<?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.2012.24032</article-id><article-id pub-id-type="publisher-id">JMF-24550</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>
 
 
  Closed-Form Approximate Solutions of Window Barrier Options with Term-Structure Volatility and Interest Rates Using the Boundary Integral Method
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>i-Long</surname><given-names>Hsiao</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Finance, National Dong Hwa University, Hualien, Taiwan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>hsiao@mail.ndhu.edu.tw</email></corresp></author-notes><pub-date pub-type="epub"><day>19</day><month>11</month><year>2012</year></pub-date><volume>02</volume><issue>04</issue><fpage>291</fpage><lpage>302</lpage><history><date date-type="received"><day>August</day>	<month>8,</month>	<year>2012</year></date><date date-type="rev-recd"><day>September</day>	<month>10,</month>	<year>2012</year>	</date><date date-type="accepted"><day>September</day>	<month>22,</month>	<year>2012</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this study we propose an approach to solve a partial differential equation (PDE), the boundary integral method, for the valuation of both discrete and continuous window barrier options, as well as multi-window barrier options within a deterministic term structure of volatility and interest rates. Numerical results reveal that the proposed method yields rapid and highly accurate closed-form approximate solutions. In addition, the term structure will have a significant impact on the valuation.
 
</p></abstract><kwd-group><kwd>Window Barrier Option; Integral Method; Integral Representation; Green’s Function; PDE Approach</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Barrier options are widely used and traded in financial markets to manage the risk related to foreign exchange, interest rates, and equity in the global market. A barrier option is a path-dependent option that is activated (i.e. knocked in), or extinguished (i.e. knocked out) when the price of the underlying asset breaches the pre-specified barrier level at any time before maturity. There are two main reasons for the prevalence of barrier options. First, barrier options are useful for limiting the risk exposure of clients, specifically in the foreign exchange market. Second, barrier options are cheaper than vanilla options with similar attributes. Therefore, they are more affordable financial instruments that can match investors’ views regarding the degree of volatility in the underlying asset price change. Additionally, they offer an appropriate level of downside protection for hedging purposes. For example, if long hedgers believe that only a mild volatility exists in the market over a given period, the hedgers will prefer to buy a knock-out option with fewer premiums than to pay the full premium for a plain vanilla option. Alternatively, when speculators believe that the price change will be volatile for a period of time, they will prefer to purchase a knock-in option rather than to obtain the plain option with a higher price. Since an ordinary option can be decomposed into two otherwise identical knock-in and knock-out options, this feature makes the barrier option a highly suitable instrument for tailor-made structured deals.</p><p>Partial barrier options are the extension of barrier options, however there is a major difference between the two. Partial barrier options assume that the barrier prevails only for some fraction of the option’s lifetime, while barrier options prevail through the entire life of the option. Heynan and Kat [<xref ref-type="bibr" rid="scirp.24550-ref1">1</xref>] studied two types of continuous partial single barrier options: 1) an option with a monitoring period which commences at the start date of the option and terminates at an arbitrary date before expiration (this is referred to as an early-end partial barrier option); and 2) an option with a monitoring period which commences strictly at the starting date and ends strictly before the expiration date.&#160;</p><p>A window barrier option incorporates a barrier which commences at an arbitrary date after the starting date and terminates at an arbitrary date before the expiration. Window barrier options are more flexible than standard barrier options because the adaptable monitoring period provides traders with the full flexibility to lock volatility risks during a specific time period. Window barrier options not only offer investors a hedge instrument maneuvered by investors’ views on the range of volatility, but these options also provide building blocks to create various types of partial exotic options embedded in structured products. In recent years they have become more popular with investors, particularly in foreign exchange markets. Meanwhile, academics and practitioners have turned their attention to the more complicated structures of barrier options.</p><p>Since Merton [<xref ref-type="bibr" rid="scirp.24550-ref2">2</xref>] first derived the analytical closedform solution to handle a down-and-out continuous monitoring barrier call, there has been a variety of research concerning this issue. Cox and Rubinstein [<xref ref-type="bibr" rid="scirp.24550-ref3">3</xref>] provided a valuation formula for an up-and-out call, which is nullified whenever the underlying asset price triggers the upper knockout price. Rubinstein and Reiner [<xref ref-type="bibr" rid="scirp.24550-ref4">4</xref>] provided the formulae for 8 types of barrier options, and Haug [<xref ref-type="bibr" rid="scirp.24550-ref5">5</xref>] gave a generation of the set of formulae provided by Rubinstein and Reiner. Kunitomo and Ikeda [<xref ref-type="bibr" rid="scirp.24550-ref6">6</xref>] provided valuation formulae based on a generalization of the Levy formula for double barrier options with two exponential curved boundaries. Geman and Yor [<xref ref-type="bibr" rid="scirp.24550-ref7">7</xref>] used the CameronMartin theorem to obtain the Laplace transformation of the values for double barrier options with two fixed boundaries.</p><p>The binomial and trinomial lattice models developed respectively by Cox, Ross and Rubinstein [<xref ref-type="bibr" rid="scirp.24550-ref8">8</xref>] and Boyle [9,10] are well-known schemes for pricing standard vanilla options. However, Boyle and Lau [<xref ref-type="bibr" rid="scirp.24550-ref11">11</xref>] demonstrated that the CRR binomial model may lead to persistent errors in barrier option pricing. Ritchken [<xref ref-type="bibr" rid="scirp.24550-ref12">12</xref>] illustrated that when the trinomial model is naively applied to the pricing of barrier options, more time steps may not always lead to more accurate prices. Boyle and Lau [<xref ref-type="bibr" rid="scirp.24550-ref11">11</xref>] and Ritchken [<xref ref-type="bibr" rid="scirp.24550-ref12">12</xref>] suggested modified lattice algorithms to generate accurate pricing for the barrier option. But as revealed in Ritchken [<xref ref-type="bibr" rid="scirp.24550-ref12">12</xref>], the modified algorithms suggested by Boyle and Lau [<xref ref-type="bibr" rid="scirp.24550-ref11">11</xref>] and Ritchken [<xref ref-type="bibr" rid="scirp.24550-ref12">12</xref>] are nevertheless inefficient for handling the barrier-too-close problem. Wang, Liu and Hsiao [<xref ref-type="bibr" rid="scirp.24550-ref13">13</xref>] used a hybrid method, which is a combination of the Laplace transformation and the finite-difference approach, to overcome the unstable problem for pricing barrier options modeled by a branching process. Figlewski and Gao [<xref ref-type="bibr" rid="scirp.24550-ref14">14</xref>] used the adaptive mesh model to discuss option pricing. Albert, Fink, Fink [<xref ref-type="bibr" rid="scirp.24550-ref15">15</xref>] priced barrier options using an adaptive mesh model under a jump-diffusion process.</p><p>Broadie, Glasserman, and Kou [<xref ref-type="bibr" rid="scirp.24550-ref16">16</xref>] and H&#246;rfelt [<xref ref-type="bibr" rid="scirp.24550-ref17">17</xref>] derived the approximation formulae for the discrete single barrier options. Boyle and Tian [<xref ref-type="bibr" rid="scirp.24550-ref18">18</xref>] proposed a modified explicit finite difference approach to the valuation of barrier options, but their method is not particularly efficient in dealing with discrete barrier option pricing. Ahn, Figlewski, and Gao [<xref ref-type="bibr" rid="scirp.24550-ref19">19</xref>] suggested the adaptive mesh model structure for pricing discrete barrier options. Kou [<xref ref-type="bibr" rid="scirp.24550-ref20">20</xref>] applied a sequential analysis to extend Broadie, Glasserman and Kou’s approximation formulae [<xref ref-type="bibr" rid="scirp.24550-ref16">16</xref>] to more general cases of discrete barrier options. Mitov, Rachev, Kim and Fabozzi [<xref ref-type="bibr" rid="scirp.24550-ref21">21</xref>] derived an analytical formula for the price of an up-and-out call, and showed that the values of barrier options priced with the branching process in a random environment model were significantly different from those modeled with a lognormal process. Hu and Knessl [<xref ref-type="bibr" rid="scirp.24550-ref22">22</xref>] analyzed the asymptotics of barrier option pricing under the constant elasticity of variance (CEV) process.</p><p>Heynen and Kat [<xref ref-type="bibr" rid="scirp.24550-ref1">1</xref>] first derived the closed-form solutions for pricing partial late-start and early-end barrier options under Black-Scholes assumptions [<xref ref-type="bibr" rid="scirp.24550-ref23">23</xref>], and their solutions were expressed in terms of the bivariate normal distribution function. Heynen and Kat [<xref ref-type="bibr" rid="scirp.24550-ref24">24</xref>] extended their closed-form formula to handle a discrete window barrier option where the barrier level may change deterministically and the monitoring points can be of unequal distance to each other. Armstrong [<xref ref-type="bibr" rid="scirp.24550-ref25">25</xref>] extended Heynen and Kat’s closed-form formula [<xref ref-type="bibr" rid="scirp.24550-ref1">1</xref>] and derived formulae with a tripartite deterministic term-structure of interest rates, volatility, and dividend yields in terms of trivariate normal distribution functions. Carr [<xref ref-type="bibr" rid="scirp.24550-ref26">26</xref>] derived a riskneutral expectation formula to value partial barrier options with a constant rebate.</p><p>Most of the partial barrier models mentioned previously, with the exception of that of Heynen and Kat [<xref ref-type="bibr" rid="scirp.24550-ref24">24</xref>], assume that the underlying asset is continuously monitored against the partial barrier level. Nevertheless, discrete barrier options are among the most popular time-dependent options traded in markets. In addition, they are monitored discretely only at a particular time, normally, at daily closing (e.g. the capped index spread on the S&amp;P100 and S&amp;P500, and the knock-out barrier options on the All Ordinary Price Index on the Australian Stock Exchange). Although Chance [<xref ref-type="bibr" rid="scirp.24550-ref27">27</xref>], Kat and Verdonk [<xref ref-type="bibr" rid="scirp.24550-ref28">28</xref>] indicated that there exists a substantial price difference between barrier options and their otherwise identical continuous counterparts even under daily monitoring, the exact pricing formula was still not extended to discrete window barrier options with more complex features such as a varying rebate, barrier, and volatility with a discrete monitoring period.</p><p>This paper proposes the boundary integral method (BIM) [<xref ref-type="bibr" rid="scirp.24550-ref29">29</xref>], which is an efficient partial differential equation (PDE) approach, to price both continuous and discrete window barrier options under the Black-Scholes economy. We extend the continuous models of Heynen and Kat [<xref ref-type="bibr" rid="scirp.24550-ref1">1</xref>] and Armstrong [<xref ref-type="bibr" rid="scirp.24550-ref25">25</xref>] to include time-dependent rebates and a tripartite deterministic term structure of interest rates and volatility. In addition, the BIM can easily be further extended to the valuation of multiwindow barrier options characterized with a ladder strike prices. The discrete window barrier option of Heynen and Kat [<xref ref-type="bibr" rid="scirp.24550-ref24">24</xref>] is also extended to accommodate the multipartite term structure of interest rates and volatility. We also demonstrate that the proposed integral method is capable of valuating the discrete window double barrier option. Numerical examples and comparisons with Armstrong [<xref ref-type="bibr" rid="scirp.24550-ref25">25</xref>] confirm that the BIM will yield rapid and highly accurate numerical solutions for both discrete and continuous window barrier options. In addition, the numerical examples confirm that the BIM has a convergence rate of order 4 in the case of discrete window barrier option pricing.</p><p>This paper is organized as follows: in Section 2 we present the valuation algorithm in terms of the initial value problem and boundary value problem. We also explain how to deal with discontinuities caused by the window barrier feature, and demonstrate how to recursively obtain the option price. Section 3 discusses the valuation of discrete window barrier options, and defines the pricing problem as a sequence of the initial value problem. Section 4 contains numerical results, and Section 5 concludes with a summary and some suggestions for future research.</p></sec><sec id="s2"><title>2. Methodology</title><sec id="s2_1"><title>2.1. Preliminary Assumptions</title><p>Since a knock-in window barrier option plus a knock-out window barrier option will be equal to the value of an otherwise equivalent vanilla option, we will concentrate only on the knock-out window barrier option. Let 0, t<sub>1</sub>, t<sub>2</sub>, and T denote the option’s starting date, the time to the start of the barrier, the time to the end of the barrier, and the option’s maturity date, respectively, and <img src="3-1490096\1f9c9a38-0123-4504-b74a-546427c49308.jpg" />. The valuation of the early-ending window barrier option can be calculated by letting t<sub>1</sub> approach 0, and the valuation of the forward-start window barrier option can be recovered by letting t<sub>2</sub> approach T.</p><p>Our objective is to apply the PDE (partial differential equation) approach to the valuation of the window barrier option in Black-Scholes economy assumptions. When the underlying is assumed to follow a lognormal random walk, under no arbitrage argument, the PDE governing the window barrier option will be as follows:</p><disp-formula id="scirp.24550-formula74948"><label>, (1)</label><graphic position="anchor" xlink:href="3-1490096\2d985e1d-0f38-4946-9e39-b1e1cc50774a.jpg"  xlink:type="simple"/></disp-formula><p>where C is the option value, S is the underlying asset price, <img src="3-1490096\b2753a46-f38a-4f83-96d8-1542150e5b2c.jpg" /> is stock’s volatility, <img src="3-1490096\def195ef-f43c-4d8c-bae4-33461cea3730.jpg" />is the risk-free interest rate, <img src="3-1490096\8489538d-6c17-4236-b272-c886cb996db5.jpg" />is the dividend yield, and t is the time. To allow for the case of greatest generality, the stock’s volatility and the risk-free interest rate may change deterministically across the barrier monitoring period. We allow for three different governing PDEs, or we may say, the Black-Scholes equation with different coefficients for time intervals [0, t<sub>1</sub>), [t<sub>1</sub>, t<sub>2</sub>], and (t<sub>2</sub>, T]. As in Armstrong [<xref ref-type="bibr" rid="scirp.24550-ref25">25</xref>], we assume a simple tripartite term structure that naturally accommodates the location of the barrier, and the risk-free interest rate, dividend yield, and volatility are given by the following step functions:</p><p><img src="3-1490096\b093d620-ae31-4328-b03c-b345f03128c6.jpg" />,</p><p><img src="3-1490096\298ab77b-c872-4cf8-8f83-e05f36187235.jpg" />,</p><p><img src="3-1490096\5d7d11fb-a24f-4b45-bf5b-b30f2e975a1a.jpg" />.</p><p>When the underlying asset price does not touch or breach the barrier level through the monitoring period, the payoff of the window barrier option at the maturity date is given as the following equation:</p><disp-formula id="scirp.24550-formula74949"><label>, (2)</label><graphic position="anchor" xlink:href="3-1490096\b2a6927b-385e-4c5a-b6c6-19befa970bc4.jpg"  xlink:type="simple"/></disp-formula><p>where K denotes the strike price.</p><p>Oppositely, if the underlying asset price triggers the barrier level throughout the monitoring period, the option will be knocked out and clients will receive an immediate rebate R<sub>b</sub>. The payoff is as follows:</p><disp-formula id="scirp.24550-formula74950"><label>(3)</label><graphic position="anchor" xlink:href="3-1490096\652f4c49-2476-4dd6-adaf-4c6a2de134c0.jpg"  xlink:type="simple"/></disp-formula><p>where B denotes the barrier price and R<sub>b</sub> denotes the immediate rebate.</p><p>The equation (1) is the governing equation and conditions (2) and (3) are the initial condition and boundary condition for the call price C(S, t) respectively.</p><p>Let</p><p><img src="3-1490096\1e8a7f38-939e-4e39-a577-c96f4b85c99b.jpg" /></p><p>Making the following variable transformations:</p><disp-formula id="scirp.24550-formula74951"><label>, (4)</label><graphic position="anchor" xlink:href="3-1490096\0ca4bc23-1017-48db-a2e1-7b35dd2014e9.jpg"  xlink:type="simple"/></disp-formula><p>equation (1) can be simplified into the heat equation with a constant diffusion coefficient as follows:</p><disp-formula id="scirp.24550-formula74952"><label>(5)</label><graphic position="anchor" xlink:href="3-1490096\5b16accd-df39-4a84-baff-55ace4caa8de.jpg"  xlink:type="simple"/></disp-formula><p>The payoff of the window barrier option at the maturity date <img src="3-1490096\2dd06a5d-3e45-461f-80c0-0541809d1e7d.jpg" /> will be transformed into:</p><disp-formula id="scirp.24550-formula74953"><label>. (6)</label><graphic position="anchor" xlink:href="3-1490096\4784f5e5-1ae8-4f7c-afac-8a3f78340474.jpg"  xlink:type="simple"/></disp-formula><p>Since the asset price is assumed to change continuously with time, if the asset price S(τ) breaches the barrier level between time interval<img src="3-1490096\b51725b4-c71d-48aa-a304-8fd18e424210.jpg" />, it will first touch the barrier level. Therefore the payoff of the option can be transformed, as in equation (7).</p><disp-formula id="scirp.24550-formula74954"><label>(7)</label><graphic position="anchor" xlink:href="3-1490096\e070738a-4fb3-4be4-8930-68881389f906.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="3-1490096\ba272935-54b7-44fc-bcd5-94af2b6ec450.jpg" /> and<img src="3-1490096\8ff069b4-3621-41a5-87c2-aa1dca8ec981.jpg" />.</p></sec><sec id="s2_2"><title>2.2. Boundary Integral Method</title><p>On the time interval<img src="3-1490096\8ed9aa5d-917a-46df-ad21-37beb1c04539.jpg" />, there is not any boundary condition; hence the solution of the PDE is uniquely determined by the initial condition (6). The problem of finding the unique solution with PDE (5) and initial condition (6) is termed the initial value problem. In our notation, the integral representation of the solution will be:</p><disp-formula id="scirp.24550-formula74955"><label>(8)</label><graphic position="anchor" xlink:href="3-1490096\42646a45-96a6-4a14-8046-bf2519d5fbad.jpg"  xlink:type="simple"/></disp-formula><p>where the function G is called Green’s function with the infinite domain or the fundamental solution of the heat equation. It can be expressed as follows:</p><disp-formula id="scirp.24550-formula74956"><label>, (9)</label><graphic position="anchor" xlink:href="3-1490096\6acb959e-9384-4cc5-a81f-d489bcb774de.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="3-1490096\d712df22-5ed2-4b04-bd4d-c061ef5df9c8.jpg" /> is the Heaviside step function, and is defined by:</p><disp-formula id="scirp.24550-formula74957"><label>. (10)</label><graphic position="anchor" xlink:href="3-1490096\d80fdd4c-6ea9-4ca8-ad04-f0f41dd4a69c.jpg"  xlink:type="simple"/></disp-formula><p>Equation (8) has some interesting interpretations with respect to the risk-neutral approach of Cox and Rubinstein [<xref ref-type="bibr" rid="scirp.24550-ref3">3</xref>]. <img src="3-1490096\0b19b533-2eba-487f-8b7f-4bd4e6581815.jpg" />and Green’s function can be interpreted as the option’s terminal payoff and its risk-neutral probability density function, respectively. Thus the integral representation of the solution can be interpreted as the option’s expected terminal payoff, and the value of the window barrier option at time <img src="3-1490096\d4ac17b5-7b5e-4d57-b62e-c330de30097c.jpg" /> will be equal to its discounted expected value as suggested by equation (4).</p><p>As in Black-Scholes [<xref ref-type="bibr" rid="scirp.24550-ref23">23</xref>], equation (8) can be further simplified into a closed-form solution as:</p><disp-formula id="scirp.24550-formula74958"><label>, (11)</label><graphic position="anchor" xlink:href="3-1490096\6de8894a-dd36-4e78-8289-1221f35fc2b9.jpg"  xlink:type="simple"/></disp-formula><p>where N (.) is the cumulative normal distribution function. <img src="3-1490096\4e248ec6-033c-4879-9db2-be93588db068.jpg" />and</p><p><img src="3-1490096\46d240e7-42dc-4678-9c0a-a481ea5c1d1e.jpg" />.</p><p>However, if the transformed underlying asset price x<sub>2 </sub><sub></sub> is within the range <img src="3-1490096\4818f16e-dd47-41b8-a1cf-3686d43a52a4.jpg" /> at<img src="3-1490096\06b802f5-3128-4b87-8c33-9491dfaaadac.jpg" />the instant after it passes the monitoring date, i.e.<img src="3-1490096\012326f4-7704-42c6-b03c-ce059e0a017a.jpg" />, the transformed window barrier price will still change continuously across the barrier monitoring date<img src="3-1490096\6db45ac8-6a1d-4c9a-817a-ab06ba1bba26.jpg" />. If we denote <img src="3-1490096\265ec564-3317-409b-bdb3-730e04a0500a.jpg" /> as the instant after<img src="3-1490096\6aac2cc0-07a5-4854-9f88-a4713af20691.jpg" />, the continuity assumption will guarantee that <img src="3-1490096\c6b5c6fb-8044-473b-9d72-165370d755a9.jpg" /> will be equal to<img src="3-1490096\e6cb6cc5-3bd0-4a4d-87e4-3dac39f96ed4.jpg" />. Therefore, the initial condition for equation (5) between <img src="3-1490096\62fdf43f-9bf4-4dba-84bb-e3717af7918e.jpg" /> will be as follows:</p><p><img src="3-1490096\2445b23c-26dc-477f-84d2-cd446679013e.jpg" />,(12)</p><p>where<img src="3-1490096\dcc58d2a-4668-4fa9-a311-3b9b1f07dfc5.jpg" />.</p><p>If the underlying asset price breaches the barrier level during the period, the window barrier option will be knocked out, and clients will receive an immediate rebate R<sub>b</sub>. The continuity property will guarantee that the asset price first touches the barrier level before it breaches the barrier level. Thus, the boundary condition for Equation (5) between <img src="3-1490096\8bbe7b24-34c8-4197-abac-d4e4a93bd9b6.jpg" /> will be specified as in Equation (13):</p><disp-formula id="scirp.24550-formula74959"><label>. (13)</label><graphic position="anchor" xlink:href="3-1490096\523540a7-f183-46ff-b8fa-c15f2299e650.jpg"  xlink:type="simple"/></disp-formula><p>There exists only one solution that satisfies the PDE (5) and is subject to the initial condition (12) and the boundary condition (13). The integral representation of a solution for the heat equation at <img src="3-1490096\2f5dbf14-f778-4694-93e7-6d67f006b1c0.jpg" /> is as follows:</p><p>If<img src="3-1490096\6527e1d5-49f3-46f8-b584-40bec11859d2.jpg" />, and<img src="3-1490096\7e51d5d1-5f2e-4be0-9453-68cb81dbe37c.jpg" />, then</p><disp-formula id="scirp.24550-formula74960"><label>, (14)</label><graphic position="anchor" xlink:href="3-1490096\dfa8b25c-789e-4d90-8e63-27251ea9dcd7.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="3-1490096\c3c1e82f-472e-405e-8706-7b4a9ca234cb.jpg" /> and</p><p><img src="3-1490096\fd2b1fc8-aef6-4a04-87f5-3f66afc39fc9.jpg" />.</p><p>G is the green function with the boundary<img src="3-1490096\b5163822-9918-4655-b0ae-f54ac791fde8.jpg" />.</p><p><img src="3-1490096\009b34bc-a0c2-45a8-8257-4752049264b0.jpg" /></p><p>where b<sub>1</sub> is the transformed barrier price at<img src="3-1490096\2e368227-95ab-48f6-892d-bafeb8df7edf.jpg" />, <img src="3-1490096\e7e8dc18-b05d-4d33-b982-9560b8c49d12.jpg" />, <img src="3-1490096\3e214b37-36d1-4e4b-818a-cb0591e79f68.jpg" />and</p><disp-formula id="scirp.24550-formula74961"><label>. (15)</label><graphic position="anchor" xlink:href="3-1490096\2f21028a-beaf-4c75-9818-77299fda554a.jpg"  xlink:type="simple"/></disp-formula><p>The functions G(.) and G<sub>x</sub>(.) in equation (14) can be interpreted as the transition probability density function and the hitting probability density function of the transformed underlying asset price, respectively. The first term in equation (14) is the expected payoff when the barrier is never breached throughout the monitoring interval [<img src="3-1490096\17e589d5-4662-4250-9dd4-0cc2b47bda91.jpg" />,<img src="3-1490096\edd50787-ede7-43bc-8004-2efe46122921.jpg" />], and the second term is the expected payoff when the underlying asset price breaches the barrier in the time interval [<img src="3-1490096\8fa160ee-1461-410e-a028-9ec615f938df.jpg" />,<img src="3-1490096\b9b8ee4b-c00f-4802-8b58-105c7ffbebe3.jpg" />]. Once again the solution can be interpreted as the expected payoff in a risk-neutral environment.</p><p>Finally, we will discuss how to cope with parameter discontinuities and obtain the ultimate solution <img src="3-1490096\67e0cb30-d169-42ae-95da-716feec5a66a.jpg" />. Let <img src="3-1490096\1f084a58-b9da-46e0-a098-b9d4bb6f1471.jpg" /> denote the instant after<img src="3-1490096\39764a5d-7e91-4c2e-8220-29f66391e63a.jpg" />; the parameter discontinuity happening between time to maturity <img src="3-1490096\648b1ef5-03bb-418c-b418-4dc24314d786.jpg" /> and <img src="3-1490096\260d5fc5-0479-4c3c-8699-913556f780b0.jpg" /> can be overcome with the same logic as in equation (12). That is, when <img src="3-1490096\06c98097-ec98-42d2-8b99-ad596e8dcdd6.jpg" /> approaches<img src="3-1490096\68671d4e-2cc4-496e-8fb2-fca595e9dad4.jpg" />, <img src="3-1490096\8a547292-4f91-41cd-a829-a51cd2c268c1.jpg" />will be equal to<img src="3-1490096\f1be8a6f-8ef1-47d8-bebb-4bf9e8440db4.jpg" />. The solution problem once again is an initial value problem analogous to the first period valuation from <img src="3-1490096\a16e9f5e-bf39-4bdc-b3e2-07aa2b05b0c9.jpg" /> to<img src="3-1490096\a0d77e39-fe36-42f1-ad52-6c03e36917e3.jpg" />. Therefore the initial condition for differential equation (5) between time interval <img src="3-1490096\6f95e1d2-4a90-4e4e-845f-4ac0d855cf02.jpg" /> has to be<img src="3-1490096\1217e95c-732c-4c2d-819b-8c86230a34e4.jpg" />, and the integral representation of the closed-form approximate solution for <img src="3-1490096\b03b217b-e5c1-41e9-a7fb-e6c2c13f7c5c.jpg" /> is as follows:</p><disp-formula id="scirp.24550-formula74962"><label>, (16)</label><graphic position="anchor" xlink:href="3-1490096\437d08bf-4470-4b5e-a5c3-10223d17e856.jpg"  xlink:type="simple"/></disp-formula><p>where Green’s function is denoted by equation (17),</p><disp-formula id="scirp.24550-formula74963"><label>. (17)</label><graphic position="anchor" xlink:href="3-1490096\d1dd22e7-342e-4fe5-938f-52bdfa246868.jpg"  xlink:type="simple"/></disp-formula><p>Finally, the theoretical value for the window barrier option, <img src="3-1490096\4e31d37d-ecc0-4564-a546-3036f0f31efe.jpg" />, can easily be obtained by the following inverse transformation:</p><disp-formula id="scirp.24550-formula74964"><label>, (18)</label><graphic position="anchor" xlink:href="3-1490096\0279abb9-6725-4196-88e4-271e2ccb7f7c.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="3-1490096\940988a7-1e38-4ec4-a647-866c0086d25c.jpg" />.</p><p>A key benefit of adopting the PDE approach is that it reduces the pricing problem for the window barrier option to two initial value problems and one boundary value problem, for all of which standard mathematical engineering numerical algorithms are well developed. These algorithms allow a straightforward numerical integration of highly accurate numerical values for window barrier options pricing. Since the Black-Scholes equation can be simplified into a homogenous linear equation such as the heat equation, the boundary integral method proposed in this paper will be a highly efficient algorithm to calculate window barrier options’ numerical solution.</p><p>In brief, the valuation of the standard partial barrier call can be divided into a three-phase process, as demonstrated in <xref ref-type="fig" rid="fig1">Figure 1</xref>. In the first phase, the terminal payoff at the maturity date, <img src="3-1490096\594895e9-28ac-45b0-94c3-2f082ce7d101.jpg" />is the initial condition for the PDE at<img src="3-1490096\a1fe835f-6ba4-4f23-9ad8-90e0d18dab59.jpg" />. By applying the integral method, we calculate the convolution of the initial condition <img src="3-1490096\46c51104-217b-4c28-9a37-a405f7023423.jpg" /> and Green’s function to acquire the integral representation of numerical solution <img src="3-1490096\3a70eb0d-94eb-4f26-adcc-68b6e80e3876.jpg" /> at<img src="3-1490096\4eb62fda-fc3d-43df-8f36-0290d091459a.jpg" />. Next, although the parameter discontinuity caused by the window barrier features will occur at<img src="3-1490096\639863a7-0d0a-4d6b-b159-afe2d842b0ab.jpg" />, the instant after the monitoring date<img src="3-1490096\dc4fe996-6ff4-423a-8578-c7896dfb174c.jpg" />, if</p><p><img src="3-1490096\1d1f0ac3-d2a0-4c82-a633-a8bdb367607f.jpg" />, <img src="3-1490096\90140b53-ab13-420e-ac4e-3a252da3b87c.jpg" />has to be continuous at<img src="3-1490096\d427ebe2-caa4-438c-bb1b-0f70fdc1daa2.jpg" />. Thus the parameter discontinuity at <img src="3-1490096\a4ae10b8-b6a1-4fd2-965b-24419574fa0b.jpg" /> can be handled accordingly, and the initial condition and the boundary condition imposing on the heat equation can be denoted as in equations (12) and (13). Since the Green function under such boundary constraints exists and is available, the boundary integral method can be applied to acquire the unique solution for differential equation (5) at time to maturity<img src="3-1490096\4bb3db01-d66c-423f-8bc9-d3dcb4a22d46.jpg" />. In the third phase, the discontinuity problem between <img src="3-1490096\d7c558d8-7e1a-4ce8-9a29-753cccfd5e7c.jpg" /> and <img src="3-1490096\4a544e49-cf48-440c-9a48-ecbb641e9464.jpg" /> can be handled in the same manner as in phase 2. Thus</p><p><img src="3-1490096\1c8a09cf-403c-46f2-bb1e-13e2f0c7c495.jpg" />will be the initial condition imposing on the differential equation between<img src="3-1490096\f754f3b0-9a68-4da2-95eb-afda01dc039b.jpg" />. Hence, the problem of finding <img src="3-1490096\8dd7bc90-a03e-44e0-8eba-c0ff5e506e1e.jpg" /> will be an initial value problem again, and the integral representation of the solution can be obtained easily, as in phase 1. The transformation of <img src="3-1490096\fd063015-3e72-4251-a9bb-0c8f8bac0d7d.jpg" /> by Equation (18) will ultimately obtain the numerical solution of the window barrier option<img src="3-1490096\bad10f5a-6e47-4051-9886-6fad09f4722c.jpg" />. In Equations (8), (14) and (16), u(.) and G(.) are very smooth functions. Thus, a simple integration scheme such as the Simpson integral will obtain exceptionally precise closed-form approximate values for both <img src="3-1490096\f7036a19-6e60-4d60-aa11-2770f7a8aba5.jpg" /> and<img src="3-1490096\a63a6f88-50b7-4f07-af8c-dee805450c1e.jpg" />. Finally, a highly accurate estimation of <img src="3-1490096\fdf738b9-bed3-4c41-81b1-54f32b76a80a.jpg" /> can be obtained by recursively integrating backward through time.</p><p>The boundary integral method proposed in this paper can be easily extended to a multi-window barrier option or window ladder option. It also accommodates the pricing of early-end and late-start barrier options. The extra flexibility makes the proposed method an applicable way to calculate options with more complex features. <xref ref-type="fig" rid="fig1">Figure 1</xref> schematically explains the concept of a recursive algorithm. Since the parameter settings, the initial condition, and the boundary condition can be manipulated easily in a standard setting, the recursive algorithm can provide flexibility to tailor a barrier position, duration, barrier level, rebate, and strike price between monitoring periods, so as to suit investors’ unique needs. It can also accommodate multi-partite term structure interest rates and volatility.</p></sec></sec><sec id="s3"><title>3. Recursive Integral Method</title><p>In practice, barrier options are frequently monitored only at specific discrete dates. The discrete feature will cause a knock-out window barrier option to be more expensive and a knock-in window barrier option to be less expensive than their respective continuous monitoring counterparts. In this section, we still assume the Black-Scholes economy, but it is not necessary to assume a flat term-structure and constant volatility. As in the pricing of a continuous window barrier option, the term-structure interest rates and volatility can be multi-partite step functions that accommodate the location of the discrete barrier. The PDE approach also allows that the discrete barrier level may change deterministically during the monitoring period, and monitoring need not necessarily take place at equal-spaced points in time. Since the multipartite term structure of interest rates and volatility can be easily handled in the standard setting, for the purpose of simplifying the notations and focusing on the main idea of the recursive integral method, we will assume constant volatility and a flat term structure in this section.</p><p>Assume the option monitoring period [t<sub>1</sub>, t<sub>2</sub>] is partitioned into m − 1 discrete time intervals, and the option is subject to m times of discrete monitoring. If <img src="3-1490096\523942e7-1007-46c0-adfb-c225df59c4ba.jpg" /> denotes the set of discrete monitoring date, and <img src="3-1490096\afb8af1b-681f-4cc4-b8e2-be8e67d77a51.jpg" /> is for the corresponding set of time to maturity. In addition, we assume that the relations between the discrete monitoring dates are<img src="3-1490096\c514f550-965a-49a4-9da6-85c6338e7606.jpg" />, <img src="3-1490096\5eb8935c-89db-429a-8d89-3a945f31d320.jpg" />.</p><p><img src="3-1490096\0fa02d72-1b5c-4b9e-8f78-e44395605a09.jpg" />denotes the instant after the corresponding discrete monitoring dates.</p><p>Under these assumptions, equation (6) is still the initial condition for differential equation (5) between<img src="3-1490096\a290abfe-8d22-4e04-bbd9-57e830b72ad2.jpg" />, and <img src="3-1490096\ea79a101-9b8f-4fb9-83a7-dd0d2c4fefc3.jpg" /> is still the unique solution that satisfies the differential equation (5) at <img src="3-1490096\4dd1280c-7998-4184-8032-81a8e4cf4234.jpg" /> subject to the initial condition (6). Since no monitoring is required during time interval<img src="3-1490096\a1ee57ef-fc80-4dbf-bef7-220a62b5d871.jpg" />, the mathematical problem of finding the solution for difference equation (5) at <img src="3-1490096\d2bedfba-08d1-40c5-a032-e260f1307524.jpg" /> will be simplified to become an initial value problem. The solution <img src="3-1490096\074f2d06-0107-48b3-a390-f5857a681010.jpg" /> that satisfies the partial differential equation (5) subject to initial condition (6) will be as follows:</p><disp-formula id="scirp.24550-formula74965"><label>. (19)</label><graphic position="anchor" xlink:href="3-1490096\b93aa4be-c36b-4660-a7f5-1b8b5403b92e.jpg"  xlink:type="simple"/></disp-formula><p>The discrete monitoring feature will introduce m discontinuities into solutions at discrete monitoring dates M<sup>*</sup>. Following the same logic as discussed in the section on pricing a continuous window barrier option, the instant after the discrete monitoring date <img src="3-1490096\13ece186-1606-46c8-828b-61656ca29bcd.jpg" /> if</p><p><img src="3-1490096\d785f8ca-b203-49c8-8e32-238d04ec3782.jpg" />, the value of the window barrier option will change continuously across the discrete monitoring date<img src="3-1490096\047f7fad-dc8b-47c2-a8be-ce19db0e1aaa.jpg" />, thus <img src="3-1490096\42ad639e-f78d-404c-8452-29a8e2be2d0d.jpg" /> will be equal to<img src="3-1490096\04f48376-ab87-4d56-a0bf-40d44b7bd53b.jpg" />. Otherwise, it will be equal to <img src="3-1490096\f15aa931-e558-4533-b932-9712cc8ed665.jpg" /> according to the pre-specified contract rebate specification. Thus the solution <img src="3-1490096\0fb31349-6d49-4ee6-a979-b9bd9401cbee.jpg" /> can be defined as follows:</p><disp-formula id="scirp.24550-formula74966"><label>. (20)</label><graphic position="anchor" xlink:href="3-1490096\8876d0ae-693f-48b5-9c72-e9ced173407a.jpg"  xlink:type="simple"/></disp-formula><p>Equation (20) will be the initial condition for Equation (5) between<img src="3-1490096\27660f4a-16fa-4a91-8f7c-4eb041bd70ee.jpg" />, and the unique solution for equation (5) at <img src="3-1490096\6d298758-7ee9-4d8c-9f33-6656c53664c6.jpg" /> is given by equation (21).</p><disp-formula id="scirp.24550-formula74967"><label>(21)</label><graphic position="anchor" xlink:href="3-1490096\529a1b52-7e40-4a15-9efb-bd8c9e1ea47d.jpg"  xlink:type="simple"/></disp-formula><p>By applying the same argument, the integral representations of solutions for differential equation (5) at<img src="3-1490096\abfe91b5-04b1-4e1b-a4b6-deed564ca581.jpg" />,<sub> <img src="3-1490096\500492c7-e400-41fd-97dc-843353e8a4e8.jpg" /></sub>, <img src="3-1490096\aecb5d32-863c-41cc-9c07-dc84d42254ed.jpg" />, are given by the recursive integral method as follows:</p><disp-formula id="scirp.24550-formula74968"><label>(22)</label><graphic position="anchor" xlink:href="3-1490096\15ef1317-8676-44c8-bb30-c7d53407c211.jpg"  xlink:type="simple"/></disp-formula><p>for<img src="3-1490096\6abd9641-393a-4021-8464-16e605f40e96.jpg" />.</p><disp-formula id="scirp.24550-formula74969"><label>(23)</label><graphic position="anchor" xlink:href="3-1490096\a66d4074-7bca-4e50-93bc-128b92e926c0.jpg"  xlink:type="simple"/></disp-formula><p>for<img src="3-1490096\fbca17e5-080c-41d5-ac0b-b3636161f1c2.jpg" />.</p><p>Finally, <img src="3-1490096\a9162362-62ac-48a2-aeea-0a3a178d5d4a.jpg" />will be equal to <img src="3-1490096\b90ed48c-08c8-4076-8089-2ce3f04532f0.jpg" /> as in the continuous window barrier option case in Section 2, and <img src="3-1490096\3e39ecdd-4b01-4d49-b983-698e96efb1cb.jpg" /> can be obtained by using <img src="3-1490096\d580d73c-6be5-44f7-96b4-f7218f5766c1.jpg" /> as the initial condition, and the unique solution for equation (5) subject to initial condition <img src="3-1490096\12ceaefa-1ac4-49ab-afd0-243ca07e52f0.jpg" /> will be:</p><disp-formula id="scirp.24550-formula74970"><label>, (24)</label><graphic position="anchor" xlink:href="3-1490096\852a75e4-8b58-421b-a7be-b12ce9e2d642.jpg"  xlink:type="simple"/></disp-formula><p>and <img src="3-1490096\17dddefc-7c03-4d65-b1b7-0608a3de1a01.jpg" /> can be obtained by dividing <img src="3-1490096\80ba4339-b3e4-486e-8d05-43d32881377a.jpg" /> with <img src="3-1490096\c1120d0f-f473-4c0e-aa7e-8c5d8cc8978f.jpg" /> as specified in equation (4).</p><p>The valuation of the discrete window barrier option can be defined as a sequence of initial value problems. The proposed recursive integral method is quite analogous to the lattice models and finite difference algorithm. All approaches involve the initial value and work backward to find a solution one step back in time, but there are no intermediate time steps between two discrete monitoring dates for the integral approach. The key advantage of the PDE approach is that most of the standard techniques for solving the PDE in engineering mathematics can be applied to calculate the option pricing, and it can provide practitioners with a more flexible and applicable way to accommodate the complexities of OTC exotic options. Furthermore, when the composite Simpson’s rule is applied to estimate the numerical solution of<img src="3-1490096\419875b6-fd38-437a-a8c4-ebf68906dc70.jpg" />, Wang and Hsiao [<xref ref-type="bibr" rid="scirp.24550-ref30">30</xref>] prove that the recursive integral method will have a convergence rate of order 4. Hence, the proposed recursive integral method will easily obtain a rapid and highly accurate solution for the discrete window barrier option.</p></sec><sec id="s4"><title>4. Numerical Examples</title><p>This section provides some numerical examples, and studies the performance of the BIM algorithm for different choices of parameter settings. To assess the validity of our approach, we compare our continuous window barrier option results with numerical results presented in Armstrong [<xref ref-type="bibr" rid="scirp.24550-ref25">25</xref>], and the parameter settings of the discrete window barrier option is identical to numerical examples discussed in Heynen and Kat [<xref ref-type="bibr" rid="scirp.24550-ref24">24</xref>].</p><p><xref ref-type="table" rid="table1">Table 1</xref> investigates the convergence rate of the BIM under different assumptions of stock prices. All examples demonstrate that the BIM has approximately a convergence rate of order 2. When the region of integration in the equation is partitioned into only 128 subintervals, the precision of our valuation algorithm has reached at least a 5 significant digit level in all cases. <xref ref-type="table" rid="table2">Table 2</xref> examines the impact of the “barrier-too-close” upon the validity of our proposed algorithm. All numerical examples still demonstrate that the BIM has approximately a convergence rate of order 2, and highly precise numerical values can be easily obtained with the region of integration partitioned into only 128 subintervals. Since we do not partition the underlying asset and time into node spaces as in lattice models, there is no discretization error or approximation error. Numerical examples in <xref ref-type="table" rid="table2">Table 2</xref> confirm that the BIM will not encounter the “barrierto-close” problem in the pricing of window barrier options.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.24550-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">R. Heynen and H. Kat, “Partial barrier options,” Journal of Financial Engineering, Vol. 3, No. 4, 1994, pp. 253-274.</mixed-citation></ref><ref id="scirp.24550-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">R. C. Merton, “Theory of Rational Option Pricing,” Bell Journal of Economics and Management Science, Vol. 4, No. 1, 1973, pp. 141-183. doi:10.2307/3003143</mixed-citation></ref><ref id="scirp.24550-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">J. C. Cox and M. Rubinstein, “Options Markets,” Prentice-Hall, Upper Saddle River, 1985.</mixed-citation></ref><ref id="scirp.24550-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">M. Rubinstein and E. Reiner, “Breaking Down the Barriers,” RISK, Vol. 4, No. 8, 1991, pp. 28-35.</mixed-citation></ref><ref id="scirp.24550-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">E. Haug, “The Complete Guide to Option Pricing Formulas,” McGraw Hill, New York, 1997.</mixed-citation></ref><ref id="scirp.24550-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">N. Kunitomo and M. Ikeda, “Pricing Options with Curved Boundaries,” Mathematical Finance, Vol. 2, No. 4, 1992, pp. 275-298. doi:10.1111/j.1467-9965.1992.tb00033.x</mixed-citation></ref><ref id="scirp.24550-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">H. Geman and M. Yor, “Pricing and Hedging Double-Barrier Options: A Probabilistic Approach,” Mathematical Finance, Vol. 6, No. 4, 1996, pp. 365-378.  
doi:10.1111/j.1467-9965.1996.tb00122.x</mixed-citation></ref><ref id="scirp.24550-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">J. C. Cox, S. A. Ross and M. Rubinstein, “Option Pricing: A Simplified Approach,” Journal of Financial Economics, Vol. 7, No. 3, 1979, pp. 229-264.  
doi:10.1016/0304-405X(79)90015-1</mixed-citation></ref><ref id="scirp.24550-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">P. P. Boyle, “Option Valuation Using a Three-Jump Process,” International Options Journal, Vol. 3, 1986, pp. 7-12.</mixed-citation></ref><ref id="scirp.24550-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">P. P. Boyle, “A Lattice Framework for Option Pricing with Two State Variables,” Journal of Financial and Quantitative Analysis, Vol. 23, No. 1, 1988, pp. 1-12.  
doi:10.2307/2331019</mixed-citation></ref><ref id="scirp.24550-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">P. P. Boyle and S. H. Lau, “Bumping Up against the Barrier with the Binomial Method,” Journal of Derivatives, Vol. 1, No. 4, 1994, pp. 6-14.  
doi:10.3905/jod.1994.407891</mixed-citation></ref><ref id="scirp.24550-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">P. Ritchken, “On Pricing Barrier Options,” Journal of Derivatives, Vol. 3, No. 2, 1995, pp. 19-28.  
doi:10.3905/jod.1995.407939</mixed-citation></ref><ref id="scirp.24550-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">M. L. Wang, Y. H. Liu and Y. L. Hsiao, “Barrier Option Pricing: A Hybrid Method Approach,” Quantitative Finance, Vol. 9, No. 3, 2009, pp. 341-352.  
doi:10.1080/14697680802595593</mixed-citation></ref><ref id="scirp.24550-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">S. Figlewski and B. Gao, “The Adaptive Mesh Model: A New Approach to Efficient Option Pricing,” Journal of Financial Economics, Vol. 53, No. 3, 1999, pp. 313-351.  
doi:10.1016/S0304-405X(99)00024-0</mixed-citation></ref><ref id="scirp.24550-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">M. Albert, J. Fink and K. E. Fink, “Adaptive Mesh Modeling and Barrier Option Pricing under a Jump-Diffusion Process,” Journal of Financial Research, Vol. 31, No. 4, 2008, pp. 381-408.  
doi:10.1111/j.1475-6803.2008.00244.x</mixed-citation></ref><ref id="scirp.24550-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">M. Broadie, P. Glasserman and S. Kuo, “Connecting Discrete and Continuous Path-Dependent Options,” Finance and Stochastics, Vol. 3, No. 1, 1999, pp. 55-82.  
doi:10.1007/s007800050052</mixed-citation></ref><ref id="scirp.24550-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">P. H?rfelt, “Extension of the Corrected Barrier Approximation by Broadie, Glassman, and Kou,” Finance and Stochastics, Vol. 7, 2003, pp. 231-243.  
doi:10.1007/s007800200077</mixed-citation></ref><ref id="scirp.24550-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">P. P. Boyle and Y. Tian, “An Explicit Finite Difference Approach to the Pricing of Barrier Options,” Journal Applied Mathematical Finance, Vol. 5, No. 1, 1998, pp. 17-43. doi:10.1080/135048698334718</mixed-citation></ref><ref id="scirp.24550-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">D. Ahn, S. Figlewski and B. Gao, “Pricing Discrete Barrier Options with an Adaptive Mesh Model,” Journal of Derivatives, Vol. 6, No. 4, 1999, pp. 33-43.  
doi:10.3905/jod.1999.319127</mixed-citation></ref><ref id="scirp.24550-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">S. G. Kou, “On Pricing of Discrete Barrier Options,” Statistica Sinica, Vol. 13, No. 4, 2003, pp. 955-964.</mixed-citation></ref><ref id="scirp.24550-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">G. K. Mitov, S. T. Rachev, Y. S. Kim and F. J. Fabozzi, “Barrier Option Pricing by Branching Processes,” International Journal of Theoretical and Applied Finance, Vol. 12, No. 7, 2009, pp. 1055-1073.  
doi:10.1142/S0219024909005555</mixed-citation></ref><ref id="scirp.24550-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">F. Hu and C. Knessl, “Asymptotics of Barrier Option Pricing under the CEV Process,” Applied Mathematical Finance, Vol. 17, No. 3, 2010, pp. 261-300.  
doi:10.1080/13504860903335355</mixed-citation></ref><ref id="scirp.24550-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">F. Black and M. Scholes, “The Pricing of Options and Corporate Liabilities,” Journal of Political Economy, Vol. 81, No. 3, 1973, pp. 637-659. doi:10.1086/260062</mixed-citation></ref><ref id="scirp.24550-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">R. Heynen and H. Kat, “Discrete Partial Barrier Options with a Moving Barrier,” Journal of Financial Engineering, Vol. 5, No. 3, 1996, pp. 199-209.</mixed-citation></ref><ref id="scirp.24550-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">G. F. Armstrong, “Valuation Formulae for Window Barrier Options,” Applied Mathematical Finance, Vol. 8, No. 4, 2001, pp. 197-208. doi:10.1080/13504860210124607</mixed-citation></ref><ref id="scirp.24550-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">P. Carr, “Two Extensions to Barrier Option Valuation,” Applied Mathematical Finance, Vol. 2, No. 3, 1995, pp. 173-209. doi:10.1080/13504869500000010</mixed-citation></ref><ref id="scirp.24550-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">D. Chance, “The Pricing and Hedging of Limited Exercise Caps and Spreads,” Journal of Financial Research, Vol. 17, No. 4, 1994, pp. 561-584.</mixed-citation></ref><ref id="scirp.24550-ref28"><label>28</label><mixed-citation publication-type="other" xlink:type="simple">H. Kat and L. Verdonk, “Tree Surgery,” RISK, Vol. 8, No. 2, 1995, pp. 53-56.</mixed-citation></ref><ref id="scirp.24550-ref29"><label>29</label><mixed-citation publication-type="other" xlink:type="simple">M. L. Wang and S. Y. Shen, “On Pricing of the Up-and-Out Call—A Boundary Integral Method Approach,” Asia Pacific Management Review, Vol. 10, No. 3, 2005, pp. 205-213.</mixed-citation></ref><ref id="scirp.24550-ref30"><label>30</label><mixed-citation publication-type="other" xlink:type="simple">M. L. Wang and Y. L. Hsiao, “A PDE Approach to Valuation of Discrete Barrier Option,” working paper, 2012.</mixed-citation></ref></ref-list></back></article>