwide stock markets commove at any rate.</p><p>The construction of the present paper is as follows. In Section 2, we propose a time series model of the boom and bust and develop its recursive estimation method. Section 3 modifies this basic model to apply for a ratio variable, which has more restrictive feature within the model of booms and busts. In Section 4, we apply the modified model to detect the nonlinear cointegration relationship between the stock price indexes of Japan and the United States. Section 5 conclude the paper.</p></sec><sec id="s2"><title>2. Model of Nonlinear Cointegration</title><p>In this section, we develop a model of nonlinear cointegration and explain how to estimate the relevant parameters.</p><sec id="s2_1"><title>2.1. The Basic Model</title><p>As an extended model to Asako and Liu (2013) [<xref ref-type="bibr" rid="scirp.66850-ref1">1</xref>], which in turn has its origin in Asako, Kanoh and Sano (1990) and Liu, Asako and Kanoh (2011) [<xref ref-type="bibr" rid="scirp.66850-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.66850-ref5">5</xref>], we propose a model of bubble booms and busts by, for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x7.png" xlink:type="simple"/></inline-formula> &gt; 0,</p><disp-formula id="scirp.66850-formula73"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x8.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x9.png" xlink:type="simple"/></inline-formula> denotes a sequence of variables measured as the ratio of stock prices in different countries and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x10.png" xlink:type="simple"/></inline-formula>denotes a probability that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x11.png" xlink:type="simple"/></inline-formula> follows model (A) depending on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x12.png" xlink:type="simple"/></inline-formula>. A newly arisen bubble <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x13.png" xlink:type="simple"/></inline-formula> is a serially independent and normally distributed random variable with mean 0 and constant variance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x14.png" xlink:type="simple"/></inline-formula> which is unknown to us. The coefficient <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x15.png" xlink:type="simple"/></inline-formula> is a time dependent parameter whose variation is given by the following random walk process:</p><disp-formula id="scirp.66850-formula74"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x16.png"  xlink:type="simple"/></disp-formula><p>Like <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x17.png" xlink:type="simple"/></inline-formula>, the constant variance of innovations <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x18.png" xlink:type="simple"/></inline-formula> is unknown to us. Since we assume <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x19.png" xlink:type="simple"/></inline-formula> &gt; 0, the probability that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x20.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x21.png" xlink:type="simple"/></inline-formula> happen to bring about <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x22.png" xlink:type="simple"/></inline-formula> ≤ 0 is assumed virtually nil.</p><p>Let us consider briefly the implication of this model. Our basic model consists of two regimes or models (A) and (B). At period t, x<sub>t</sub> is expressed by a divergent time series model when a speculative bubble continues. We describe this phenomenon by the autoregressive model (A) with parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x23.png" xlink:type="simple"/></inline-formula> exceeding unity. As implied by a speculative bubble, the divergent sequence will suddenly crash at a certain unknown time. We formulate this event by a systematic and probabilistic switch from model (A) to model (B). In model (B), irrespective of the position <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x24.png" xlink:type="simple"/></inline-formula> at the previous period, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x25.png" xlink:type="simple"/></inline-formula> on average returns at period t to the fundamental value θ<sub>t</sub>.</p><p>More concretely, we assume that the probability of bubble continuation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x26.png" xlink:type="simple"/></inline-formula> can be expressed as</p><disp-formula id="scirp.66850-formula75"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x27.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66850-formula76"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x28.png"  xlink:type="simple"/></disp-formula><p>where α and γ are positive unknown parameters. This formulation implies that π<sub>t</sub> decreases as the deviation between x<sub>t</sub> and θ<sub>t</sub> becomes grater in its absolute value. To put it another way, the probability of a bubble crash, 1-<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x29.png" xlink:type="simple"/></inline-formula>, is an increasing function of how distant the observed bubble deviates from market fundamentals. When α = 0, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x30.png" xlink:type="simple"/></inline-formula> is independent of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x31.png" xlink:type="simple"/></inline-formula> and therefore the probability of crash is constant, which corresponds to the formulation given by Blanchard and Watson (1982) [<xref ref-type="bibr" rid="scirp.66850-ref6">6</xref>]. When α = γ = 0, the whole process is described by the autoregressive process (A) and when γ is large or <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x32.png" xlink:type="simple"/></inline-formula> = 0, the process reduces to a simple white noise process and there is no speculative bubble. Thus, by investigating the parameter estimates, we may statistically test the properties of the process.</p><p>In principle, we can generalize our formulation by considering a broader class of stochastic models for u<sub>t</sub> such as ARMA process or by introducing the fundamental values into the functional form of the transition probability (3). However, we have tried to keep our model as simple as possible because this paper is only meant to be a first step in this research direction. The specification, (3), of the probability turns out to be one of the few analytically tractable formulations in the following analyses.</p><p>When the probability structure of crashes is taken into consideration, we see that the bubble cannot continue forever. As it grows, the probability of a crash approaches unity and x<sub>t</sub> will sooner or later be pulled back to the fundamental value θ<sub>t</sub>. In this way, the time series of x<sub>t</sub> never diverges, but exhibits more or less stable behavior in the longer run.</p><p>Note that letting θ<sub>t</sub> = 0 and assuming away the constraint x<sub>t</sub> &gt; 0 leads us to the models of Asako, Kanoh and Sano (1990) [<xref ref-type="bibr" rid="scirp.66850-ref4">4</xref>], Liu, Asako and Kanoh (2011) [<xref ref-type="bibr" rid="scirp.66850-ref5">5</xref>] and Asako and Liu (2013) [<xref ref-type="bibr" rid="scirp.66850-ref1">1</xref>]. In those models, x<sub>t</sub> is not a ratio variable but is a stock price bubble measured as deviations from their fundamental values. The model of nonlinear cointegration, which is developed in Section 4, adds to this basic model the property that ratio bubbles are symmetric between upwards and downwards.</p></sec><sec id="s2_2"><title>2.2. On Recursive Estimation</title><p>In Liu, Asako and Kanoh (2011) [<xref ref-type="bibr" rid="scirp.66850-ref5">5</xref>] and Asako and Liu (2013) [<xref ref-type="bibr" rid="scirp.66850-ref1">1</xref>], the entire Bayesian recursive estimation process is described for the periods from 0 to 1 and from period t-1 to period t, thus establishing by way of mathematical induction the validity of the recursive estimation method. We develop here only the recursive way of estimating parameters at period t conditioned on the available data up to period t-1. For more in detail of the entire estimation, refer to Liu, Asako and Kanoh (2011) [<xref ref-type="bibr" rid="scirp.66850-ref5">5</xref>] or Asako and Liu (2013) [<xref ref-type="bibr" rid="scirp.66850-ref1">1</xref>].</p><p>One notable difference between the present model (1)-(4) and the earlier ones is that Liu, Asako and Kanoh (2011) [<xref ref-type="bibr" rid="scirp.66850-ref5">5</xref>] and Asako and Liu (2013) [<xref ref-type="bibr" rid="scirp.66850-ref1">1</xref>] assume θ<sub>t</sub> = 0. Once we allow for θ<sub>t</sub> &gt; 0, whether θ<sub>t</sub> is known or unknown causes a big difference in the Bayesian recursive estimation. If it is unknown and to be estimated in the same way as the other parameters of the model, the estimation process becomes too complicated for us to manipulate the model explicitly. On the other hand, if θ<sub>t</sub> is known and treated as a predetermined parameter even though we have to somehow “estimate” it eventually, this estimation can be separated from the estimation of the entire model and its recursive estimation process remains, in terms of hardness, almost at the same level as Asako and Liu (2013) [<xref ref-type="bibr" rid="scirp.66850-ref1">1</xref>]. In fact, we let θ<sub>t</sub> be known and propose its two candidates in Section 3.</p></sec><sec id="s2_3"><title>2.3. Recursive Estimation at Period t</title><p>In this section, we describe a Bayesian recursive technic to estimate the parameters of our model. Before proceeding to this task, we put <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x33.png" xlink:type="simple"/></inline-formula> the set of data observations up to period t, and by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x34.png" xlink:type="simple"/></inline-formula>, we denote the set of ordered integer indices where each i<sub>s</sub> (s = 1; 2; : : : ; t) is either 1, 2, or 3.</p><p>With these new notations, we write down the joint density for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x35.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x36.png" xlink:type="simple"/></inline-formula> conditional on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x37.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.66850-formula77"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x38.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula> are certain deterministic functions of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula> that are to be determined in the sequel so as to satisfy the recursive pattern, whereas P(.) and N(.) denote density functions; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x43.png" xlink:type="simple"/></inline-formula> is the joint prior density function for constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x44.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x45.png" xlink:type="simple"/></inline-formula><sup>1</sup> over time conditioned on X<sup>t</sup> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x46.png" xlink:type="simple"/></inline-formula> is the density function of the normal distribution with mean <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x47.png" xlink:type="simple"/></inline-formula> and variance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x48.png" xlink:type="simple"/></inline-formula>. Their detailed functional forms as well as the definition of the other factors on the right-hand-side of (4) are given immediately below. Note that the summation is over the entire combination of indices which amount to 3<sup>t-1</sup> terms at stage t. Then, in view of (2), the joint prior density function for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x49.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x50.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x51.png" xlink:type="simple"/></inline-formula> conditioned on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x52.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.66850-formula78"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x53.png"  xlink:type="simple"/></disp-formula><p>Now our main task is to calculate the updated posterior density (6) by utilizing the Bayes’ theorem:</p><disp-formula id="scirp.66850-formula79"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x54.png"  xlink:type="simple"/></disp-formula><p>Introducing a new parameter</p><disp-formula id="scirp.66850-formula80"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x55.png"  xlink:type="simple"/></disp-formula><p>for the sake of later convenience in notation, from (1) and the normality of u<sub>t</sub>, we have</p><disp-formula id="scirp.66850-formula81"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x56.png"  xlink:type="simple"/></disp-formula><p>Therefore, in view of (7), the multiplication of (6) and (9) yields the updated formula of (6) for period t if and only if we have, to begin with</p><disp-formula id="scirp.66850-formula82"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x57.png"  xlink:type="simple"/></disp-formula><p>where the first and second terms within the large brackets represent, respectively, the probability density function of exponentially and mutually independently distributed <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x58.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x59.png" xlink:type="simple"/></inline-formula><sup>2</sup>. The integer function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x60.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.66850-formula83"><graphic  xlink:href="http://html.scirp.org/file/66850x61.png"  xlink:type="simple"/></disp-formula><p>is introduced to simplify the mathematical expression.</p><p>Moreover, for the unspecified coefficient functions, we must have</p><disp-formula id="scirp.66850-formula84"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x62.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.66850-formula85"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x63.png"  xlink:type="simple"/></disp-formula><p>Also for means and variances of the normal distributions, it must be</p><disp-formula id="scirp.66850-formula86"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x65.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.66850-formula87"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x66.png"  xlink:type="simple"/></disp-formula><p>Finally, it must be recalled, that by making use of the relationship that applies for conditional density functions</p><disp-formula id="scirp.66850-formula88"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x67.png"  xlink:type="simple"/></disp-formula><p>and knowing that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x68.png" xlink:type="simple"/></inline-formula> are mutually independent in (6), we immediately obtain</p><disp-formula id="scirp.66850-formula89"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x69.png"  xlink:type="simple"/></disp-formula><p>which appears in the denominators of (7) and (11). This establishes all requirement that enable Bayesian recursive estimation to update consistently.</p><sec id="s2_3_1"><title>2.3.1. Parameter Estimates</title><p>The estimates of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x70.png" xlink:type="simple"/></inline-formula> at period t are the conditional expectations on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x71.png" xlink:type="simple"/></inline-formula>. Thus, referring to period t by suffix t, we have</p><disp-formula id="scirp.66850-formula90"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x72.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66850-formula91"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x73.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.66850-formula92"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x74.png"  xlink:type="simple"/></disp-formula><p>We also obtain the probability estimate of bubble continuation from period t-1 to t as</p><disp-formula id="scirp.66850-formula93"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x75.png"  xlink:type="simple"/></disp-formula><p>or we can directly obtain the conditional expectation as</p><disp-formula id="scirp.66850-formula94"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x76.png"  xlink:type="simple"/></disp-formula><p>Finally, the estimate of the variance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x77.png" xlink:type="simple"/></inline-formula> is given by</p><disp-formula id="scirp.66850-formula95"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x78.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_3_2"><title>2.3.2. Maximum Likelihood Estimates of Variances</title><p>In carrying out the recursive procedure explained above, two variance parameters are to be specified. These are the dispersions of the random terms in (1) and (2), i.e., <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x79.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x80.png" xlink:type="simple"/></inline-formula>. The likelihood function for these parameters can be obtained in the following way.</p><p>Let us put <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x81.png" xlink:type="simple"/></inline-formula> for simplicity. The likelihood function for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x82.png" xlink:type="simple"/></inline-formula> with T periods of data is defined as</p><disp-formula id="scirp.66850-formula96"><graphic  xlink:href="http://html.scirp.org/file/66850x83.png"  xlink:type="simple"/></disp-formula><p>On the other hand, since</p><disp-formula id="scirp.66850-formula97"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x84.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.66850-formula98"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x85.png"  xlink:type="simple"/></disp-formula><p>we have, like (16)</p><disp-formula id="scirp.66850-formula99"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x86.png"  xlink:type="simple"/></disp-formula><p>Therefore, the log likelihood function of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x87.png" xlink:type="simple"/></inline-formula> can be expressed by</p><disp-formula id="scirp.66850-formula100"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x88.png"  xlink:type="simple"/></disp-formula><p>and the resulting set of variances <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x89.png" xlink:type="simple"/></inline-formula> which maximize (27) are the desired estimates.</p></sec><sec id="s2_3_3"><title>2.3.3. Condensation of Recursive Estimation</title><p>So far is the complete and mathematically rigorous description of the Bayesian recursive estimation and we can estimate parameters for any length of sample periods. However, the number of terms we need to compute in equations from (11) to (14) and others increases at a rate of 3<sup>t</sup> to exceed a standard capacity of computer as the number of time series data increases. For this reason and to reduce the computational burden, we introduce the so-called condensation procedure first proposed by Harrison and Stevens (1981) [<xref ref-type="bibr" rid="scirp.66850-ref7">7</xref>] and applied for the estimation of the basic model by Liu, Asako and Kanoh (2011) [<xref ref-type="bibr" rid="scirp.66850-ref5">5</xref>] and Asako and Liu (2013) [<xref ref-type="bibr" rid="scirp.66850-ref1">1</xref>]. By condensation, we update the parameters of the next period’s prior distribution by utilizing the first and second moments of the approximated marginal posterior distribution. This enables the computational burden to remain at a constant level over time.</p><p>What we have to do in practice is to approximate the posterior density (5) at period t or the left hand side of (7) by a joint density of the following form</p><disp-formula id="scirp.66850-formula101"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x90.png"  xlink:type="simple"/></disp-formula><p>where we utilize the fact that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x91.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x92.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x93.png" xlink:type="simple"/></inline-formula> are mutually independent. Then the first and second moments of the marginal densities for each parameter are equated. That is, (5) at period t is approximated by</p><disp-formula id="scirp.66850-formula102"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x94.png"  xlink:type="simple"/></disp-formula><p>so that the joint prior density at period t + 1 can be written as</p><disp-formula id="scirp.66850-formula103"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x95.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x96.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x97.png" xlink:type="simple"/></inline-formula> are equated, respectively, to the reciprocal of the mean estimates (17) and (19)</p><disp-formula id="scirp.66850-formula104"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x98.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66850-formula105"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x99.png"  xlink:type="simple"/></disp-formula><p>whereas <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x100.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x101.png" xlink:type="simple"/></inline-formula> are estimates given by (18) and (22). This procedure can be repeated at each stage.</p></sec></sec><sec id="s2_4"><title>2.4. Nonliner Cointegration</title><p>The basic bubble model (1)-(4) formulates the feature that a ratio variable returns to its fundamental value in the long run as the probability that a bubble crashes reaches 100% insofar as the divergent bubble continues. In other words, although short-run bubbles generate explosive discrepancies between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x102.png" xlink:type="simple"/></inline-formula> and θ<sub>t</sub>, divergent booms would bust eventually and in this sense there is a stable relationship in the long run. This phenomenon is what we call the nonlinear cointegration.</p><p>Unlike the definition of linear cointegration, the definition of nonlinear relationship is model-specific. There may be other models of nonlinear cointegration and our nonlinear cointegration should more restrictively be named speculative bubble nonlinear cointegration or boom and bust nonlinear cointegration.</p><p>Such being the case, there is no established method to test the nonlinear cointegration relationship. Instead, we are obliged to accept the existence of the nonlinear relationship only passively. We especially put emphasis on the bubble process in (2) and thereby we detect whether <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x103.png" xlink:type="simple"/></inline-formula> and how often switches occur between two models or how high is the probability of bubble continuation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x104.png" xlink:type="simple"/></inline-formula>.</p><p>In the empirical analysis in Section 4, we compute the pseudo-t statistics:</p><disp-formula id="scirp.66850-formula106"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x105.png"  xlink:type="simple"/></disp-formula><p>in order to sense the “significance“ regarding the validity of β<sub>t</sub> &gt; 1. Since the present estimation technic is Baye- sian in the sense that we utilize prior information besides the information extracted from the data, statistics like (33) may not obey Student’s t-distribution. Nonetheless, we would presume that t = 1.65, which is one sided 5% significant for a standard t test, is a critical level to rely on.</p><p>In detecting the validity of the nonlinear cointegration, we may as well examine into the probability of bubble continuation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x106.png" xlink:type="simple"/></inline-formula>. We check in Section 4 the probability of bubble crash, 1-<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x107.png" xlink:type="simple"/></inline-formula>, and see its movement over time.</p></sec></sec><sec id="s3"><title>3. Nonlinear Cointegration: Modification of the Basic Model</title><p>The basic model we developed in Section 2 is applicable to any series of x<sub>t</sub>. In this section, we modify the basic model to deal with a ratio variable x<sub>t</sub> &gt; 0．A ratio variable may exhibit both upwards and downwards bubble processes with θ<sub>t</sub> &gt; 0, which necessitates certain nontrivial revision in recursive estimation.</p><sec id="s3_1"><title>3.1. Modification of the Basic Model</title><p>We alter the basic model into a double regime switching model. One regime switching is that the basic model is of the boom-and-bust type. The other regime switching is that a ratio variable has both upwards (or positive) and downwards (or negative) bubble processes. On the other hand, we maintain (2) or the transition equation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x108.png" xlink:type="simple"/></inline-formula>as it is.</p><p>Then, we can naturally regard it a bubble by β<sub>t</sub> &gt; 1 once <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x109.png" xlink:type="simple"/></inline-formula> keeps increasing over time. But even when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x110.png" xlink:type="simple"/></inline-formula> keeps decreasing by a downwards bubble, estimates may end up with β<sub>t</sub> &lt; 1 for certain periods of time. In such a case, we may misunderstand what is really happening because β<sub>t</sub> &lt; 1 is usually a case for a stationary autoregressive process. This is quite embarrassing and we may as well be advised to treat the upwards and downwards bubbles asymmetrically. For this aim, we take the reciprocal of the original ratio when the ratio itself is smaller than θ<sub>t</sub> as in (3), thus resulting in a drastic regime switch for negative downwards bubbles.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x111.png" xlink:type="simple"/></inline-formula> represent an original ratio variable of two stock prices, and let us redefine x<sub>t</sub> by</p><disp-formula id="scirp.66850-formula107"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x112.png"  xlink:type="simple"/></disp-formula><p>With this new x<sub>t</sub><sub>,</sub>, we assume that every aspect of the basic model (1)-(4) is valid, i.e.,</p><disp-formula id="scirp.66850-formula108"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x113.png"  xlink:type="simple"/></disp-formula><p>except that</p><disp-formula id="scirp.66850-formula109"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x114.png"  xlink:type="simple"/></disp-formula><p>replaces (8).</p><p>Note that integrating artificially two regimes most likely causes heteroscedasticity in innovation term u<sub>t</sub> in (1) or (35). In fact, we will introduce proportional variance of u<sub>t</sub> to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x115.png" xlink:type="simple"/></inline-formula> squared in our empirical analysis in Section 4:</p><disp-formula id="scirp.66850-formula110"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x116.png"  xlink:type="simple"/></disp-formula><p>Lastly, we need to revise the probability of bubble continuation. That is, in (3), we have</p><disp-formula id="scirp.66850-formula111"><label>(38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x117.png"  xlink:type="simple"/></disp-formula><p>or</p><disp-formula id="scirp.66850-formula112"><label>(39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x118.png"  xlink:type="simple"/></disp-formula><p>that replaces (4). In (38) or (39), the greater deviation is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x119.png" xlink:type="simple"/></inline-formula> for the positive upwards bubble and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x120.png" xlink:type="simple"/></inline-formula> = 1/y<sub>t</sub> − 1/θ<sub>t</sub> for the negative downwards bubble.</p></sec><sec id="s3_2"><title>3.2. Known θ<sub>t</sub></title><p>As we have already noted, the fundamental stock prices ratio θ<sub>t</sub> is assumed known and given to us exogenously at period t. There may be several candidates for θ<sub>t</sub>. Here we propose two alternative ones<sup>3</sup>.</p><sec id="s3_2_1"><title>3.2.1. Past Average</title><p>The first candidate is the simple arithmetic average of all the past data:</p><disp-formula id="scirp.66850-formula113"><label>(40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x121.png"  xlink:type="simple"/></disp-formula><p>Although we put equal weight on each data, the informational role of the current data decreases over time as (40) by definition is rewritten as θ<sub>t</sub> = {(t-1) θ<sub>t</sub><sub>-1</sub><sup>+</sup>y<sub>t</sub>}/t, which in turn is rewritten as</p><disp-formula id="scirp.66850-formula114"><label>(41)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x122.png"  xlink:type="simple"/></disp-formula><p>Equation (41) implies that θ<sub>t</sub> follows a random-walk type sticky movement except that the drift term is not stochastic but is given deterministically. As t increases, the contribution of the second term on the right hand side of (41) decreases over time.</p></sec><sec id="s3_2_2"><title>3.2.2. Fixed Period Moving Average</title><p>The second candidate approximates the fundamental value by the fixed period (say 12 months) moving average up to the current one. Thus in place of (40) we have</p><disp-formula id="scirp.66850-formula115"><label>(42)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x123.png"  xlink:type="simple"/></disp-formula><p>And thereby in place of (41), we have</p><disp-formula id="scirp.66850-formula116"><label>(43)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/66850x124.png"  xlink:type="simple"/></disp-formula><p>for t &gt; 12. As for the first 12 months, we use the simple average (40).</p></sec></sec><sec id="s3_3"><title>3.3. Estimation Procedure at Period t</title><p>At period t, we compute θ<sub>t</sub> once we get a new data y<sub>t</sub> and we determine which regime we are in, i.e., whether a positive bubble (y<sub>t</sub> ≥ θ<sub>t</sub>) or a negative bubble (y<sub>t</sub> &lt; θ<sub>t</sub>). If we are rigorously interested in whether the stock price ratio is in positive upwards phase or in negative downwards phase, we may watch where we have been in the past. For example, we would recognize regime shifts only if the opposite new regime continues at least a few consecutive periods. This will exclude a fake regime shift that occurs unsystematically. The idea of this rule of thumb stems from the Bry-Boschan method in the judgment of the business cycle phase.</p><p>Once θ<sub>t</sub> and thereby the data x<sub>t</sub> of (34) is obtained, we are ready to utilize the recursive estimation technic developed in Section 2. We estimate the basic model as applied to the stock market prices of Japan and the United States.</p></sec></sec><sec id="s4"><title>4. Stock Prices of Japan and the United States</title><p>Asako, Zhang and Liu (2014) attempted to apply the nonlinear cointegration to the stock markets of Japan, the United States and China. They first checked whether there is a linear cointegration relationship between these countries and concluded negatively for any pair of countries. Then they estimated the basic model of (1)-(4) and of three ways of the known fundamental stock prices ratio including (40) and (42). Among these, in what follow, we develop the most representative case of the nonlinear cointegration; namely the one between the stock price indexes of Japan and the United State.</p><sec id="s4_1"><title>4.1. Preparatory Steps</title><p>The monthly time series data we have chosen are the Nikkei225 index (hereinafter Nikkei225) for Japan and the Dow-Jones Industrial Average Stock Price Index (hereinafter DJ) for the United States. <xref ref-type="fig" rid="fig1">Figure 1</xref> plots these stock prices and their ratio (DJ/Nikkei225) from January 1970 to December 2012.</p><sec id="s4_1_1"><title>4.1.1. Derivation of Known θ<sub>t</sub></title><p><xref ref-type="fig" rid="fig2">Figure 2</xref> exhibits the fundamental stock prices ratio given by (40) and (42). Not surprisingly, (i) the past average <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x126.png" xlink:type="simple"/></inline-formula> shows a random-walk type sluggish swing whereas (ii) the fixed period moving average <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x127.png" xlink:type="simple"/></inline-formula> traces short lived ups and downs around the historical actual path of the ratio y<sub>t</sub>.</p></sec><sec id="s4_1_2"><title>4.1.2. Artificial Dependent Variable</title><p>Next, we construct from the time series y<sub>t</sub> that of the artificial variable x<sub>t</sub> by (34). Referring to the realized y<sub>t</sub> and two fundamental stock prices ratio θ<sub>t</sub>, the time series of x<sub>t</sub> consists of negative bubble (y<sub>t</sub> &lt; θ<sub>t</sub>) up to the mid 1990s and thereby, by definition, x<sub>t</sub> equals the reciprocal of y<sub>t</sub>. On the contrary, during the latter half of the sample period, x<sub>t</sub> consists of positive bubble (y<sub>t</sub> &gt; θ<sub>t</sub>) and x<sub>t</sub> is y<sub>t</sub> itself. In the case of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x128.png" xlink:type="simple"/></inline-formula>, however, y<sub>t</sub> &gt; θ<sub>t</sub> and y<sub>t</sub> &lt; θ<sub>t</sub> interchange with small intervals, as does x<sub>t</sub>.</p></sec><sec id="s4_1_3"><title>4.1.3. Maximum Likelihood Estimates of Variances</title><p>We need to obtain the maximum likelihood estimates for the variances of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x129.png" xlink:type="simple"/></inline-formula> in (1) and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x130.png" xlink:type="simple"/></inline-formula> in (2). We also have to set initial values in beginning the recursive estimation. The effect of the initial conditions turns out to be minimal as we tried several combinations to result in little difference in the main feature of estimation except for several initial periods. The final choice was <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x131.png" xlink:type="simple"/></inline-formula> = 1, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x132.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x133.png" xlink:type="simple"/></inline-formula> = <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x134.png" xlink:type="simple"/></inline-formula> = 0.01 and denoting by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x135.png" xlink:type="simple"/></inline-formula> the pair of standard deviations, the maximum likelihood estimates were (0.0536, 0.0000) for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x136.png" xlink:type="simple"/></inline-formula> and (0.0456, 0.0000) for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x137.png" xlink:type="simple"/></inline-formula>. The resultant log likelihoods were 377.9 and 600.7, respectively.</p><p>Judging on the log likelihood, between the two fundamental stock prices ratio, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x141.png" xlink:type="simple"/></inline-formula> fits the data better than <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x142.png" xlink:type="simple"/></inline-formula> does. Knowing this consequence, we yet report those alternative fundamental values as these yield really comparable estimation results as we explain in the sequel<sup>4</sup>.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Stock Price Indexes: Japan and the US. Note) The Nikkei225 for Japan and DJ for the United States</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/66850x143.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Fundamental value θ<sub>t</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/66850x144.png"/></fig></sec></sec><sec id="s4_2"><title>4.2. Necessary Condition for the Bubble</title><p>With the above preparation, <xref ref-type="fig" rid="fig3">Figure 3</xref> exhibits the estimate of the key parameter β<sub>t</sub>. The percentage of samples that satisfies the necessary requirement for bubbles β<sub>t</sub> &gt; 1 amounts to 82.9% for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x145.png" xlink:type="simple"/></inline-formula> and 100% for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x146.png" xlink:type="simple"/></inline-formula> among the entire 43 years’ sample periods (516 months from 1970; 1 to 2012;12). Namely with both <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x147.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x148.png" xlink:type="simple"/></inline-formula>, samples with β<sub>t</sub> &gt; 1 exceed more than 80%. These observations may as well support the view that the model (1)-(4) with reasonable modification fits the data and the stock markets of Japan and the United States are cointegrated nonlinearly in the long run. But how reliable is this result?</p><p>To answer to this question, we checked the pseudo t t-statistic (33) and found, as summarized in <xref ref-type="table" rid="table1">Table 1</xref>, that β<sub>t</sub> &gt; 1 is one sided 5% “pseudo-significant” is nil for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x149.png" xlink:type="simple"/></inline-formula> and 93.0% for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x150.png" xlink:type="simple"/></inline-formula> (similarly the nonstationarity condition β<sub>t</sub> &lt; 1 is not significant). These suggest that the standard deviation of β<sub>t</sub> is relatively large, and the reliability of the estimates is limited. Note, on the contrary, that β<sub>t</sub> &gt; 1 is 93.3% pseudo-significant for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x151.png" xlink:type="simple"/></inline-formula>.</p><p>A clue to this is that the maximum likelihood variance estimate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x152.png" xlink:type="simple"/></inline-formula> is extremely small and is virtually the corner solution at zero. In this case, the key parameter β<sub>t</sub> is theoretically regarded constant in (2). But, like the parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x153.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x154.png" xlink:type="simple"/></inline-formula>, the estimate of β<sub>t</sub> does not have to stay unchanged over time. Even if the variance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x155.png" xlink:type="simple"/></inline-formula> is 0 in (2), we have</p><p>β<sub>t</sub> = β<sub>t</sub><sub>-1</sub> + constant,</p><p>and β<sub>t</sub> can be different from β<sub>t</sub><sub>-1</sub>. Moreover, even if the constant term is 0 and β<sub>t</sub> = β<sub>t</sub><sub>-1</sub>, in theory, because β<sub>t</sub> is estimated as the expected value of the posterior distribution &#224; la Bayesian, it can differ from β<sub>t</sub><sub>-1</sub> once the data increases information in the posterior distribution in (18).</p></sec><sec id="s4_3"><title>4.3. Probability of Bubble Crash</title><p>In <xref ref-type="fig" rid="fig4">Figure 4</xref>, we plot the probability of bubble crash, 1-π<sub>t</sub>. As π<sub>t</sub>, the conditional expectation (21), rather than the point estimate (20), is chosen<sup>5</sup>. With <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x157.png" xlink:type="simple"/></inline-formula> the crash probability remains small except for the early 1970’s, which seems to be a transitional feature incorporating specific initial conditions, whereas with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x158.png" xlink:type="simple"/></inline-formula> the probability repeatedly rises and falls depending on the state of bubbles.</p></sec><sec id="s4_4"><title>4.4. Other Cases</title><p>Asako, Zhang and Liu (2014) [<xref ref-type="bibr" rid="scirp.66850-ref3">3</xref>] estimate several other cases including exchange rate adjusted stock prices, the</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Estimate of β<sub>t</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/66850x159.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Probability of bubble crash</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/66850x160.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Number of months of the estimated β<sub>t</sub></title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  ></th><th align="center" valign="middle" >1970 -72</th><th align="center" valign="middle" >1973 -76</th><th align="center" valign="middle" >1977 -80</th><th align="center" valign="middle" >1981 -84</th><th align="center" valign="middle" >1985 -88</th><th align="center" valign="middle" >1989 -92</th><th align="center" valign="middle" >1993 -96</th><th align="center" valign="middle" >1997 -2000</th><th align="center" valign="middle" >2001 -04</th><th align="center" valign="middle" >2005 -08</th><th align="center" valign="middle" >2009 -12</th></tr></thead><tr><td align="center" valign="middle"  colspan="2"  ></td><td align="center" valign="middle" >β<sub>t</sub> ≥ 1</td><td align="center" valign="middle" >35</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >21</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >40</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >44</td><td align="center" valign="middle" >48</td></tr><tr><td align="center" valign="middle"  colspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x161.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >significant at 5%</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle"  colspan="2"  ></td><td align="center" valign="middle" >β<sub>t</sub> &lt; 1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >27</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle"  colspan="2"  ></td><td align="center" valign="middle" >significant at 5%</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle"  colspan="2"  ></td><td align="center" valign="middle" >β<sub>t</sub> ≥ 1</td><td align="center" valign="middle" >35</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td></tr><tr><td align="center" valign="middle"  colspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x162.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >significant at 5%</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >47</td><td align="center" valign="middle" >40</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td><td align="center" valign="middle" >48</td></tr><tr><td align="center" valign="middle"  colspan="2"  ></td><td align="center" valign="middle" >β<sub>t</sub> &lt; 1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle"  colspan="2"  ></td><td align="center" valign="middle" >significant at 5%</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><p>case of Var (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x163.png" xlink:type="simple"/></inline-formula>) = <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/66850x164.png" xlink:type="simple"/></inline-formula> instead of (37), stock prices ratio of Japan and China, and that of China and the United States. The estimation results vary case by case but reaches the conclusion that the basic model (1)-(4) and its modification with β<sub>t</sub> &gt; 1 fits the data reasonably well, thus establishing the latent nonlinear boom and bust relationship between relevant stock prices.</p></sec></sec><sec id="s5"><title>5. Concluding Remarks</title><p>In this paper we proposed and developed the recursive estimation method of the nonlinear cointegration. The purpose of this attempt has been to show the usefulness of introducing the idea of nonlinear cointegration. By applying this idea to the stock market indexes of Japan and the United States, we have seen that these indexes commove in the long run although they deviate from this relationship in the short run.</p></sec><sec id="s6"><title>Cite this paper</title><p>Kazumi Asako,Zhentao Liu, (2016) Comovement of Stock Markets—An Analysis by Nonlinear Cointegration*. Open Journal of Social Sciences,04,64-75. doi: 10.4236/jss.2016.45010</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.66850-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Asako, K. and Liu, Z.T. (2013) A Statistical Moddel of Speculative Bubbles, with Applications to the Stock Markets of the United States, Japan, and China. Journal of Banking &amp; Finance, 37, 2639-2651.  
http://dx.doi.org/10.1016/j.jbankfin.2013.02.015</mixed-citation></ref><ref id="scirp.66850-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Engle, R.F. and Granger, C.W.J. (1987) Cointegration and Error Correction: Representation, Estimation and Testing.  Econometrica, 55, 251-276. http://dx.doi.org/10.2307/1913236</mixed-citation></ref><ref id="scirp.66850-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Asako, K., Zhang, Y. and Liu, Z.T. (2014) The Comovement in Stock Price Indexes of Japan, United States, and China: Estimation of a Nonlinear Cointe-gration. Economic Review, 65, 56-85 (in Japanese).</mixed-citation></ref><ref id="scirp.66850-ref4"><label>4</label><mixed-citation publication-type="book" xlink:type="simple">Asako, K., Kanoh, S. and Sano, H. (1990) Stock Price and Bubble. In: Nishimura, K. and Miwa, Y., Eds., Stock and Land Prices in Japan—Mechanism of Price Determination, University of Tokyo Press, 57-86 (in Japanese).</mixed-citation></ref><ref id="scirp.66850-ref5"><label>5</label><mixed-citation publication-type="book" xlink:type="simple">Liu, Z.T., Asako, K. and Kanoh, S. (2011) Estimation of Speculative Bubble—Application to the Stock Markets of Japan, the United States and China. In: Asakoand, K. and Watanabe T., Eds., Econometrical Analyses of Finance and Business Cycle, Minerva Shobou, 9-34 (in Japanese).</mixed-citation></ref><ref id="scirp.66850-ref6"><label>6</label><mixed-citation publication-type="book" xlink:type="simple">Blanchard, O.J. and Watson, M. (1982) Bubbles, Rational Expectations and Financial Markets. In: Wachtel, P., Ed., Crises in the Economic and Financial Structure, Lexington Books, 295-315.</mixed-citation></ref><ref id="scirp.66850-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Harrison, P.J. and Stevens, C.F. (1976) Bayesian Forcasting (with Discussion). Journal of the Royal Statistical Society: Series B, 38, 205-247.</mixed-citation></ref></ref-list></back></article>