<?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">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2016.79075</article-id><article-id pub-id-type="publisher-id">AM-66771</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  A New Approach for Solving Boundary Value Problem in Partial Differential Equation Arising in Financial Market
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>adugba</surname><given-names>Sunday Emmanuel</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>Emeka</surname><given-names>Helen Oluyemisi</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Mathematical and Physical Sciences, Afe Babalola University, Ado Ekiti, Nigeria</addr-line></aff><aff id="aff1"><addr-line>Department of Mathematical Sciences, Ekiti State University, Ado Ekiti, Nigeria</addr-line></aff><pub-date pub-type="epub"><day>26</day><month>05</month><year>2016</year></pub-date><volume>07</volume><issue>09</issue><fpage>840</fpage><lpage>851</lpage><history><date date-type="received"><day>1</day>	<month>April</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>23</month>	<year>May</year>	</date><date date-type="accepted"><day>26</day>	<month>May</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this paper, we present a new approach for solving boundary value problem in partial differential equation arising in financial market by means of the Laplace transform. The result shows that the Laplace transform for the price of the European call option which pays dividend yield reduces to the Black-Scholes-Merton model.
 
</p></abstract><kwd-group><kwd>Black-Scholes-Merton Model</kwd><kwd> Boundary Value Problem</kwd><kwd> European Call Option</kwd><kwd> Financial Market</kwd><kwd> Laplace Transform</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>An option is a contract that gives the right (not an obligation) to its holder to buy or sell some amount of the underlying asset at a future date for a prescribed price. The underlying assets include stocks, stock indices, debt instruments, commodities and foreign currency. A call option gives its holder the right to buy the underlying asset, whereas a put option gives its holder the right to sell. Vanilla options are actively traded on organized exchanges. They are also subject to certain regularity and standardization conditions. Vanilla options can be classified as American options and European options. An American option gives a financial agent the right, but not obligation to buy or to sell the underlying assets on or prior to the expiry date at the specified price called the exercise price. European option is an option that can be exercised only at the expiry date with linear payoff. European option comes in two forms namely European call and put options.</p><p>A European call option is an option that can be exercised only at expiry and has a linear payoff given by the difference between underlying asset price at maturity and the exercise price. The payoff for the European call option is given by</p><disp-formula id="scirp.66771-formula935"><label>. (1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x7.png"  xlink:type="simple"/></disp-formula><p>A European put option is an option that can be exercised only at expiry and has a linear payoff given by the difference between the exercise price and underlying asset price at maturity. The payoff for the European put option is given by</p><disp-formula id="scirp.66771-formula936"><label>. (2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x8.png"  xlink:type="simple"/></disp-formula><p>The revolution on derivative securities both in exchange markets and in academic communities began in the early 1970’s. How to rationally price an option was not clear until 1973, when Black and Scholes published their seminal work on option pricing in which they described a mathematical frame work for finding the fair price of a European option (see [<xref ref-type="bibr" rid="scirp.66771-ref1">1</xref>] ).</p><p>Moreover, in the same year, [<xref ref-type="bibr" rid="scirp.66771-ref2">2</xref>] extended the Black-Scholes model in several important ways. Since its invention, the Black-Scholes formula has been widely used by traders to determine the price of an option. However this famous formula has been questioned after the 1987 crash.</p><p>One of the main concerns about financial options is what the exact values of options are. For the simplest model in the case of constant coefficients, an exact pricing formula was derived by Black and Scholes, known as the Black-Scholes formula. However, in the general case of time and space dependent coefficients the exact pricing formula is not yet established, and thus numerical solutions have been used (see [<xref ref-type="bibr" rid="scirp.66771-ref3">3</xref>] ).</p><p>There are many exhaustive texts and literatures in this subject area such as [<xref ref-type="bibr" rid="scirp.66771-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.66771-ref10">10</xref>] , just to mention a few.</p><p>In this paper, we present a new approach for solving boundary value problem in partial differential equation arising in financial market via the Laplace transform. The rest of the paper is organized as follows: Section 2 presents the Black-Scholes-Merton partial differential equation for the price of European call option which pays a dividend yield. In Section 3, we consider the Laplace transform and some of its fundamental properties. Section 4 presents the Laplace transform for solving boundary value problem in partial differential equation arising in financial market. We also show that our result reduces to Black-Scholes-Merton like formula. Section 5 concludes the paper.</p></sec><sec id="s2"><title>2. The Black-Scholes-Merton Partial Differential Equation</title><p>We consider a market where the underlying asset price <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x9.png" xlink:type="simple"/></inline-formula> is governed by the stochastic differential equation of the form</p><disp-formula id="scirp.66771-formula937"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x10.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x11.png" xlink:type="simple"/></inline-formula> is the volatility, r is the riskless interest rate, d is the dividend yield and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x12.png" xlink:type="simple"/></inline-formula> is a one-dimensional Wiener process. Standard arbitrage arguments show that any derivative <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x13.png" xlink:type="simple"/></inline-formula> written on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x14.png" xlink:type="simple"/></inline-formula> must satisfy the partial differential equation of the form</p><disp-formula id="scirp.66771-formula938"><label>. (4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x15.png"  xlink:type="simple"/></disp-formula><p>Setting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x16.png" xlink:type="simple"/></inline-formula> in (4), then we have the Black-Scholes-Merton partial differential equation for the price of European call option given by</p><disp-formula id="scirp.66771-formula939"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x17.png"  xlink:type="simple"/></disp-formula><p>with boundary conditions</p><disp-formula id="scirp.66771-formula940"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x18.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula941"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x19.png"  xlink:type="simple"/></disp-formula><p>and final time condition given by</p><disp-formula id="scirp.66771-formula942"><label>. (8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x20.png"  xlink:type="simple"/></disp-formula><p>Equation (7) states that the option is worthless when the stock price is zero.</p></sec><sec id="s3"><title>3. The Laplace Transform and Its Fundamental Properties</title><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x21.png" xlink:type="simple"/></inline-formula> be a piece-wise continuous function on every closed interval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x22.png" xlink:type="simple"/></inline-formula> there exists <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x23.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x24.png" xlink:type="simple"/></inline-formula>. Then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x25.png" xlink:type="simple"/></inline-formula> is called the Laplace transform of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x26.png" xlink:type="simple"/></inline-formula> and is defined as</p><disp-formula id="scirp.66771-formula943"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x27.png"  xlink:type="simple"/></disp-formula><p>whenever the integral exists. Conversely, the inverse Laplace transform of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x28.png" xlink:type="simple"/></inline-formula> is defined as</p><disp-formula id="scirp.66771-formula944"><label>. (10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x29.png"  xlink:type="simple"/></disp-formula><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x30.png" xlink:type="simple"/></inline-formula> be a piece-wise continuous with the Laplace transform<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x31.png" xlink:type="simple"/></inline-formula>. The fundamental properties of the Laplace transform hold.</p><p>1) Linearity of the Laplace Transform</p><disp-formula id="scirp.66771-formula945"><label>. (11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x32.png"  xlink:type="simple"/></disp-formula><p>Equation (11) is intermediate from the definition and the linearity of the definite integral.</p><p>2) Scaling Property</p><disp-formula id="scirp.66771-formula946"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x33.png"  xlink:type="simple"/></disp-formula><p>3) Shifting Property</p><disp-formula id="scirp.66771-formula947"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x34.png"  xlink:type="simple"/></disp-formula><p>4) Commutativity Property</p><p>The Laplace transform is commutative. i.e.</p><disp-formula id="scirp.66771-formula948"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x35.png"  xlink:type="simple"/></disp-formula><p>5) The Laplace Transforms on Differentiation</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x36.png" xlink:type="simple"/></inline-formula> be a differentiable function with the derivative <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x37.png" xlink:type="simple"/></inline-formula> being continuous. Suppose that</p><p>there exist constant M and X such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x38.png" xlink:type="simple"/></inline-formula> then</p><disp-formula id="scirp.66771-formula949"><label>. (15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x39.png"  xlink:type="simple"/></disp-formula><p>Note that the condition</p><disp-formula id="scirp.66771-formula950"><label>. (16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x40.png"  xlink:type="simple"/></disp-formula><p>6) Convolution Property</p><p>Theorem 1: Convolution Theorem</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x41.png" xlink:type="simple"/></inline-formula> denote the Laplace transforms of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x42.png" xlink:type="simple"/></inline-formula>, respectively. Then the</p><p>product given by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x43.png" xlink:type="simple"/></inline-formula> is the Laplace transform of the convolution of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x44.png" xlink:type="simple"/></inline-formula></p><p>is denoted by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x45.png" xlink:type="simple"/></inline-formula> and the integral representation</p><disp-formula id="scirp.66771-formula951"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x46.png"  xlink:type="simple"/></disp-formula><p>We present some of the results on the existence and uniqueness of the Laplace transform below.</p><p>Theorem 2: Existence of Laplace Transform</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x47.png" xlink:type="simple"/></inline-formula> be a piecewise continuous function on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x48.png" xlink:type="simple"/></inline-formula> (for every<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x49.png" xlink:type="simple"/></inline-formula>) and have an exponential order</p><p>at infinity with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x50.png" xlink:type="simple"/></inline-formula>. Then, the Laplace transform <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x51.png" xlink:type="simple"/></inline-formula> is defined for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x52.png" xlink:type="simple"/></inline-formula>, i.e.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x53.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 3: Uniqueness of Laplace Transform Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x54.png" xlink:type="simple"/></inline-formula> be two piecewise continuous func-</p><p>tions with an exponential order at infinity. Assume that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x55.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x56.png" xlink:type="simple"/></inline-formula></p><p>for every<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x57.png" xlink:type="simple"/></inline-formula>, except may be for a finite set of points.</p>Relation to the Mellin and the Fourier Transformations<p>Laplace transformation is closely related to an extended form of other popular transforms, particularly Mellin and Fourier. Both can be obtained through a change of variables. By setting</p><disp-formula id="scirp.66771-formula952"><label>. (18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x58.png"  xlink:type="simple"/></disp-formula><p>The Laplace transform (9) yields</p><disp-formula id="scirp.66771-formula953"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x59.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x60.png" xlink:type="simple"/></inline-formula> denote the Mellin transform, the Fourier transform and the Laplace transform respectively</p></sec><sec id="s4"><title>4. Laplace Transform for Solving Boundary Value Problems in Partial Differential Equation Arising in Financial Market</title><p>By change of variables<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x61.png" xlink:type="simple"/></inline-formula>, (5) becomes</p><disp-formula id="scirp.66771-formula954"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x62.png"  xlink:type="simple"/></disp-formula><p>with boundary conditions</p><disp-formula id="scirp.66771-formula955"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x63.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula956"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x64.png"  xlink:type="simple"/></disp-formula><p>and final time condition given by</p><disp-formula id="scirp.66771-formula957"><label>. (23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x65.png"  xlink:type="simple"/></disp-formula><p>Let the Laplace transform for the price of the European call option be defined as</p><disp-formula id="scirp.66771-formula958"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x66.png"  xlink:type="simple"/></disp-formula><p>and the inverse Laplace transform for the price of the European call option be given by</p><disp-formula id="scirp.66771-formula959"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x67.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x68.png" xlink:type="simple"/></inline-formula> is the Laplace operator and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x69.png" xlink:type="simple"/></inline-formula> is the Laplace transform with parameter w.</p><p>Taking the Laplace transform of (5) using (24) we have that</p><disp-formula id="scirp.66771-formula960"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x70.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.66771-formula961"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x71.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula962"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x72.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula963"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x73.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula964"><label>. (30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x74.png"  xlink:type="simple"/></disp-formula><p>Substituting (27), (28), (29) and (30) into (26) yields</p><disp-formula id="scirp.66771-formula965"><label>. (31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x75.png"  xlink:type="simple"/></disp-formula><p>Simplifying further and rearranging terms in (31) we have that</p><disp-formula id="scirp.66771-formula966"><label>. (32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x76.png"  xlink:type="simple"/></disp-formula><p>We consider the following two cases as follows.</p><p>CASE I</p><p>For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x77.png" xlink:type="simple"/></inline-formula>, (32) becomes</p><disp-formula id="scirp.66771-formula967"><label>. (33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x78.png"  xlink:type="simple"/></disp-formula><p>The general solution to (33) can be obtained as</p><disp-formula id="scirp.66771-formula968"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x79.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x80.png" xlink:type="simple"/></inline-formula> are the complementary solution to the homogeneous part of (33) which is of the form</p><disp-formula id="scirp.66771-formula969"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x81.png"  xlink:type="simple"/></disp-formula><p>and the particular solution respectively.</p><p>We assume that the solution to (33) is of the form</p><disp-formula id="scirp.66771-formula970"><label>. (36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x82.png"  xlink:type="simple"/></disp-formula><p>The first and the second derivatives of (36) are obtained as</p><disp-formula id="scirp.66771-formula971"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x83.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.66771-formula972"><label>. (38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x84.png"  xlink:type="simple"/></disp-formula><p>Substituting (36), (37) and (38) into (35), and simplifying further, we have that</p><disp-formula id="scirp.66771-formula973"><label>. (39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x85.png"  xlink:type="simple"/></disp-formula><p>Solving (39), we obtain the following roots</p><disp-formula id="scirp.66771-formula974"><label>(40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x86.png"  xlink:type="simple"/></disp-formula><p>Hence the complementary solution to the homogeneous part of (33) is obtained as</p><disp-formula id="scirp.66771-formula975"><label>(41)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x87.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x88.png" xlink:type="simple"/></inline-formula> are given by (40).</p><p>For the particular solution of (33), we assume that</p><disp-formula id="scirp.66771-formula976"><label>. (42)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x89.png"  xlink:type="simple"/></disp-formula><p>Using (42) and (33), and equating the coefficients of terms, we obtain</p><disp-formula id="scirp.66771-formula977"><label>(43)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x90.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula978"><label>. (44)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x91.png"  xlink:type="simple"/></disp-formula><p>Substituting (43) and (44) into the particular solution, we have that</p><disp-formula id="scirp.66771-formula979"><label>. (45)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x92.png"  xlink:type="simple"/></disp-formula><p>Substituting (41) and (45) into (34)</p><disp-formula id="scirp.66771-formula980"><label>. (46)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x93.png"  xlink:type="simple"/></disp-formula><p>Equation (46) is the general solution to (33) for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x94.png" xlink:type="simple"/></inline-formula>.</p><p>CASE II</p><p>For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x95.png" xlink:type="simple"/></inline-formula>, (33) becomes</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x96.png" xlink:type="simple"/></inline-formula>.</p><p>Following the above procedures, the general solution to the last equation is obtained as</p><disp-formula id="scirp.66771-formula981"><label>(47)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x97.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.66771-formula982"><graphic  xlink:href="http://html.scirp.org/file/4-7403149x98.png"  xlink:type="simple"/></disp-formula><p>Equation (47) coincides with the complementary solution of (33) given by (41).</p><p>In the case of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x99.png" xlink:type="simple"/></inline-formula>, we set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x100.png" xlink:type="simple"/></inline-formula> to ensure the boundedness of the derivative<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x101.png" xlink:type="simple"/></inline-formula>. In the case of</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x102.png" xlink:type="simple"/></inline-formula>to ensure that the option’s value approaches zero as the stock price goes to zero. The solutions for the two cases equations (46) and (47) become</p><disp-formula id="scirp.66771-formula983"><label>(48)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x103.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula984"><label>. (49)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x104.png"  xlink:type="simple"/></disp-formula><p>We want the option pricing function to be continuous and differentiable at the transition point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x105.png" xlink:type="simple"/></inline-formula>, Therefore, the values of the function and their first derivatives from (48) and (49) must equal to each other. These conditions can be used to solve for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x106.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x107.png" xlink:type="simple"/></inline-formula>. The function values and derivatives at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x108.png" xlink:type="simple"/></inline-formula> from (48) and (49) are given by</p><disp-formula id="scirp.66771-formula985"><label>(50)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x109.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula986"><label>(51)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x110.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula987"><label>(52)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x111.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula988"><label>. (53)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x112.png"  xlink:type="simple"/></disp-formula><p>Setting (50) = (52) and (51) = (53) and solving further, we obtain</p><disp-formula id="scirp.66771-formula989"><label>(54)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x113.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.66771-formula990"><label>. (55)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x114.png"  xlink:type="simple"/></disp-formula><p>Substituting (54) and (55) into (49) and (48), we have</p><disp-formula id="scirp.66771-formula991"><label>(56)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x115.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.66771-formula992"><label>(57)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x116.png"  xlink:type="simple"/></disp-formula><p>respectively. Equations (56) and (57) can also be written as</p><disp-formula id="scirp.66771-formula993"><label>(58)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x117.png"  xlink:type="simple"/></disp-formula><p>Equation (58) is the Laplace transform of the price of European call option which pays a dividend yield.</p><p>Theorem 4</p><p>If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x118.png" xlink:type="simple"/></inline-formula>, then the Laplace transform of the price of European call option with dividend yield given by</p><disp-formula id="scirp.66771-formula994"><label>(58a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x119.png"  xlink:type="simple"/></disp-formula><p>reduces to the Black-Scholes-Merton valuation formula</p><disp-formula id="scirp.66771-formula995"><label>(58b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x120.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.66771-formula996"><graphic  xlink:href="http://html.scirp.org/file/4-7403149x121.png"  xlink:type="simple"/></disp-formula><p>by means of the Laplace transform of the form</p><disp-formula id="scirp.66771-formula997"><label>(58c)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x122.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.66771-formula998"><label>(58d)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x123.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x124.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x125.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x126.png" xlink:type="simple"/></inline-formula> and g are arbitrary constants.</p><p>Proof: From (57) and (58a) we can write that</p><disp-formula id="scirp.66771-formula999"><label>. (59)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x127.png"  xlink:type="simple"/></disp-formula><p>Setting</p><disp-formula id="scirp.66771-formula1000"><label>(60)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x128.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.66771-formula1001"><label>. (61)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x129.png"  xlink:type="simple"/></disp-formula><p>Therefore, (59) becomes</p><disp-formula id="scirp.66771-formula1002"><label>. (62)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x130.png"  xlink:type="simple"/></disp-formula><p>Let us first consider the term</p><disp-formula id="scirp.66771-formula1003"><label>. (63)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x131.png"  xlink:type="simple"/></disp-formula><p>Using the values of</p><disp-formula id="scirp.66771-formula1004"><graphic  xlink:href="http://html.scirp.org/file/4-7403149x132.png"  xlink:type="simple"/></disp-formula><p>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x133.png" xlink:type="simple"/></inline-formula>.</p><p>Therefore (63) yields</p><disp-formula id="scirp.66771-formula1005"><graphic  xlink:href="http://html.scirp.org/file/4-7403149x134.png"  xlink:type="simple"/></disp-formula><p>Thus,</p><disp-formula id="scirp.66771-formula1006"><label>(64)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x135.png"  xlink:type="simple"/></disp-formula><p>Substituting the value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x136.png" xlink:type="simple"/></inline-formula> into (64) and simplifying further, we obtain</p><disp-formula id="scirp.66771-formula1007"><label>(65)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x137.png"  xlink:type="simple"/></disp-formula><p>Comparing (65) with (58c), we have that</p><disp-formula id="scirp.66771-formula1008"><label>(66)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x138.png"  xlink:type="simple"/></disp-formula><p>Taking the inverse Laplace transform of (65), we obtain</p><disp-formula id="scirp.66771-formula1009"><label>(67)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x139.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.66771-formula1010"><label>. (68)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x140.png"  xlink:type="simple"/></disp-formula><p>We also consider the term</p><disp-formula id="scirp.66771-formula1011"><label>. (69)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x141.png"  xlink:type="simple"/></disp-formula><p>Substituting the values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x142.png" xlink:type="simple"/></inline-formula> into (69) yields</p><disp-formula id="scirp.66771-formula1012"><label>. (70)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x143.png"  xlink:type="simple"/></disp-formula><p>Simplifying (70) further, we obtain</p><disp-formula id="scirp.66771-formula1013"><label>. (71)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x144.png"  xlink:type="simple"/></disp-formula><p>Once again we compare (71) with (58c), we deduce that</p><disp-formula id="scirp.66771-formula1014"><label>(72)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x145.png"  xlink:type="simple"/></disp-formula><p>Taking the Laplace transform of (72), we have that</p><disp-formula id="scirp.66771-formula1015"><label>(73)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x146.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.66771-formula1016"><label>. (74)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x147.png"  xlink:type="simple"/></disp-formula><p>The inverse Laplace transform of (62) is obtained as</p><disp-formula id="scirp.66771-formula1017"><label>. (75)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x148.png"  xlink:type="simple"/></disp-formula><p>Substituting (67), (68), (73) and (74) into (75) yields</p><disp-formula id="scirp.66771-formula1018"><graphic  xlink:href="http://html.scirp.org/file/4-7403149x149.png"  xlink:type="simple"/></disp-formula><p>This completes the proof.</p><p>Theorem 5</p><p>If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x150.png" xlink:type="simple"/></inline-formula>, then the Laplace transform of the price of European call option with dividend yield given by</p><disp-formula id="scirp.66771-formula1019"><label>(76)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x151.png"  xlink:type="simple"/></disp-formula><p>reduces to the Black-Scholes-Merton valuation formula given by</p><disp-formula id="scirp.66771-formula1020"><label>(76a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x152.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.66771-formula1021"><graphic  xlink:href="http://html.scirp.org/file/4-7403149x153.png"  xlink:type="simple"/></disp-formula><p>by means of the Laplace transform given by</p><disp-formula id="scirp.66771-formula1022"><label>(76b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x154.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.66771-formula1023"><label>(76c)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403149x155.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x156.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x157.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403149x158.png" xlink:type="simple"/></inline-formula> and g are arbitrary constants.</p><p>Remark 1</p><p>1) The proof of Theorem 5 follows from Theorem 4, since (56) and (57) have the same inverse Laplace transforms.</p><p>2 The above results show that the prices of European call option with dividend yield given by (56) and (57) coincide with the Black-Scholes-Merton model given by (58b) by means of (58c).</p></sec><sec id="s5"><title>5. Conclusion</title><p>Finance is one of the fastest developing areas in the modern corporate and banking world. In this paper, we have considered the boundary value problem in partial differential equation arising in financial market. We used a new approach for solving the Black-Scholes-Merton partial differential equation for the price of European call option which pays a dividend yield by means of the Laplace transform. The same approach can be used for European put option with dividend paying stock. The results show that the Laplace transform for the price of the European call option with dividend paying stock coincides with the Black-Scholes-Merton model; it is very effective and is a good tool for solving partial differential equations arising in financial market and other areas such as engineering and applied sciences.</p></sec><sec id="s6"><title>Cite this paper</title><p>Fadugba Sunday Emmanuel,Emeka Helen Oluyemisi, (2016) A New Approach for Solving Boundary Value Problem in Partial Differential Equation Arising in Financial Market. Applied Mathematics,07,840-851. doi: 10.4236/am.2016.79075</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.66771-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Black, F. and Scholes, M. (1973) The Pricing of Options and Corporate Liabilities. 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