<?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">JMF</journal-id><journal-title-group><journal-title>Journal of Mathematical Finance</journal-title></journal-title-group><issn pub-type="epub">2162-2434</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmf.2016.65058</article-id><article-id pub-id-type="publisher-id">JMF-72118</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> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  A Target Zone Model Where the Fundamentals Follow a Geometric Brownian Motion
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jean</surname><given-names>René Cupidon</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Judex</surname><given-names>Hyppolite</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Economics, Finance, and Real Estate, Monmouth University, West Long Branch, NJ, USA</addr-line></aff><aff id="aff1"><addr-line>Department of Economics, Berea Collge, Berea, KY, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>cupidonj@berea.edu(JRC)</email>;<email>jhyppoli@monmouth.edu(JH)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>10</day><month>11</month><year>2016</year></pub-date><volume>06</volume><issue>05</issue><fpage>866</fpage><lpage>886</lpage><history><date date-type="received"><day>October</day>	<month>5,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>November</month>	<year>15,</year>	</date><date date-type="accepted"><day>November</day>	<month>18,</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>
 
 
  In this paper, we propose a model of exchange rate target zone based on a specification of the economic fundamentals known as a Geometric Brownian Motion. The rationale behind this specification is that the fundamentals series is not necessarily normally distributed as commonly assumed, as indicated by its excess kurtosis and ARCH properties. Therefore, assuming a normal specification can be problematic. The main difficulty is that with such a specification finding a closed form solution for the model becomes somehow more involved. We present some results in which the exchange rate formula is explicitly derived. Then we look at several types of central bank interventions in the foreign exchange market such as Krugman’s marginal interventions, central bank interventions a la Caballero and central bank interventions a la Flood-Garber. In addition, we present some empirical investigations where it is found that, for the most part, these exchange rate models do not fit the data well and a case where the model performs satisfactorily. We believe that the sources of the problem may reside in the complexity of estimating the models efficiently given that the theoretical approach is quite sound.
 
</p></abstract><kwd-group><kwd>Exchange Rates</kwd><kwd> Target Zone</kwd><kwd> Stochastic Differential Equations</kwd><kwd> Delay Differential Equations</kwd><kwd> Simulated Methods of Moments</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>A target zone model is an exchange rate model where the monetary authorities are committed to keeping the exchange rate within some specific bands commonly known as a target zone [<xref ref-type="bibr" rid="scirp.72118-ref1">1</xref>] . Establishing a zone is one type of central bank interventions. One of the main goals is to stabilize the currency. Given the weak empirical support for most of the basic target zone models [<xref ref-type="bibr" rid="scirp.72118-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.72118-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.72118-ref4">4</xref>] as provided by Jong [<xref ref-type="bibr" rid="scirp.72118-ref2">2</xref>] and Spencer and Smith [<xref ref-type="bibr" rid="scirp.72118-ref5">5</xref>] , a number of alternative models of target zone modeling have been introduced by relaxing the two main assumptions of the basic target zone model [<xref ref-type="bibr" rid="scirp.72118-ref6">6</xref>] , namely infinitesimal marginal interventions and perfect credibility [<xref ref-type="bibr" rid="scirp.72118-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.72118-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.72118-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.72118-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.72118-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.72118-ref11">11</xref>] . However, regardless of the alternative model being introduced, no serious attention has been given to the fundamentals’ variable behavior and therefore an agnostic arithmetic Brownian motion process is commonly used to describe the stochastic process governing the fundamentals, though some models include the possibility of jump in the diffusion process for the fundamentals [<xref ref-type="bibr" rid="scirp.72118-ref12">12</xref>] . But assuming an arithmetic Brownian Motion (ABM) process for the fundamentals is basically assuming the variable has a normal distribution, at least within the band, an assumption would be hard to be maintained given a related work on an empirical study of the specific fundamental determinant of exchange rate determination in a working paper where we have seen that the fundamentals for the most part exhibit kurtosis and skewness properties and even ARCH properties. It is true that which fundamentals to be used depend on the model of exchange determination being considered. Our analysis is based on the monetary model of exchange rate determination [<xref ref-type="bibr" rid="scirp.72118-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.72118-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.72118-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.72118-ref16">16</xref>] , the most commonly used model of exchange rate determination in empirical work, which leads to the following fundamental equation of exchange rate determination.</p><disp-formula id="scirp.72118-formula71"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x2.png"  xlink:type="simple"/></disp-formula><p>Equivalently, we can write</p><disp-formula id="scirp.72118-formula72"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x3.png"  xlink:type="simple"/></disp-formula><p>Here, we propose a model where the fundamentals follow a geometric Brownian Motion (GBM). We will also consider the predictions of the model for target zone modeling under Krugman interventions as well as under discrete interventions by the monetary authorities. First, we present some background about the behavior of the fundamentals assumed to drive exchange rate movements.</p></sec><sec id="s2"><title>2. Some Computational Aspects of the Fundamentals</title><p>The model assumes that the fundamentals follow a Geometric Brownian Motion (GBM)</p><disp-formula id="scirp.72118-formula73"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x4.png"  xlink:type="simple"/></disp-formula><p>where W(t) is a standard brownian motion or Wiener process. Here,the drift parameter, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x5.png" xlink:type="simple"/></inline-formula>, and the volatility or diffusion parameter, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x6.png" xlink:type="simple"/></inline-formula>, are time-varying. In fact, this is more consistent with empirical examinations of the fundamentals where it is found that the fundamentals do often exhibit ARCH effects. The ABM formulation assumes that such parameters are constant over time. From stochastic calculus, it can be shown easily that if the fundamentals follow an ABM process, then we have</p><disp-formula id="scirp.72118-formula74"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x7.png"  xlink:type="simple"/></disp-formula><p>Now, we want to investigate the distribution of the GBM process. The equation above is a diffusion stochastic differential equation. If we can solve the SDE, probably that can shed some light on the distribution of the process. The fact is that this class of linear stochastic differential equations can be solved analytically. For completeness, we will present the details of the solution method. Also, we will calculate some moments. First, to find the mean, we rewrite the SDE in an equivalent integral form</p><disp-formula id="scirp.72118-formula75"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x8.png"  xlink:type="simple"/></disp-formula><p>The first integral is the integral of a random function with respect to a standard measure, the Riemann measure, and the second integral is an Ito stochastic integral. We have</p><disp-formula id="scirp.72118-formula76"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x9.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula77"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x10.png"  xlink:type="simple"/></disp-formula><p>The last equation results from the Ito isometry theorem. Taking expectations, we ob- tain</p><disp-formula id="scirp.72118-formula78"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x11.png"  xlink:type="simple"/></disp-formula><p>Setting<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x12.png" xlink:type="simple"/></inline-formula>, the moment equation becomes</p><disp-formula id="scirp.72118-formula79"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x13.png"  xlink:type="simple"/></disp-formula><p>This equation is an integral equation of the first kind which occurs commonly in the theory of integral equations and can be easily solved. Differentiate both sides to obtain</p><disp-formula id="scirp.72118-formula80"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x14.png"  xlink:type="simple"/></disp-formula><p>The solution to this linear differential equation is given by</p><disp-formula id="scirp.72118-formula81"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x15.png"  xlink:type="simple"/></disp-formula><p>Now, we look at the second moment, the variance of the process. To do that, we first try to compute<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x16.png" xlink:type="simple"/></inline-formula>. To do so, a standard technique is to use Ito’s lemma. De- fine a new process,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x17.png" xlink:type="simple"/></inline-formula>. Ito’s lemma implies</p><disp-formula id="scirp.72118-formula82"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x18.png"  xlink:type="simple"/></disp-formula><p>Then</p><disp-formula id="scirp.72118-formula83"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x19.png"  xlink:type="simple"/></disp-formula><p>This implies that</p><disp-formula id="scirp.72118-formula84"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x20.png"  xlink:type="simple"/></disp-formula><p>Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x21.png" xlink:type="simple"/></inline-formula>. We obtain the following integral equation</p><disp-formula id="scirp.72118-formula85"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x22.png"  xlink:type="simple"/></disp-formula><p>Therefore, we obtain the following ODE</p><disp-formula id="scirp.72118-formula86"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x23.png"  xlink:type="simple"/></disp-formula><p>The solution is given by</p><disp-formula id="scirp.72118-formula87"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x24.png"  xlink:type="simple"/></disp-formula><p>The variance is given as</p><disp-formula id="scirp.72118-formula88"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x25.png"  xlink:type="simple"/></disp-formula><p>Now, we would like to determine the distribution of the process f(t). The interesting property of such a formulation is that we can solve explicitly the SDE as it is known in the literature. The SDE</p><disp-formula id="scirp.72118-formula89"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x26.png"  xlink:type="simple"/></disp-formula><p>is a linear SDE with nonconstant coefficients,we can solve the SDE using the integrating factor technique. But, using this method leads to stochastic integral equation which is more difficult to solve than the SDE itself. Alternatively, we use the common solution technique, though a general method of solving linear SDEs. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x27.png" xlink:type="simple"/></inline-formula>. Using Ito’s lemma, we have</p><disp-formula id="scirp.72118-formula90"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x28.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula91"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x29.png"  xlink:type="simple"/></disp-formula><p>That is</p><disp-formula id="scirp.72118-formula92"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x30.png"  xlink:type="simple"/></disp-formula><p>This solution does not tell us much about the distribution of the stochastic process governing the fundamentals. But, we can find out about the nature of the distribution by observing the following.</p><p>Rewrite (18) as</p><disp-formula id="scirp.72118-formula93"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x31.png"  xlink:type="simple"/></disp-formula><p>It is clear that</p><disp-formula id="scirp.72118-formula94"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x32.png"  xlink:type="simple"/></disp-formula><p>It follows that</p><disp-formula id="scirp.72118-formula95"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x33.png"  xlink:type="simple"/></disp-formula><p>That is, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x34.png" xlink:type="simple"/></inline-formula>has a lognormal distribution. The lognormal probability distribu-</p><p>tion function is very important in applied work. We can analyze its kurtosis and skewness by using a very powerful statistical technique, namely, the moment generating function technique without having to rely on some relatively tedious calculations. We briefly define the lognormal distribution and show how the moment generating function technique can be applied to calculate some of the moments.</p><p>Suppose that the random variable X has a lognormal distribution with μ and variance σ<sup>2</sup>. Now, we apply the moment generating function technique to find the first and second moment. Define the random variable<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x35.png" xlink:type="simple"/></inline-formula>. The mean is given by</p><disp-formula id="scirp.72118-formula96"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x36.png"  xlink:type="simple"/></disp-formula><p>Similarly, we obtain</p><disp-formula id="scirp.72118-formula97"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x37.png"  xlink:type="simple"/></disp-formula><p>Therefore, the variance of X is given by</p><disp-formula id="scirp.72118-formula98"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x38.png"  xlink:type="simple"/></disp-formula><p>We see that we could have used this result on lognormal probability distribution functions to calculate the first moments of the f(t) process. A final remark to be made about the stochastic process governing the fundamentals f(t) is that the SDE that defines the process has two unknown parameters, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x39.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x40.png" xlink:type="simple"/></inline-formula>. Empirically, such parameters defined this way in an SDE can be estimated by simulation. In the target zone model we will analyze, such a method would not be appropriate. The model’s parameters should be estimated simultaneously. Besides, the target zone model is based on the so-called regulated stochastic differential equations. Now, it is time to tackle the main topic of this subject given the rationale behind the set up of the SDE describing the behavior of the fundamentals, at least within the band.</p></sec><sec id="s3"><title>3. Estimating the Fundamentals’ Parameters</title><p>In this section, we pay a special attention to the task of estimating the parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x41.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x42.png" xlink:type="simple"/></inline-formula> of the GBM specification for the fundamentals process, f(t). In the above sec-</p><p>tion we showed that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x43.png" xlink:type="simple"/></inline-formula> follows a log-normal distribution when the fundamentals</p><p>are modeled as a geometric Brownian motion. More specifically,</p><disp-formula id="scirp.72118-formula99"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x44.png"  xlink:type="simple"/></disp-formula><p>In this specific case the parameters can be estimated by exact maximum likelihood. For the sample<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x45.png" xlink:type="simple"/></inline-formula>, the likelihood can be written as</p><disp-formula id="scirp.72118-formula100"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x46.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x47.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x48.png" xlink:type="simple"/></inline-formula> can be estimated by maximizing the logarithm of the preceding likelihood.</p><p>However, for more general cases, in particular when the geometric Brownian is regulated, the exact likelihood function is unknown and the researcher has to rely on approximation methods. A large body of literature has been devoted to parameter estimation of SDEs such as Discrete Maximum Likelihood (DML) methods, Hermite Polynomial Approximations, Infinitesimal Operator methods advocated by [<xref ref-type="bibr" rid="scirp.72118-ref17">17</xref>] . In essence, most of these numerical methods focus on approximating the transitional PDF of the process, which, in general, does not have a closed form expression.</p><p>For an SDE of the form</p><disp-formula id="scirp.72118-formula101"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x49.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x50.png" xlink:type="simple"/></inline-formula> is a vector of parameters.</p><p>The transitional PDF satisfies the Fokker-Plank equation with initial and boundary conditions</p><disp-formula id="scirp.72118-formula102"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x51.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula103"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x52.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula104"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x53.png"  xlink:type="simple"/></disp-formula><p>where S is the state space, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x54.png" xlink:type="simple"/></inline-formula>is the initial time and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x55.png" xlink:type="simple"/></inline-formula> is the initial state of the pro- cess at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x56.png" xlink:type="simple"/></inline-formula>. Discrete Maximum Likelihood methods have been very popular in empirical work. The traditional DML uses an Euler-Maruyama algorithm with one step of duration:</p><disp-formula id="scirp.72118-formula105"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x57.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x58.png" xlink:type="simple"/></inline-formula>.</p><p>Other methods use a Milstein approximation algorithm which, in most cases, give superior estimators compared to the Euler-Maruyama scheme. Our model specification for the fundamentals process states that</p><disp-formula id="scirp.72118-formula106"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x59.png"  xlink:type="simple"/></disp-formula><p>Letting<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x60.png" xlink:type="simple"/></inline-formula>, an Euler-Maruyama algorithm with one step of duration gives the discretization</p><disp-formula id="scirp.72118-formula107"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x61.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x62.png" xlink:type="simple"/></inline-formula> is a standard normal random variable.Hence, the approximated transitional PDF is assumed to be normal with mean <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x63.png" xlink:type="simple"/></inline-formula> and variance<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x64.png" xlink:type="simple"/></inline-formula>.</p><p>Now, take a sample <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x65.png" xlink:type="simple"/></inline-formula> of N + 1 observations of the process f at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x66.png" xlink:type="simple"/></inline-formula>. The likelihood function of the sample observation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x67.png" xlink:type="simple"/></inline-formula> is given by</p><disp-formula id="scirp.72118-formula108"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x68.png"  xlink:type="simple"/></disp-formula><p>where we define</p><disp-formula id="scirp.72118-formula109"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x69.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula110"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x70.png"  xlink:type="simple"/></disp-formula><p>The log-likelihood function is given by</p><disp-formula id="scirp.72118-formula111"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x71.png"  xlink:type="simple"/></disp-formula><p>The first order conditions entail</p><disp-formula id="scirp.72118-formula112"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x72.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula113"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x73.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula114"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x74.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula115"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x75.png"  xlink:type="simple"/></disp-formula><p>As indicated above, in our formulation, no approximation is necessary for estimation purposes given that a closed form solution for the likelihood function is available. We present the exact maximum likelihood estimation results as well as the pseudo maximum likelihood results below where we use velocity as economic fundamentals, as in [<xref ref-type="bibr" rid="scirp.72118-ref6">6</xref>] . This is slight departure from the monetary fundamentals specification based on the monetary model of exchange rate determination.</p><p>The estimates are presented below (<xref ref-type="table" rid="table1">Table 1</xref>).</p><p>It is clear that the model is consistent with the data.</p></sec><sec id="s4"><title>4. The Target Zone Model</title><p>The target zone model considered here is driven by the behavior of the process governing the fundamentals process. We argued previously that a formulation of the series governing the fundamental determinant of exchange rate, f(t), is supposed to be guided by empirical considerations on the behavior of the series f(t) and therefore, models, whatever variables being considered as economic fundamentals, should not be agnostic about such behavior. In effect, the fundamental series f(t), as we have previously highlighted, depends on the model of exchange rate determination being considered. Again, the emphasis is put on the classical monetary model of exchange rate determination as in [<xref ref-type="bibr" rid="scirp.72118-ref18">18</xref>] .</p><p>As before, we assume that the dynamic behavior of the fundamentals is governed by the stochastic differential equation</p><disp-formula id="scirp.72118-formula116"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x76.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x77.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x78.png" xlink:type="simple"/></inline-formula> are parameters to be estimated along with the other parameter of the model, which is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x79.png" xlink:type="simple"/></inline-formula> in our model. As before, we use the fundamental equation for the exchange rate derived from the monetary model in continuous time</p><disp-formula id="scirp.72118-formula117"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x80.png"  xlink:type="simple"/></disp-formula><p>or equivalently,</p><disp-formula id="scirp.72118-formula118"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x81.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x82.png" xlink:type="simple"/></inline-formula> is positive.</p><p>The model’s parameters are<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x83.png" xlink:type="simple"/></inline-formula>. These parameters need to be estimated simultaneously. Though the solution to the SDE governing the dynamic behavior of the fundamentals is not required for estimation purposes, it is necessary to find a closed form solution for the exchange rate, s(t), satisfying the fundamental equation. The solution is given in the following proposition.</p><p>Proposition 1. Suppose that the fundamentals, f(t), satisfy the stochastic differential equation</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Estimates of the parameters of the fundamentals process</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="3"  >Exact MLE</th><th align="center" valign="middle"  colspan="3"  >Pseudo MLE</th></tr></thead><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >estimates</td><td align="center" valign="middle" >ste</td><td align="center" valign="middle" >p-value</td><td align="center" valign="middle" >estimates</td><td align="center" valign="middle" >ste</td><td align="center" valign="middle" >p-value</td></tr><tr><td align="center" valign="middle" >m</td><td align="center" valign="middle" >0.010</td><td align="center" valign="middle" >0.004</td><td align="center" valign="middle" >0.021</td><td align="center" valign="middle" >0.010</td><td align="center" valign="middle" >0.005</td><td align="center" valign="middle" >0.038</td></tr><tr><td align="center" valign="middle" >s</td><td align="center" valign="middle" >0.033</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >0.034</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >0.000</td></tr><tr><td align="center" valign="middle" >Log-likelihood</td><td align="center" valign="middle" >−183.333</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >−177.237</td><td align="center" valign="middle" >0.000</td><td align="center" valign="middle" >0.000</td></tr></tbody></table></table-wrap><disp-formula id="scirp.72118-formula119"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x84.png"  xlink:type="simple"/></disp-formula><p>Also, assume that the exchange rate is determined by the equation</p><disp-formula id="scirp.72118-formula120"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x85.png"  xlink:type="simple"/></disp-formula><p>Then a family of solutions for the exchange rate is given by</p><disp-formula id="scirp.72118-formula121"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x86.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.72118-formula122"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x87.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula123"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x88.png"  xlink:type="simple"/></disp-formula><p>where A and B are arbitrary constants.</p><p>Proof. The fundamentals are assumed to satisfy the SDE or GBM</p><disp-formula id="scirp.72118-formula124"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x89.png"  xlink:type="simple"/></disp-formula><p>Guess that the exchange rate function is a time invariant function of the current fundamentals, that is, s(t) has the strong Markov property. Thus, we can set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x90.png" xlink:type="simple"/></inline-formula>. By Ito’s lemma also known as Ito’s stochastic change of variable formula, we have</p><disp-formula id="scirp.72118-formula125"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x91.png"  xlink:type="simple"/></disp-formula><p>Then we obtain</p><disp-formula id="scirp.72118-formula126"><label>(38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x92.png"  xlink:type="simple"/></disp-formula><p>This leads to the following second order differential equation given by</p><disp-formula id="scirp.72118-formula127"><label>(39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x93.png"  xlink:type="simple"/></disp-formula><p>This is a functional equation of the form</p><disp-formula id="scirp.72118-formula128"><label>(40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x94.png"  xlink:type="simple"/></disp-formula><p>This belongs to a well known class of ordinary differential equations known as the Cauchy-Euler or Equidimensional equation. Closed form solutions for such a class of differential equations exist. There are several methods for solving this class of ODEs. One such methods is he to use the theory of Laplace transforms. But, finding the inverse Laplace transform may be not that simple. The easiest solution method is to set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x95.png" xlink:type="simple"/></inline-formula> and obtain</p><disp-formula id="scirp.72118-formula129"><label>(41)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x96.png"  xlink:type="simple"/></disp-formula><p>As usual, we solve the second order homogeneous ODE</p><disp-formula id="scirp.72118-formula130"><label>(42)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x97.png"  xlink:type="simple"/></disp-formula><p>The characteristic equation is given by</p><disp-formula id="scirp.72118-formula131"><label>(43)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x98.png"  xlink:type="simple"/></disp-formula><p>Given the definition of a, b, c, we have</p><disp-formula id="scirp.72118-formula132"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x99.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula133"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x100.png"  xlink:type="simple"/></disp-formula><p>Therefore, the general solution to the homogeneous equation is given by</p><disp-formula id="scirp.72118-formula134"><label>(44)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x101.png"  xlink:type="simple"/></disp-formula><p>To find a particular solution, suppose it is given by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x102.png" xlink:type="simple"/></inline-formula>.</p><p>Assuming that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x103.png" xlink:type="simple"/></inline-formula>, it can be shown that the coefficients are given by</p><disp-formula id="scirp.72118-formula135"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x104.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula136"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x105.png"  xlink:type="simple"/></disp-formula><p>Finally, the general solution is given by</p><disp-formula id="scirp.72118-formula137"><label>(45)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x106.png"  xlink:type="simple"/></disp-formula><p>Moreover, since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x107.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.72118-formula138"><label>(46)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x108.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x109.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x110.png" xlink:type="simple"/></inline-formula>, we obtain then</p><disp-formula id="scirp.72118-formula139"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x111.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x112.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x113.png" xlink:type="simple"/></inline-formula> are as defined above.</p></sec><sec id="s5"><title>5. Monetary Interventions</title><p>The next task is to definitize the coefficients A and B. To do that, we consider different types of central bank interventions. As before, we consider a target zone<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x114.png" xlink:type="simple"/></inline-formula>. Introducing a target zone of this sort defines the fundamentals as a regulated Brownian motion. The point of the matter is that whenever the exchange rate falls within the band, the central bank or the monetary authorities do not intervene. Whenever the fundamentals touch one of the bands, the authorities do intervene. In the next section, we will consider the most widely used types of interventions we have previously examined such as Krugman’s infinitesimal marginal intervention [<xref ref-type="bibr" rid="scirp.72118-ref6">6</xref>] , Flood-Garber interventions [<xref ref-type="bibr" rid="scirp.72118-ref19">19</xref>] , and interventions in the sense of Bertola and Caballero [<xref ref-type="bibr" rid="scirp.72118-ref10">10</xref>] . Each type of interventions leads to different estimates of the integration coefficients A and B.</p><sec id="s5_1"><title>5.1. Krugman’s Type Interventions</title><p>As we have previously mentioned, Krugman infinitesimal marginal interventions assume that the monetary authorities intervene in the foreign exchange market so as to prevent the exchange rate from ever leaving the target zone band. At the time of interventions,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x115.png" xlink:type="simple"/></inline-formula>. “Smooth-pasting” conditions imply that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x116.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x117.png" xlink:type="simple"/></inline-formula>. These two boundary conditions are sufficient to determine or definitize the constants of integration A and B. We have the following result which we will state as a corollary.</p><p>Corollary 2. Under Krugman interventions and with a geometric brownian motion for the fundamentals:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x118.png" xlink:type="simple"/></inline-formula>, the exchange rate series, s(t), is given by</p><disp-formula id="scirp.72118-formula140"><label>(47)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x119.png"  xlink:type="simple"/></disp-formula><p>where A and B are given by</p><disp-formula id="scirp.72118-formula141"><label>(48)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x120.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula142"><label>(49)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x121.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula143"><label>(50)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x122.png"  xlink:type="simple"/></disp-formula><p>Furthermore, assuming symmetry, in the sense that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x123.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x124.png" xlink:type="simple"/></inline-formula>, then we have</p><disp-formula id="scirp.72118-formula144"><label>(51)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x125.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula145"><label>(52)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x126.png"  xlink:type="simple"/></disp-formula><p>Proof. We have</p><disp-formula id="scirp.72118-formula146"><label>(53)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x127.png"  xlink:type="simple"/></disp-formula><p>“Smooth-pasting” conditions imply</p><disp-formula id="scirp.72118-formula147"><label>(54)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x128.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula148"><label>(55)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x129.png"  xlink:type="simple"/></disp-formula><p>We obtain</p><disp-formula id="scirp.72118-formula149"><label>(56)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x130.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula150"><label>(57)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x131.png"  xlink:type="simple"/></disp-formula><p>For the symmetric case, we target zone becomes <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x132.png" xlink:type="simple"/></inline-formula> so that the zone is symmetric about zero. We have</p><disp-formula id="scirp.72118-formula151"><label>(58)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x133.png"  xlink:type="simple"/></disp-formula><p>A similar expression is obtained for B</p><disp-formula id="scirp.72118-formula152"><label>(59)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x134.png"  xlink:type="simple"/></disp-formula><p>Also, in the symmetric case, we have</p><disp-formula id="scirp.72118-formula153"><label>(60)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x135.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula154"><label>(61)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x136.png"  xlink:type="simple"/></disp-formula></sec><sec id="s5_2"><title>5.2. Flood-Garber Interventions</title><p>It is widely accepted in the literature that discrete interventions are more realistic than infinitesimal marginal interventions &#224; la Krugman due to the fact that the central bank starts with a fixed amount of reserves which will eventually be exhausted [<xref ref-type="bibr" rid="scirp.72118-ref19">19</xref>] . In this section, we discuss the behavior of the exchange rate in the case of discrete interventions &#224; la Flood-Garber. This type of intervention assumes perfect credibility of the zone from the point of view of market participants. We start by rewriting the exchange rate function as follows</p><disp-formula id="scirp.72118-formula155"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x137.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x138.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x139.png" xlink:type="simple"/></inline-formula>. That is, we obtain</p><disp-formula id="scirp.72118-formula156"><label>(62)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x140.png"  xlink:type="simple"/></disp-formula><p>The monetary authorities intervene in the foreign exchange market whenever f hits either the upper or lower bound of the target zone by placing the fundamental back in the middle of the band.</p><disp-formula id="scirp.72118-formula157"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x141.png"  xlink:type="simple"/></disp-formula><p>When the fundamentals hit the lower band <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x142.png" xlink:type="simple"/></inline-formula> at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x143.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.72118-formula158"><label>(63)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x144.png"  xlink:type="simple"/></disp-formula><p>At time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x145.png" xlink:type="simple"/></inline-formula>, market participants know with certainty that the monetary authori-</p><p>ties will reset f at the middle of the band, that is, at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x146.png" xlink:type="simple"/></inline-formula>.</p><p>Hence,</p><disp-formula id="scirp.72118-formula159"><label>(64)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x147.png"  xlink:type="simple"/></disp-formula><p>UIP implies no jumps and therefore</p><disp-formula id="scirp.72118-formula160"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x148.png"  xlink:type="simple"/></disp-formula><p>That is,</p><disp-formula id="scirp.72118-formula161"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x149.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula162"><label>(65)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x150.png"  xlink:type="simple"/></disp-formula><p>Similarly, at the instant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x151.png" xlink:type="simple"/></inline-formula> where the fundamentals hit the upper bound of the target zone,</p><disp-formula id="scirp.72118-formula163"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x152.png"  xlink:type="simple"/></disp-formula><p>we see that</p><disp-formula id="scirp.72118-formula164"><label>(66)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x153.png"  xlink:type="simple"/></disp-formula><p>At the next instant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x154.png" xlink:type="simple"/></inline-formula>, we have, as before</p><disp-formula id="scirp.72118-formula165"><label>(67)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x155.png"  xlink:type="simple"/></disp-formula><p>That is,</p><disp-formula id="scirp.72118-formula166"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x156.png"  xlink:type="simple"/></disp-formula><p>Equivalently, we can write</p><disp-formula id="scirp.72118-formula167"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x157.png"  xlink:type="simple"/></disp-formula><p>We obtain the following system of linear equations</p><disp-formula id="scirp.72118-formula168"><label>(68)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x158.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula169"><label>(69)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x159.png"  xlink:type="simple"/></disp-formula><p>To solve the system, we set</p><disp-formula id="scirp.72118-formula170"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x160.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula171"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x161.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula172"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x162.png"  xlink:type="simple"/></disp-formula><p>The solution to the system is therefore obtained as</p><disp-formula id="scirp.72118-formula173"><label>(70)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x163.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula174"><label>(71)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x164.png"  xlink:type="simple"/></disp-formula><p>The complete solution to the model under Flood-Garber interventions can be summarized in the following proposition</p><p>Proposition 3. Under Flood-Garber interventions, the solution to the target zone model is given by</p><disp-formula id="scirp.72118-formula175"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x165.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.72118-formula176"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x166.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula177"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x167.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula178"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x168.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula179"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x169.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula180"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x170.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula181"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x171.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula182"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x172.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula183"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x173.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula184"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x174.png"  xlink:type="simple"/></disp-formula><p>To complete the discussion under this type of interventions, we consider the symmetric case. This has only a theoretical value given that for our model, the fundamentals are either positive or negative.</p><p>Suppose that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x175.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x176.png" xlink:type="simple"/></inline-formula> so that the target zone is symmetric about zero. Then, it follows that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x177.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x178.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x179.png" xlink:type="simple"/></inline-formula>. Also,</p><disp-formula id="scirp.72118-formula185"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x180.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula186"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x181.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula187"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x182.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula188"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x183.png"  xlink:type="simple"/></disp-formula><p>We present below a possible graph (<xref ref-type="fig" rid="fig1">Figure 1</xref>) for the exchange under some specific value of the target zone band.</p></sec><sec id="s5_3"><title>5.3. Bertola-Caballero Interventions</title><p>This type of intervention is justified by the fact that the monetary authorities start with a fixed amount of reserves which will eventually be exhausted and hence the target zone cannot be completely credible. Therefore, the assumption of perfect credibility is relaxed here. When the exchange rate hits either band limits, the monetary authorities either realign or mount a defense of the zone. Let p be the probability of realignment and 1 − p the probability that the monetary authorities mount a target zone defense. Suppose further that the fundamentals hit the upper bound,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x184.png" xlink:type="simple"/></inline-formula>. At time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x185.png" xlink:type="simple"/></inline-formula> when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x186.png" xlink:type="simple"/></inline-formula> is hit, we have</p><disp-formula id="scirp.72118-formula189"><label>(72)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x187.png"  xlink:type="simple"/></disp-formula><p>At the next instant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x188.png" xlink:type="simple"/></inline-formula>, we have</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Relationship between f and s when f follows a GBM and Flood- Garber interventions</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-1490487x189.png"/></fig><p>1) With realignment (with probability p), we have a new band <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x190.png" xlink:type="simple"/></inline-formula> and</p><disp-formula id="scirp.72118-formula190"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x191.png"  xlink:type="simple"/></disp-formula><p>2) If a defense is mounted, then the monetary authorities place the fundamentals back to the middle of the band:</p><disp-formula id="scirp.72118-formula191"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x192.png"  xlink:type="simple"/></disp-formula><p>Uncovered interest parity implies</p><disp-formula id="scirp.72118-formula192"><label>(73)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x193.png"  xlink:type="simple"/></disp-formula><p>But, it is seen that</p><disp-formula id="scirp.72118-formula193"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x194.png"  xlink:type="simple"/></disp-formula><p>As before, UIP implies</p><disp-formula id="scirp.72118-formula194"><label>(74)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x195.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.72118-formula195"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x196.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula196"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x197.png"  xlink:type="simple"/></disp-formula><p>Now we consider the case where f hits the lower bound at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x198.png" xlink:type="simple"/></inline-formula>. Then</p><disp-formula id="scirp.72118-formula197"><label>(75)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x199.png"  xlink:type="simple"/></disp-formula><p>If realignment occurs, then at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x200.png" xlink:type="simple"/></inline-formula>, we have a new band <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x201.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.72118-formula198"><label>(76)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x202.png"  xlink:type="simple"/></disp-formula><p>If a defense is mounted, then we obtain</p><disp-formula id="scirp.72118-formula199"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x203.png"  xlink:type="simple"/></disp-formula><p>This implies that</p><disp-formula id="scirp.72118-formula200"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x204.png"  xlink:type="simple"/></disp-formula><p>As before, UIP implies that exchange rate does not jump so that</p><disp-formula id="scirp.72118-formula201"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x205.png"  xlink:type="simple"/></disp-formula><p>We can rearrange this equation to obtain</p><disp-formula id="scirp.72118-formula202"><label>(77)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x206.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.72118-formula203"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x207.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula204"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x208.png"  xlink:type="simple"/></disp-formula><p>Finally, we consider the symmetric case. Suppose that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x209.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x210.png" xlink:type="simple"/></inline-formula>, so that the target band is symmetric about zero. Then, we have</p><disp-formula id="scirp.72118-formula205"><label>(78)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x211.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula206"><label>(79)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x212.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula207"><label>(80)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x213.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula208"><label>(81)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x214.png"  xlink:type="simple"/></disp-formula><p>These results are summarized in the following proposition.</p><p>Proposition 4. Under Flood-Garber interventions, the solution to the target zone model is given by</p><disp-formula id="scirp.72118-formula209"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x215.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.72118-formula210"><label>(82)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x216.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula211"><label>(83)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x217.png"  xlink:type="simple"/></disp-formula><p>and as given above</p><disp-formula id="scirp.72118-formula212"><label>(84)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x218.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula213"><label>(85)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x219.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula214"><label>(86)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1490487x220.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula215"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x221.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula216"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x222.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula217"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x223.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72118-formula218"><graphic  xlink:href="http://html.scirp.org/file/11-1490487x224.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x225.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x226.png" xlink:type="simple"/></inline-formula> are as before.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> SMM estimates of the Flood-Garber target zone model for Japan</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Parameter</th><th align="center" valign="middle" >estimate</th><th align="center" valign="middle" >t-statistic</th><th align="center" valign="middle" >J-Statistic</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x227.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.0728</td><td align="center" valign="middle" >2.2338</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x228.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.3257</td><td align="center" valign="middle" >4.8284</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x229.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >6.253</td><td align="center" valign="middle" >3.7351</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x230.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.2594</td><td align="center" valign="middle" >2.1443</td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x231.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >5.2138</td><td align="center" valign="middle" >2.8573</td><td align="center" valign="middle" ></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" >2.9744</td></tr></tbody></table></table-wrap></sec></sec><sec id="s6"><title>6. Estimation Results of the Model’s Parameters</title><p>In this section, we present some estimates of the model’s parameters for the Krugman’s and Flood-Garber’s types of interventions. We use Daily exchange rate data for Japan and Sweden from 1987 to 1990. Though the data are relatively old, we use it to illustrate the findings that the model gives some satisfactory results contrary the basic target zones models in the literature. The estimation technique being used is the Simulated Method of Moments (SMM) procedure [<xref ref-type="bibr" rid="scirp.72118-ref17">17</xref>] . Our task here is to estimate the parameters<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x232.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x233.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x234.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x235.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1490487x236.png" xlink:type="simple"/></inline-formula> of the model. We obtain the following estimates for Japan data (<xref ref-type="table" rid="table2">Table 2</xref>).</p><p>As indicated by the table, the estimates are quite reasonable in magnitude and, as expected, have the correct signs. Moreover, the J-Statistic of the one overidentifying restriction is not rejected and therefore the model does a good job in fitting the data, at the most commonly used significance levels.</p><p>We also found that the model does not perform well in the case for the Krugman marginal interventions. The estimates are reasonable in signs and magnitudes. However, the high value of the J-Statistics indicates that the model is not supported by the data. In essence, this can be due to the fact that it is commonly not easy to estimate these models efficiently.</p></sec><sec id="s7"><title>7. Conclusion</title><p>In this paper, we have derived analytical or closed form expressions for the exchange rate function under the assumption that the fundamentals follow a geometric Brownian motion within the target zone band. Preliminary estimates from Simulated Method of Moments (SMM) show that the data do not show great support for the Krugman infinitesimal marginal interventions in the foreign exchange market, as indicated by the high value of the J-statistic. However, we found strong evidence for the target zone model for Flood-Garber interventions for the case of Japan, as indicated by the low value of the J-statistic. This indicates that it is likely that Japan has used an unofficial exchange rate target zone band during the 1987-1990 period. This is not a surprise due to the fact that central banks do not often reveal their intervention strategies. No such evidence has been found for the case of Germany.</p></sec><sec id="s8"><title>Cite this paper</title><p>Cupidon, J.R. and Hyppolite, J. (2016) A Target Zone Model Where the Fundamentals Follow a Geometric Brownian Motion. Journal of Mathematical Finance, 6, 866-886. http://dx.doi.org/10.4236/jmf.2016.65058</p></sec></body><back><ref-list><title>References</title><ref id="scirp.72118-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Mark, N.C. (2001) International Macroeconomics and Finance: Theory and Econometric Methods. Wiley-Blackwell.</mixed-citation></ref><ref id="scirp.72118-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">De Jong, F. (1994) A Univariate Analysis of EMS Exchange Rate Using a Target Zone Model. 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