<?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.2015.311005</article-id><article-id pub-id-type="publisher-id">JSS-61332</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>
 
 
  A Note on the Kou’s Continuity Correction Formula
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ting</surname><given-names>Liu</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>Chang</surname><given-names>Feng</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yanqiong</surname><given-names>Lu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Bei</surname><given-names>Yao</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>School of Mathematic and Statistic, Huazhong University of Science and Technology, Wuhan, China</addr-line></aff><aff id="aff1"><addr-line>School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan, China</addr-line></aff><pub-date pub-type="epub"><day>11</day><month>11</month><year>2015</year></pub-date><volume>03</volume><issue>11</issue><fpage>28</fpage><lpage>34</lpage><history><date date-type="received"><day>October</day>	<month>2015</month>	</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 article introduces a hyper-exponential jump diffusion process based on the continuity correction for discrete barrier options under the standard B-S model, using measure transformation and stopping time theory to prove the correction, thus broadening the conditions of the continuity correction of Kou. 
 
</p></abstract><kwd-group><kwd>B-S Model</kwd><kwd> Discrete Barrier Options</kwd><kwd> Hyper-Exponential Jump Diffusion</kwd><kwd> Continuity Correction Formula</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In 2003, S. G. Kou [<xref ref-type="bibr" rid="scirp.61332-ref1">1</xref>] generalized a double exponential jump diffusion model into the pricing of continuity single barrier options. They analyzed the joint distribution of the final asset price by focusing on first passage time and combining it with the nonlinear renewal theory of the time series analysis. The Laplace transforms and the non-memory property of exponential distribution were also used during the analyzing process. In his article which was published in 1997, Kou [<xref ref-type="bibr" rid="scirp.61332-ref2">2</xref>]-[<xref ref-type="bibr" rid="scirp.61332-ref4">4</xref>] put forward a continuity correction of B-S model, which combined the pricing method of continuity barrier options with that of discrete barrier options. In 2013, D. Jun [<xref ref-type="bibr" rid="scirp.61332-ref5">5</xref>] generalized the continuity correction formula into the double barrier options in view of Kou’s report. Also in 2013, C. D. Fuh [<xref ref-type="bibr" rid="scirp.61332-ref6">6</xref>] introduced the double exponential jump diffusion model to the pricing of discrete single barrier options and look-back options. His article widened the conditions of the continuity correction formula of Kou and obtained a correction formula of discrete barrier options based on the double exponential jump diffusion process.</p><p>This article uses Kou’s theoretical derivation method for the first passage time and C. D. Fuh’s thought of proving the correction formula based on double exponential jump diffusion model for reference. In order to generalize the model into the pricing of both the discrete single and double barrier options on the basis of the hyper-exponential jump diffusion process, we combine the correction formula of discrete single barrier options raised by Kou with D. Jun’s correction of discrete double barrier options under the B-S model. Although formally, the correction formula in this article seems to be same as Kou’s and D. Jun’s, there are no restrictions of strike price K and barrier value H in the correction formula in this passage, which means that the scope of application of Kou’s and D. Jun’s correction are widened. Additionally, compared with the double exponential jump diffusion model of C. D. Fuh, the hyper-exponential jump diffusion model in this article is more general.</p></sec><sec id="s2"><title>2. Pricing on Barrier Options</title><sec id="s2_1"><title>2.1. Continuity Correction Model</title><p>In 1997, Steven Kou put forward the concept of continuity correction in his paper, which combined the continuity barrier options with the discrete barrier options through the continuity correction formula. Denote the stopping time by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x4.png" xlink:type="simple"/></inline-formula>, the definition goes as follows:</p><disp-formula id="scirp.61332-formula154"><label>(2.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x5.png"  xlink:type="simple"/></disp-formula><p>or</p><disp-formula id="scirp.61332-formula155"><label>(2.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x6.png"  xlink:type="simple"/></disp-formula><p>Here H stands for the barrier level and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x7.png" xlink:type="simple"/></inline-formula> is the frequency of monitoring. Formula (2.1) and (2.2) represent the situation of continuously monitored and discretely monitored, respectively. Apparently, an up model has <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x8.png" xlink:type="simple"/></inline-formula> and a down model has<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x9.png" xlink:type="simple"/></inline-formula>. For convenience, we assume the risk-neutral interest rate r is a constant in this case. Because of the existence of jump, the “market” here is not a complete market, which means that the risk neutrality measure is not unique (more details can be found in Kou [<xref ref-type="bibr" rid="scirp.61332-ref7">7</xref>]). As a matter of convenience, we assume the risk neutrality measure Q just needs to meet the premise of rational expected equilibrium.</p><p>Kou has pointed out in his article that when m is large enough, which means<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x10.png" xlink:type="simple"/></inline-formula>, Formula (2.2) is weakly convergent to Formula (2.1). However, with the increasing of m, the convergence rate will become very slow and the error will also increase. To solve this problem, Kou implemented methods of time series analysis, which could provide limitations of K and H, and established correction formula as follow, based on the B-S model to fasten the convergence rate:</p><disp-formula id="scirp.61332-formula156"><label>(2.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x11.png"  xlink:type="simple"/></disp-formula><p>If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x12.png" xlink:type="simple"/></inline-formula>, “+” will be applied, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x13.png" xlink:type="simple"/></inline-formula>, “−” will be applied.</p><p>Here, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x14.png" xlink:type="simple"/></inline-formula>, with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x15.png" xlink:type="simple"/></inline-formula> standing for Riemann zeta function, which can be concretely written as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x16.png" xlink:type="simple"/></inline-formula>.This method of adjustment is called continuity correction.</p><p>According to the correction formula, we could find that the barrier-crossing probability will be lower after the adjustment of discretely monitored barrier. The amount of the adjustment is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x17.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s2_2"><title>2.2. Hyper-Exponential Jump Diffusion Model</title><p>We assume that under the risk neutrality measure Q, the asset price <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x18.png" xlink:type="simple"/></inline-formula> will obey the following hyper-expo- nential jump diffusion geometric Brownian motion model:</p><disp-formula id="scirp.61332-formula157"><label>(2.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x19.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61332-formula158"><label>(2.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x20.png"  xlink:type="simple"/></disp-formula><p>Here <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x21.png" xlink:type="simple"/></inline-formula> is a standard Brownian motion, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x22.png" xlink:type="simple"/></inline-formula>is a Poisson process with intensity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x23.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x24.png" xlink:type="simple"/></inline-formula>stands for the underlying asset price at previous moment, and constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x25.png" xlink:type="simple"/></inline-formula> represent the risk-free interest</p><p>rate, dividend rate and risk volatility, respectively. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x26.png" xlink:type="simple"/></inline-formula>is a sequence of independent identically distributed random variables, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x27.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x28.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.61332-formula159"><label>(2.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x29.png"  xlink:type="simple"/></disp-formula><p>Using Ito lemma and theories of calculation of stochastic partial differential equations, the solution of model (2.4) under continuously monitored situation is:</p><disp-formula id="scirp.61332-formula160"><label>(2.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x30.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x31.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x32.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x33.png" xlink:type="simple"/></inline-formula>.</p><p>It’s obvious that, when we assume the discretely monitored time interval is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x34.png" xlink:type="simple"/></inline-formula>, the discretely monitored asset price is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x35.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x36.png" xlink:type="simple"/></inline-formula>at the nth time of monitoring. As a result,</p><disp-formula id="scirp.61332-formula161"><label>(2.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x37.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x38.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x39.png" xlink:type="simple"/></inline-formula>. All random variables here are independent. Now we suppose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x40.png" xlink:type="simple"/></inline-formula> is the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x41.png" xlink:type="simple"/></inline-formula>algebra, consequently, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x42.png" xlink:type="simple"/></inline-formula>will still be a Q-martingale. Take the continuous up-in-put options for example, the option return is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x43.png" xlink:type="simple"/></inline-formula>, and the corresponding discrete situation is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x44.png" xlink:type="simple"/></inline-formula>. We use <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x45.png" xlink:type="simple"/></inline-formula> to replace <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x46.png" xlink:type="simple"/></inline-formula> for more explicit expression. Therefore, equations (2.1), (2.2) could be written as:</p><disp-formula id="scirp.61332-formula162"><label>(2.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x47.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x48.png" xlink:type="simple"/></inline-formula>.</p><p>Now we try to find the relationship between this two joint distribution densities, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x49.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x50.png" xlink:type="simple"/></inline-formula>. For (2.7) and (2.8), define<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x51.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x52.png" xlink:type="simple"/></inline-formula>. According to the L&#233;vy-Khintchine formula, the characteristic function can be expressed as</p><disp-formula id="scirp.61332-formula163"><graphic  xlink:href="http://html.scirp.org/file/61332x53.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61332-formula164"><label>(2.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x54.png"  xlink:type="simple"/></disp-formula><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x55.png" xlink:type="simple"/></inline-formula> be the corresponding characteristic function of jump size J, and the cumulative generating function is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x56.png" xlink:type="simple"/></inline-formula> (namely<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x57.png" xlink:type="simple"/></inline-formula>). Therefore,</p><disp-formula id="scirp.61332-formula165"><label>(2.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x58.png"  xlink:type="simple"/></disp-formula><p>For convenience, we use <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x59.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x60.png" xlink:type="simple"/></inline-formula> to replace <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x61.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x62.png" xlink:type="simple"/></inline-formula>, respectively. Denote<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x63.png" xlink:type="simple"/></inline-formula>, and now we provide the corresponding Laplace transform.</p><p>Proposition 2.1. [<xref ref-type="bibr" rid="scirp.61332-ref8">8</xref>] For hyper-exponential jump diffusion model (2.4) and (2.5), when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x64.png" xlink:type="simple"/></inline-formula>, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x65.png" xlink:type="simple"/></inline-formula>, the Laplace operator of stopping time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x66.png" xlink:type="simple"/></inline-formula> can be written as follows:</p><disp-formula id="scirp.61332-formula166"><label>(2.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x67.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x68.png" xlink:type="simple"/></inline-formula> is uniquely determined by linear equations <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x69.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x70.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x71.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x72.png" xlink:type="simple"/></inline-formula>.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x73.png" xlink:type="simple"/></inline-formula>.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x74.png" xlink:type="simple"/></inline-formula>. What’s more,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x75.png" xlink:type="simple"/></inline-formula>. In view of proposition 2.1, we can obtain the probability distribution of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x76.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.61332-formula167"><label>(2.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x77.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_3"><title>2.3. Pricing on Discrete Single Barrier Options</title><p>In this section, based on the discrete model (2.8), firstly, we make an adjustment on the discrete model<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x78.png" xlink:type="simple"/></inline-formula>, denote<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x79.png" xlink:type="simple"/></inline-formula>, then `<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x80.png" xlink:type="simple"/></inline-formula>. As a result,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x81.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x82.png" xlink:type="simple"/></inline-formula>,</p><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x83.png" xlink:type="simple"/></inline-formula>. So we can have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x84.png" xlink:type="simple"/></inline-formula>.</p><p>The preparation has been done, however, two preparatory lemmas will be introduced before finally exhibit the main conclusion.</p><p>Lemma 2.2. For continuously monitored stopping time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x85.png" xlink:type="simple"/></inline-formula>, discretely monitored stopping time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x86.png" xlink:type="simple"/></inline-formula> (Formula (2.9)), maturity T and monitoring time interval<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x87.png" xlink:type="simple"/></inline-formula>, when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x88.png" xlink:type="simple"/></inline-formula>, the following equation is satisfied for arbitrary constant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x89.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.61332-formula168"><label>(2.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x90.png"  xlink:type="simple"/></disp-formula><p>Proof: Assume (2.14) is a true statement, in view of (2.12) and (2.13), when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x91.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.61332-formula169"><label>(2.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x92.png"  xlink:type="simple"/></disp-formula><p>From proposition 2.1, the equation above will be true if the following equation is proved:</p><disp-formula id="scirp.61332-formula170"><label>(2.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x93.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x94.png" xlink:type="simple"/></inline-formula>. To prove this formula, for an arbitrary constant b &gt; 0 and constant h &gt; 0, define a function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x95.png" xlink:type="simple"/></inline-formula>, satisfy<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x96.png" xlink:type="simple"/></inline-formula>, which can be written as :</p><disp-formula id="scirp.61332-formula171"><label>(2.17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x97.png"  xlink:type="simple"/></disp-formula><p>In order to obtain Equation (2.15), here, we solve this problem by adjusting Kou’s method of the first passage time under the double exponential jump diffusion process. Noticing that</p><disp-formula id="scirp.61332-formula172"><label>(2.18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x98.png"  xlink:type="simple"/></disp-formula><p>where L stands for the infinitesimal generator</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x99.png" xlink:type="simple"/></inline-formula> (2.19).</p><p>Here, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x100.png" xlink:type="simple"/></inline-formula>is supposed to be twice continuously differentiable. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x101.png" xlink:type="simple"/></inline-formula>, we use formula <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x102.png" xlink:type="simple"/></inline-formula> to construct a series of function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x103.png" xlink:type="simple"/></inline-formula>, As a result, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x104.png" xlink:type="simple"/></inline-formula>, there are<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x105.png" xlink:type="simple"/></inline-formula>. Then combining (2.18) and (2.19), for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x106.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.61332-formula173"><graphic  xlink:href="http://html.scirp.org/file/61332x107.png"  xlink:type="simple"/></disp-formula><p>As<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x108.png" xlink:type="simple"/></inline-formula>, for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x109.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.61332-formula174"><label>(2.20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x110.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x111.png" xlink:type="simple"/></inline-formula>. And because <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x112.png" xlink:type="simple"/></inline-formula> is a constant, we can obtain that</p><disp-formula id="scirp.61332-formula175"><label>(2.21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x113.png"  xlink:type="simple"/></disp-formula><p>Focusing on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x114.png" xlink:type="simple"/></inline-formula>, we implement formula <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x115.png" xlink:type="simple"/></inline-formula> and combine (2.21), for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x116.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.61332-formula176"><label>(2.22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x117.png"  xlink:type="simple"/></disp-formula><p>is the local martingale and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x118.png" xlink:type="simple"/></inline-formula>. According to the definition, there are a series of stopping time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x119.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x120.png" xlink:type="simple"/></inline-formula> as well. Therefore, for every<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x121.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x122.png" xlink:type="simple"/></inline-formula>is a martingale. And according to Lebesgue’s dominated convergence theorem,</p><disp-formula id="scirp.61332-formula177"><graphic  xlink:href="http://html.scirp.org/file/61332x123.png"  xlink:type="simple"/></disp-formula><p>more precisely,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x124.png" xlink:type="simple"/></inline-formula>,</p><p>and in view of (2.21)</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x125.png" xlink:type="simple"/></inline-formula>.</p><p>If we integrate the three formulas above, for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x126.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x127.png" xlink:type="simple"/></inline-formula>,</p><p>Now for convenience, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x128.png" xlink:type="simple"/></inline-formula>is used to replace<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x129.png" xlink:type="simple"/></inline-formula>. Based on Kubilius [<xref ref-type="bibr" rid="scirp.61332-ref9">9</xref>], let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x130.png" xlink:type="simple"/></inline-formula>, when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x131.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x132.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.61332-formula178"><graphic  xlink:href="http://html.scirp.org/file/61332x133.png"  xlink:type="simple"/></disp-formula><p>As <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x134.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x135.png" xlink:type="simple"/></inline-formula> are asymptotically independent, when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x136.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.61332-formula179"><label>(2.23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x137.png"  xlink:type="simple"/></disp-formula><p>which obeys Taylor expansion of the first order and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x138.png" xlink:type="simple"/></inline-formula>. Here we use Kou’s treatment of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x139.png" xlink:type="simple"/></inline-formula> for reference and define random walk</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x140.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x141.png" xlink:type="simple"/></inline-formula></p><p>When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x142.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.61332-formula180"><label>(2.24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x143.png"  xlink:type="simple"/></disp-formula><p>Lemma 2.2 can be proved by substituting (2.24) and (2.16) into (2.15).</p><p>Lemma 2.3. For discrete barrier options with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x144.png" xlink:type="simple"/></inline-formula> times of monitoring and value of barrier H, there are stopping time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x145.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x146.png" xlink:type="simple"/></inline-formula>(for convenience, denote<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x147.png" xlink:type="simple"/></inline-formula>), and their corresponding logarithm underlying asset prices<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x148.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x149.png" xlink:type="simple"/></inline-formula>(Formula (2.8)). For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x150.png" xlink:type="simple"/></inline-formula> (Formula (2.11)), the joint distribution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x151.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x152.png" xlink:type="simple"/></inline-formula> meet the following equation:</p><disp-formula id="scirp.61332-formula181"><label>(2.25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x153.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x154.png" xlink:type="simple"/></inline-formula>.</p><p>Proof:</p><disp-formula id="scirp.61332-formula182"><graphic  xlink:href="http://html.scirp.org/file/61332x155.png"  xlink:type="simple"/></disp-formula><p>On the basis of proposition 2.1 in Kou [<xref ref-type="bibr" rid="scirp.61332-ref1">1</xref>] and Zhang [<xref ref-type="bibr" rid="scirp.61332-ref10">10</xref>], <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x156.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x157.png" xlink:type="simple"/></inline-formula> are asymptotically independent, denote<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x158.png" xlink:type="simple"/></inline-formula>.</p><p>When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x159.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x160.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.61332-formula183"><graphic  xlink:href="http://html.scirp.org/file/61332x161.png"  xlink:type="simple"/></disp-formula><p>Therefore,</p><disp-formula id="scirp.61332-formula184"><label>(2.26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x162.png"  xlink:type="simple"/></disp-formula><p>Then lemma 2.3 can be proved by using corollary 3.3 in Kou [<xref ref-type="bibr" rid="scirp.61332-ref4">4</xref>].</p><p>Theorem 2.1. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x163.png" xlink:type="simple"/></inline-formula> denote the price of continuously monitored options with barrier value H, accordingly, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x164.png" xlink:type="simple"/></inline-formula>is the price of discretely monitored options with the monitoring frequency<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x165.png" xlink:type="simple"/></inline-formula>. Consequently, for an arbitrary discrete barrier option with maturity T, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x166.png" xlink:type="simple"/></inline-formula>, and when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x167.png" xlink:type="simple"/></inline-formula>, we obtain the following correction formula:</p><disp-formula id="scirp.61332-formula185"><label>(2.27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/61332x168.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x169.png" xlink:type="simple"/></inline-formula>, with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x170.png" xlink:type="simple"/></inline-formula> the Riemann zeta function.</p><p>The proof of the theorem can be derived directly from Lemma 2.2 and 2.3. What we need to illustrate is that although the conclusion here seems to be similar to Kou [<xref ref-type="bibr" rid="scirp.61332-ref2">2</xref>]’s, there are no restriction of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x171.png" xlink:type="simple"/></inline-formula> (upward) and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/61332x172.png" xlink:type="simple"/></inline-formula> (downward) for the striking price K and barrier H.</p></sec></sec><sec id="s3"><title>Cite this paper</title><p>Ting Liu,Chang Feng,Yanqiong Lu,Bei Yao, (2015) A Note on the Kou’s Continuity Correction Formula. Open Journal of Social Sciences,03,28-34. doi: 10.4236/jss.2015.311005</p></sec></body><back><ref-list><title>References</title><ref id="scirp.61332-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Kou, S.G. (2003) First Passage Times of a Jump Diffusion Process. Advances in Applied Probability, 35, 504-531. 
http://dx.doi.org/10.1239/aap/1051201658</mixed-citation></ref><ref id="scirp.61332-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Kou, S. (1997) A Continuity Correction for Discrete Barrier Options. Mathematical Finance, 7, 325-348. 
http://dx.doi.org/10.1111/1467-9965.00035</mixed-citation></ref><ref id="scirp.61332-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Broadie, M., Glasserman, P. and Kou, S.G. (1999) Connecting Discrete and Continuous Path-Dependent Options. Finance Stochastic, 3, 55-82. http://dx.doi.org/10.1007/s007800050052</mixed-citation></ref><ref id="scirp.61332-ref4"><label>4</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Kou</surname><given-names> S.G. </given-names></name>,<etal>et al</etal>. (<year>2003</year>)<article-title>On Pricing of Discrete Barrier Options</article-title><source> Statistic Sinica</source><volume> 13</volume>,<fpage> 955</fpage>-<lpage>964</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.61332-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Jun, D. (2013) Continuity Correction for Discrete Barrier Options with Two Barriers. Journal of Computational and Applied Mathematics, 237, 520-528. http://dx.doi.org/10.1016/j.cam.2012.06.021</mixed-citation></ref><ref id="scirp.61332-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Fuh, C.D., Luo, S.F. and Yen, J.F. (2013) Pricing Discrete Path-Dependent Options under a Double Exponential Jump- Diffusion Model. Journal of Banking &amp; Finance, 37, 2702-2713. http://dx.doi.org/10.1016/j.jbankfin.2013.03.023</mixed-citation></ref><ref id="scirp.61332-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Kou, S.G. (2002) A Jump-Diffusion Model for Option Pricing. Management Science, 48, 1086-1101. 
http://dx.doi.org/10.1287/mnsc.48.8.1086.166</mixed-citation></ref><ref id="scirp.61332-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Cai, N. (2009) On First Passage Times of a Hyper-Exponential Jump Diffusion Process. Operations Research Letters, 37, 127-134. http://dx.doi.org/10.1016/j.orl.2009.01.002</mixed-citation></ref><ref id="scirp.61332-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Thakoor, N., Tangman, D.Y. and Bhuruth, M. (2014) Efficient and High Accuracy Pricing of Barrier Options under the CEV Diffusion. Journal of Computational and Applied Mathematics, 259, 182-193. 
http://dx.doi.org/10.1016/j.cam.2013.05.009</mixed-citation></ref><ref id="scirp.61332-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Zhang, C.H. (1988) A Nonlinear Renewal Theory. Annals of Probability, 6, 93-824.  
http://dx.doi.org/10.1214/aop/1176991788</mixed-citation></ref></ref-list></back></article>