<?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">ME</journal-id><journal-title-group><journal-title>Modern Economy</journal-title></journal-title-group><issn pub-type="epub">2152-7245</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/me.2015.66067</article-id><article-id pub-id-type="publisher-id">ME-57255</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></subj-group></article-categories><title-group><article-title>
 
 
  In-Arrears Interest Rate Derivatives under the 3/2 Model
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>oanna</surname><given-names>Goard</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>School of Mathematics and Applied Statistics, University of Wollongong, Wollongong, Australia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>08</day><month>06</month><year>2015</year></pub-date><volume>06</volume><issue>06</issue><fpage>707</fpage><lpage>716</lpage><history><date date-type="received"><day>15</day>	<month>May</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>15</month>	<year>June</year>	</date><date date-type="accepted"><day>18</day>	<month>June</month>	<year>2015</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><html>
 <head></head>
 
  Lie symmetry methods are used to find a closed form solution for in-arrears swaps under the 3/2 model 
  <img src="Edit_42466f32-4d7e-4a57-ae1f-687244b56cb8.bmp" alt="" />
  <b></b>
  . As well, approximate solutions are found for short-tenor in-arrears caplets and floorlets under the same interest rate model. Comparisons are made of the approximate option values with those obtained with a computationally-intensive numerical scheme. The approximate pricing is found to be substantially fast and easy to implement, while the relative errors with respect to the “true” prices are very small.
 
</html></p></abstract><kwd-group><kwd>In-Arrears Swaps</kwd><kwd> Interest Rate Options</kwd><kwd> 3/2 Model</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Interest rate derivatives are contracts whose value depends in some way on the level of interest rates. Swap contracts have existed since the early 1980s and since then there has been significant growth in terms of volume and diversity of contracts. In general an interest rate swap is an agreement between two companies, whereupon one company agrees to pay cash flows equal to the interest on a predetermined fixed rate on a notional principal, X, at regular set times <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x6.png" xlink:type="simple"/></inline-formula> (e.g. every 6 months) over the length of the contract time and in return receives interest at a floating rate (usually the LIBOR rate) on the same notional amount on the same set payment periods within the contract time. In the “plain vanilla” interest rate swap, the floating rate is the rate that prevails at the previous payment date, or in the case of the first payment, the rate at the opening of the contract. With LIBOR- in-arrears swaps, the floating rate paid on a payment date equals the rate observed on the payment date itself. Hence the floating leg cannot be valued as the sum of forward LIBORs.</p><p>Caplets and floorlets are the interest rate counterparts of European call and put options. Similar to vanilla swaps, the payoff of vanilla caplets and floorlets is based on the interest rate at the previous payment date whereas the payoff of in-arrears caplets and floorlets is based on the LIBOR rates at the actual time of the payment. Hence in-arrears derivatives are not as straightforward to price as their vanilla counterparts.</p><p>As stated by Chen and Sandmann [<xref ref-type="bibr" rid="scirp.57255-ref1">1</xref>] , typically when no assumptions are made about the term structure of interest rates, it is not possible to price these in-arrears products; and even when term structures are assumed, it is often not possible to find closed form solutions for the products. For this reason convexity adjustments (or convexity corrections) are often used by practitioners as a rule of thumb in the valuation of in-arrears term structure products. In [<xref ref-type="bibr" rid="scirp.57255-ref2">2</xref>] , Mallier and Alobaidi assume that risk-neutral interest rates follow the Cox-Ingersoll-Ross (CIR) model of the form</p><disp-formula id="scirp.57255-formula733"><graphic  xlink:href="http://html.scirp.org/file/7-7201061x7.png"  xlink:type="simple"/></disp-formula><p>where a, b and c are constants and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x8.png" xlink:type="simple"/></inline-formula> is a Wiener process under a risk-neutral probability measure. By using a Green’s function approach they manage to derive an analytical expression for in-arrears swaps.</p><p>It has been shown (see e.g. [<xref ref-type="bibr" rid="scirp.57255-ref3">3</xref>] ) that when the short-term interest rate, r, follows a stochastic differential equation of the form</p><disp-formula id="scirp.57255-formula734"><graphic  xlink:href="http://html.scirp.org/file/7-7201061x9.png"  xlink:type="simple"/></disp-formula><p>where a, b, γ and c are constants and dZ is an increment in a Wiener process under a real probability measure<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x10.png" xlink:type="simple"/></inline-formula>; the value of γ is very important in differentiating between the different models’ abilities to adequately capture the dynamics of interest rates. In particular the unconstrained estimate of γ by Chan et al. [<xref ref-type="bibr" rid="scirp.57255-ref3">3</xref>] was 1.5. This was agreed upon by Campbell et al. [<xref ref-type="bibr" rid="scirp.57255-ref4">4</xref>] who showed that the heteroskedasticity of the short rate was markedly reduced as γ increased from 1 to 1.5. In [<xref ref-type="bibr" rid="scirp.57255-ref5">5</xref>] , Ahn and Gao showed that the interest rate model</p><disp-formula id="scirp.57255-formula735"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x11.png"  xlink:type="simple"/></disp-formula><p>outperformed many of the popular interest rate models including the Vasicek and CIR models. The nonlinear drift in (1) implies a substantial nonlinear mean-reverting behaviour when the interest rate is above its long-run mean. Hence after a large interest rate rise, the interest rate can potentially quickly decrease, while after a low interest rate period, it can be slow to increase. It has also been shown that with a &gt; 0, r will always remain positive. This model was further improved (see e.g. [<xref ref-type="bibr" rid="scirp.57255-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.57255-ref7">7</xref>] )</p><disp-formula id="scirp.57255-formula736"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x12.png"  xlink:type="simple"/></disp-formula><p>to include a time-dependent long-run target allowing yield-curves to be fitted.</p><p>In [<xref ref-type="bibr" rid="scirp.57255-ref6">6</xref>] , a solution was found for the price of bonds with maturity T, under the assumption that the risk-neutral process for r has a similar form to (2), namely</p><disp-formula id="scirp.57255-formula737"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x13.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x14.png" xlink:type="simple"/></inline-formula> is a Wiener process under an equivalent risk-neutral measure<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x15.png" xlink:type="simple"/></inline-formula>. The solution given is</p><disp-formula id="scirp.57255-formula738"><label>(4a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x16.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.57255-formula739"><label>(4b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x17.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.57255-formula740"><label>(4c)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x18.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.57255-formula741"><label>(4d)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x19.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.57255-formula742"><label>(4e)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x20.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x21.png" xlink:type="simple"/></inline-formula> is the Kummer-M function (see e.g. [<xref ref-type="bibr" rid="scirp.57255-ref8">8</xref>] ). This was found by solving the governing partial differential Equation (PDE) for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x22.png" xlink:type="simple"/></inline-formula> namely</p><disp-formula id="scirp.57255-formula743"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x23.png"  xlink:type="simple"/></disp-formula><p>subject to the final condition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x24.png" xlink:type="simple"/></inline-formula> and boundary conditions<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x25.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x26.png" xlink:type="simple"/></inline-formula>.</p><p>In Section 3 of this paper, we extend the results in [<xref ref-type="bibr" rid="scirp.57255-ref6">6</xref>] by finding an exact solution for in-arrears swaps under the assumption that risk-neutral interest rates follow the time-dependent 3/2 model (3). As is typical with swap pricing, we divide the swap into a series of forward rate agreements (FRAs) and price each of these individually. The value of the swap is the sum of the individual FRAs. This was also the approach of Mallier and Alobaidi [<xref ref-type="bibr" rid="scirp.57255-ref2">2</xref>] . Then in Section 4 we derive analytic approximations for caplets and floorlets based on the time-dependent interest rate model (3) and compare their values with those obtained using an accurate (but computationally intensive) numerical scheme. Firstly however, we briefly summarise Lie’s classical symmetries method which is used to solve the PDEs in this paper.</p></sec><sec id="s2"><title>2. Lie’s Classical Symmetries Method</title><p>In essence, the classical method for finding symmetry reductions of a second-order PDE in one dependent variable V and two independent variables (r, t)</p><disp-formula id="scirp.57255-formula744"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x27.png"  xlink:type="simple"/></disp-formula><p>is to find a one-parameter Lie group of transformations in infinitesimal form</p><disp-formula id="scirp.57255-formula745"><label>(7a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x28.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.57255-formula746"><label>(7b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x29.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.57255-formula747"><label>(7c)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x30.png"  xlink:type="simple"/></disp-formula><p>which leaves (6) invariant. The coefficients <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x31.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x32.png" xlink:type="simple"/></inline-formula> of the infinitesimal symmetry are often referred to as the “infinitesimals”. This invariance requirement is determined by</p><disp-formula id="scirp.57255-formula748"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x33.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.57255-formula749"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x34.png"  xlink:type="simple"/></disp-formula><p>are vector fields that span the associated Lie algebra, and are called the infinitesimal generators of the transformation (7a-c), and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x35.png" xlink:type="simple"/></inline-formula> is the second extension (or second prolongation) of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x36.png" xlink:type="simple"/></inline-formula>, extended to the second jet space, co-ordinatised by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x37.png" xlink:type="simple"/></inline-formula> (see Chapter 2 in the book of Bluman and Kumei [<xref ref-type="bibr" rid="scirp.57255-ref9">9</xref>] ).</p><p>Then for known functions<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x38.png" xlink:type="simple"/></inline-formula>, invariant solutions V corresponding to (7a-c) satisfy the invariant surface condition (ISC)</p><disp-formula id="scirp.57255-formula750"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x39.png"  xlink:type="simple"/></disp-formula><p>which when solved as a first-order PDE by the method of characteristics, yields the functional form of the similarity solution in terms of an arbitrary function, i.e.</p><disp-formula id="scirp.57255-formula751"><graphic  xlink:href="http://html.scirp.org/file/7-7201061x40.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.57255-formula752"><graphic  xlink:href="http://html.scirp.org/file/7-7201061x41.png"  xlink:type="simple"/></disp-formula><p>and where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x42.png" xlink:type="simple"/></inline-formula> is an arbitrary function of invariant z for the symmetry. Substituting this functional form into (6) produces an ordinary differential Equation which one solves for the function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x43.png" xlink:type="simple"/></inline-formula>.</p><p>Further, for a final-value problem with the final condition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x44.png" xlink:type="simple"/></inline-formula> then we need a linear combination of generators such that condition (10) is satisfied at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x45.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x46.png" xlink:type="simple"/></inline-formula>i.e.</p><disp-formula id="scirp.57255-formula753"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x47.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x48.png" xlink:type="simple"/></inline-formula>can be found from the final condition. As well, for evolution equations <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x49.png" xlink:type="simple"/></inline-formula> can be found from the governing PDE (see [<xref ref-type="bibr" rid="scirp.57255-ref10">10</xref>] for details).</p></sec><sec id="s3"><title>3. LIBOR-in-Arrears Swaps</title><p>In this section we derive the analytic solution for the price of in-arrears swaps based on the risk-neutral interest rate model (3). The value given here is from the perspective of the receiver i.e. the investor who receives the fixed rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x50.png" xlink:type="simple"/></inline-formula> and pays the floating rate. As in [<xref ref-type="bibr" rid="scirp.57255-ref11">11</xref>] , we assume that the actual floating rate is the spot rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x51.png" xlink:type="simple"/></inline-formula>. The value to the payer i.e. the investor who pays the fixed and receives the floating, is simply the negative of the value given here.</p><p>Theorem 1. The value of an in-arrears swap with notional value 1 and fixed rate r<sub>0</sub> to a receiver with payment times T<sub>i</sub> every half year, when the interest rate follows the risk-neutral process (3) is given by</p><disp-formula id="scirp.57255-formula754"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x52.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.57255-formula755"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x53.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x54.png" xlink:type="simple"/></inline-formula> are given in (4b-e).</p><p>Proof. The value of an FRA to the investor who receives the fixed rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x55.png" xlink:type="simple"/></inline-formula> at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x56.png" xlink:type="simple"/></inline-formula> satisfies (5) subject to</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x57.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x58.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x59.png" xlink:type="simple"/></inline-formula>. As (5) is linear and homogeneous, and the solution to the</p><p>bond under (3) is already known (given by Equation (4a-e)), we need only find the solution to (5) subject to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x60.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x61.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x62.png" xlink:type="simple"/></inline-formula>. We denote this solution as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x63.png" xlink:type="simple"/></inline-formula>.</p><p>With the help of the package Dimsym [<xref ref-type="bibr" rid="scirp.57255-ref12">12</xref>] , we find that PDE (5) has the symmetry with generator</p><disp-formula id="scirp.57255-formula756"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x64.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.57255-formula757"><graphic  xlink:href="http://html.scirp.org/file/7-7201061x65.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.57255-formula758"><graphic  xlink:href="http://html.scirp.org/file/7-7201061x66.png"  xlink:type="simple"/></disp-formula><p>and where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x67.png" xlink:type="simple"/></inline-formula> are arbitrary constants and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x68.png" xlink:type="simple"/></inline-formula>.</p><p>In order for the final condition to satisfy (11) and the boundary conditions to be invariant we choose</p><disp-formula id="scirp.57255-formula759"><graphic  xlink:href="http://html.scirp.org/file/7-7201061x69.png"  xlink:type="simple"/></disp-formula><p>noting that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x70.png" xlink:type="simple"/></inline-formula>. Solving the ISC (10) corresponding to (14), then upon simplification, the functional form of the solution can be written as</p><disp-formula id="scirp.57255-formula760"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x71.png"  xlink:type="simple"/></disp-formula><p>Substitution of this functional form into (5) gives that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x72.png" xlink:type="simple"/></inline-formula> needs to satisfy</p><disp-formula id="scirp.57255-formula761"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x73.png"  xlink:type="simple"/></disp-formula><p>subject to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x74.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x75.png" xlink:type="simple"/></inline-formula> and where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x76.png" xlink:type="simple"/></inline-formula></p><p>Solving (16) for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x77.png" xlink:type="simple"/></inline-formula> we get</p><disp-formula id="scirp.57255-formula762"><graphic  xlink:href="http://html.scirp.org/file/7-7201061x78.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x79.png" xlink:type="simple"/></inline-formula>, and A and B are constants. Taking into consideration the boundary conditions we take B = 0 and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x80.png" xlink:type="simple"/></inline-formula>.</p><p>Undoing the change of variables we get the solution to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x81.png" xlink:type="simple"/></inline-formula> as given in (13).</p></sec><sec id="s4"><title>4. Asymptotic Solution for Caplets</title><p>Again assuming equidistant payment times<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula>, in a vanilla cap the contract holder receives <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula> at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula> X is the notional amount, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula>is the LIBOR rate at time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula> is the fixed cap rate. In a vanilla floor with fixed floor rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula> the payment size is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula> at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula>with the first payment time at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x94.png" xlink:type="simple"/></inline-formula> and last one at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x95.png" xlink:type="simple"/></inline-formula>. Hence the payment size at time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x96.png" xlink:type="simple"/></inline-formula> is based on the LIBOR rate at time<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x97.png" xlink:type="simple"/></inline-formula>. In contrast with in-arrears caps and floors the contract holder receives <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x98.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x99.png" xlink:type="simple"/></inline-formula> respectively at times<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x100.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x101.png" xlink:type="simple"/></inline-formula>so that the payment size at time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x102.png" xlink:type="simple"/></inline-formula> is actually based on the LIBOR rate at time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x103.png" xlink:type="simple"/></inline-formula> Each of the individual cashflows in a cap are called caplets and the individual cashflows in a floor are called floorlets. Hence caps and floors are sums of the individual caplets and floorlets respectively. Further, the value of a floor can be found from the cap-floor parity, namely “floor = cap − swap” (see e.g. [<xref ref-type="bibr" rid="scirp.57255-ref11">11</xref>] ). The most common valuation of interest rate caplets is via the Black-76 model [<xref ref-type="bibr" rid="scirp.57255-ref13">13</xref>] . Under this model the underlying interest rate is assumed to follow a log-normal distribution, which is not in agreement with empirical findings.</p><p>In this section we look at approximating the value of caplets and floorlets for short times to expiry, based on the risk-neutral interest rate model (3). We note that caplets and floorlets characteristically have short tenor, especially when the associated caps and floors have maturities of about one year. For simplicity we let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x104.png" xlink:type="simple"/></inline-formula> but the solutions derived can simply be multiplied by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x105.png" xlink:type="simple"/></inline-formula> We start with the caplet.</p><p>With<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x106.png" xlink:type="simple"/></inline-formula>, from Equation (5) the value of an in-arrears caplet <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x107.png" xlink:type="simple"/></inline-formula> with fixed cap rate K and expiry T satisfies</p><disp-formula id="scirp.57255-formula763"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x108.png"  xlink:type="simple"/></disp-formula><p>subject to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x109.png" xlink:type="simple"/></inline-formula> where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x110.png" xlink:type="simple"/></inline-formula>. To find an approximation to (17) for small <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x111.png" xlink:type="simple"/></inline-formula> we follow the method outlined by Howison [<xref ref-type="bibr" rid="scirp.57255-ref14">14</xref>] . We let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x112.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x113.png" xlink:type="simple"/></inline-formula> and assume the solution can be expanded as a series</p><disp-formula id="scirp.57255-formula764"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x114.png"  xlink:type="simple"/></disp-formula><p>Substituting (18) into (17) we get</p><disp-formula id="scirp.57255-formula765"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x115.png"  xlink:type="simple"/></disp-formula><p>Upon equating coefficients of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x116.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x117.png" xlink:type="simple"/></inline-formula>, and with consideration of corresponding boundary and initial con- ditions, we get that</p><disp-formula id="scirp.57255-formula766"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x118.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x119.png" xlink:type="simple"/></inline-formula>. However, the above solution is not differentiable at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x120.png" xlink:type="simple"/></inline-formula> and as we expect large Gamma</p><p>i..e <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x121.png" xlink:type="simple"/></inline-formula> near<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x122.png" xlink:type="simple"/></inline-formula>, this “outer” solution is not valid in the vicinity of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x123.png" xlink:type="simple"/></inline-formula>. For the “inner” solution where</p><p>r is near K, the second-order derivative with respect to r needs to be included in the differential system. We in-</p><p>troduce the inner variable <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x124.png" xlink:type="simple"/></inline-formula> and rescale V to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x125.png" xlink:type="simple"/></inline-formula>.</p><p>This leads to the equation</p><disp-formula id="scirp.57255-formula767"><graphic  xlink:href="http://html.scirp.org/file/7-7201061x126.png"  xlink:type="simple"/></disp-formula><p>i.e</p><disp-formula id="scirp.57255-formula768"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x127.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x128.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x129.png" xlink:type="simple"/></inline-formula>, to be solved subject to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x130.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x131.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x132.png" xlink:type="simple"/></inline-formula>.</p><p>We now expand</p><disp-formula id="scirp.57255-formula769"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x133.png"  xlink:type="simple"/></disp-formula><p>and substitute this form into (21). Equating terms of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x134.png" xlink:type="simple"/></inline-formula> we get</p><disp-formula id="scirp.57255-formula770"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x135.png"  xlink:type="simple"/></disp-formula><p>subject to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x136.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x137.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x138.png" xlink:type="simple"/></inline-formula>.</p><p>PDE (23) admits a six-dimensional finite Lie group of transformations (see e.g. [<xref ref-type="bibr" rid="scirp.57255-ref9">9</xref>] ). With consideration of the</p><p>initial and boundary conditions, we use the symmetry with generator<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x139.png" xlink:type="simple"/></inline-formula>. This leads to</p><p>an invariant solution of the form <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x140.png" xlink:type="simple"/></inline-formula> where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x141.png" xlink:type="simple"/></inline-formula>. Substitution of this invariant form into (23) yields the reduced equation</p><disp-formula id="scirp.57255-formula771"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x142.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.57255-formula772"><graphic  xlink:href="http://html.scirp.org/file/7-7201061x143.png"  xlink:type="simple"/></disp-formula><p><sup>1</sup>We use the results [<xref ref-type="bibr" rid="scirp.57255-ref14">14</xref>] that (i) if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x144.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x145.png" xlink:type="simple"/></inline-formula> then a particular solution is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x146.png" xlink:type="simple"/></inline-formula> and (ii) if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x147.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x148.png" xlink:type="simple"/></inline-formula> then a particular solution is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x149.png" xlink:type="simple"/></inline-formula></p><p>which needs to be solved subject to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x150.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x151.png" xlink:type="simple"/></inline-formula></p><p>Hence we get that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x152.png" xlink:type="simple"/></inline-formula> and so</p><disp-formula id="scirp.57255-formula773"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x153.png"  xlink:type="simple"/></disp-formula><p>Now collecting terms of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x154.png" xlink:type="simple"/></inline-formula> we get that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x155.png" xlink:type="simple"/></inline-formula> satisfies</p><disp-formula id="scirp.57255-formula774"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x156.png"  xlink:type="simple"/></disp-formula><p>subject to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x157.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x158.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x159.png" xlink:type="simple"/></inline-formula>. The solution to this problem is1</p><disp-formula id="scirp.57255-formula775"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x160.png"  xlink:type="simple"/></disp-formula><p>The two-term inner expansion can then be found by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x161.png" xlink:type="simple"/></inline-formula>.</p><p>We then match the inner and outer solutions to get a solution that is uniformly valid by calculating “outer + inner − common” where “common” is that part of the solution that is common to both. In this case as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x162.png" xlink:type="simple"/></inline-formula> the inner solution is the same as the outer solution and so the outer expansion is in fact the common expansion. This means that the inner expansion is uniformly valid. In terms of the original variables our approximate solution for a caplet with fixed cap rate K and short time to expiry T based on the risk-neutral interest rate (3) is then</p><disp-formula id="scirp.57255-formula776"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x163.png"  xlink:type="simple"/></disp-formula><p>In a similar way we get an approximate solution for the value of a floorlet with expiry T and fixed floor rate K as</p><disp-formula id="scirp.57255-formula777"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7201061x164.png"  xlink:type="simple"/></disp-formula><p>To test our approximate solutions we numerically solve PDE (17) using the mathematics software package MAPLE [<xref ref-type="bibr" rid="scirp.57255-ref15">15</xref>] (which uses a centered implicit finite-difference scheme) with step sizes of 10<sup>−</sup><sup>4</sup> and use this as a proxy for the true solution. We note that obtaining such numerical values is very labour-intensive and computationally-intensive whereas our approximate values are fast and easy-to-implement. Firstly, to test the accuracy of the finite-difference scheme, we used the method to numerically solve for in-arrears swap values i.e. Equation (5) subject to the conditions for the swap as given in Section 3, and compared these values to the exact solution (12). Using the parameter values<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x165.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x166.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x167.png" xlink:type="simple"/></inline-formula>and with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x168.png" xlink:type="simple"/></inline-formula> we found that for r values from 0.045 to 0.065, with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x169.png" xlink:type="simple"/></inline-formula>, absolute errors were of the order of 10<sup>−10</sup>; for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x170.png" xlink:type="simple"/></inline-formula> absolute errors were of the order of 10<sup>−6</sup> and for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x171.png" xlink:type="simple"/></inline-formula> absolute errors did not exceed 10<sup>−5</sup>.</p><p>Using the same parameter values as our testing procedure, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x172.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x173.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x174.png" xlink:type="simple"/></inline-formula>and with c = 1,</p><p>we computed signed percentage errors for caplet values i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x175.png" xlink:type="simple"/></inline-formula>, using the approximate solution</p><p>(28) and the “parity” value i.e “floorlet + swap” value using the exact value of the swap given by Equation (12) multiplied by −2, and the approximate floorlet value given in Equation (29). The results are listed in <xref ref-type="table" rid="table1">Table 1</xref>. Similarly in <xref ref-type="table" rid="table2">Table 2</xref> are the percentage errors of the approximate floorlet solutions given by (29) and the parity values found from “caplet-swap”.</p><p>From <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref> it can be seen that as expected, in general, the shorter times to expiry yield the more accurate results. In particular we note</p><p> Equation (28) yields values for caplets that are at-the-money (ATM) or in-the-money (ITM) that are above our exact values, with relative errors &lt;1.1% for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x176.png" xlink:type="simple"/></inline-formula>, &lt;2.15% for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x177.png" xlink:type="simple"/></inline-formula> and &lt;3.2% for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x178.png" xlink:type="simple"/></inline-formula>.</p><p> For caplets that are ATM or ITM, the parity formula yields the more accurate results where the value is dominated by the exact swap value. ATM options are slightly overpriced and mostly ITM options are underpriced slightly.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Signed percentage errors of caplet approximations with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x179.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x180.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x181.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x182.png" xlink:type="simple"/></inline-formula></title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x183.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x184.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x185.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >r</td><td align="center" valign="middle" >Equation (28)</td><td align="center" valign="middle" >Parity Value</td><td align="center" valign="middle" >Equation (28)</td><td align="center" valign="middle" >Parity Value</td><td align="center" valign="middle" >Equation (28)</td><td align="center" valign="middle" >Parity Value</td></tr><tr><td align="center" valign="middle" >0.045</td><td align="center" valign="middle" >−3.77%</td><td align="center" valign="middle" >54.9%</td><td align="center" valign="middle" >−0.45%</td><td align="center" valign="middle" >27.2%</td><td align="center" valign="middle" >0.614%</td><td align="center" valign="middle" >22.7%</td></tr><tr><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.657%</td><td align="center" valign="middle" >0.588%</td><td align="center" valign="middle" >1.3%</td><td align="center" valign="middle" >1.19%</td><td align="center" valign="middle" >2.06%</td><td align="center" valign="middle" >1.92%</td></tr><tr><td align="center" valign="middle" >0.055</td><td align="center" valign="middle" >0.844%</td><td align="center" valign="middle" >−0.04%</td><td align="center" valign="middle" >1.7%</td><td align="center" valign="middle" >−0.06%</td><td align="center" valign="middle" >2.63%</td><td align="center" valign="middle" >0.237%</td></tr><tr><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >0.73%</td><td align="center" valign="middle" >−0.01%</td><td align="center" valign="middle" >1.9%</td><td align="center" valign="middle" >−0.076%</td><td align="center" valign="middle" >2.85%</td><td align="center" valign="middle" >−0.037%</td></tr><tr><td align="center" valign="middle" >0.065</td><td align="center" valign="middle" >1.07%</td><td align="center" valign="middle" >&lt;10<sup>−</sup><sup>4</sup>%</td><td align="center" valign="middle" >2.13%</td><td align="center" valign="middle" >0.0028%</td><td align="center" valign="middle" >3.19%</td><td align="center" valign="middle" >−0.088%</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Signed percentage errors of floorlet approximations with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x186.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x187.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x188.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x189.png" xlink:type="simple"/></inline-formula></title></caption><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x190.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x191.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x192.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >r</td><td align="center" valign="middle" >Equation (29)</td><td align="center" valign="middle" >Parity Value</td><td align="center" valign="middle" >Equation (29)</td><td align="center" valign="middle" >Parity Value</td><td align="center" valign="middle" >Equation (29)</td><td align="center" valign="middle" >Parity Value</td></tr><tr><td align="center" valign="middle" >0.035</td><td align="center" valign="middle" >0.544%</td><td align="center" valign="middle" >&lt;10<sup>−</sup><sup>4</sup>%</td><td align="center" valign="middle" >1.1%</td><td align="center" valign="middle" >−0.0078%</td><td align="center" valign="middle" >1.57%</td><td align="center" valign="middle" >−0.051%</td></tr><tr><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >0.614%</td><td align="center" valign="middle" >−0.0091%</td><td align="center" valign="middle" >1.17%</td><td align="center" valign="middle" >−0.076%</td><td align="center" valign="middle" >1.70%</td><td align="center" valign="middle" >−0.146%</td></tr><tr><td align="center" valign="middle" >0.045</td><td align="center" valign="middle" >0.645%</td><td align="center" valign="middle" >−0.049%</td><td align="center" valign="middle" >1.29%</td><td align="center" valign="middle" >−0.022%</td><td align="center" valign="middle" >1.92%</td><td align="center" valign="middle" >0.067%</td></tr><tr><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.591%</td><td align="center" valign="middle" >0.682%</td><td align="center" valign="middle" >1.15%</td><td align="center" valign="middle" >1.38%</td><td align="center" valign="middle" >1.67%</td><td align="center" valign="middle" >2.11%</td></tr><tr><td align="center" valign="middle" >0.055</td><td align="center" valign="middle" >−1.69%</td><td align="center" valign="middle" >37.6%</td><td align="center" valign="middle" >0.066%</td><td align="center" valign="middle" >23.9%</td><td align="center" valign="middle" >0.866%</td><td align="center" valign="middle" >22.2%</td></tr></tbody></table></table-wrap><p> For the values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x193.png" xlink:type="simple"/></inline-formula> where caplets are out-of-the money (OTM), the floorlet values have small percentage errors but these errors are large in comparison to the corresponding caplet values thus producing very large parity percentage errors.</p><p> Equation (29) yields values for ATM and ITM floorlets with relative errors &lt;0.65% for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x194.png" xlink:type="simple"/></inline-formula>, &lt;1.3% for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x195.png" xlink:type="simple"/></inline-formula> and &lt;2% for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x196.png" xlink:type="simple"/></inline-formula>.</p><p> For floorlets that are ITM, the parity formula yields the more accurate results where the value is dominated by the exact swap value.</p><p> For the values of r where floorlets are out-of-the money (OTM), the caplet values have small percentage errors but these are large in comparison to corresponding floorlet values producing very large parity percentage errors.</p><p>The results suggest that parity values would be best to price ATM and ITM caplets and ITM floorlets; their values mostly slightly underpricing compared to the exact solution, while Equation (28) could be used to price OTM caplets and Equation (29) used to price ATM and OTM floorlets; their values producing small percentage errors especially (and surprisingly) for the larger values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x197.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x197.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7201061x198.png" xlink:type="simple"/></inline-formula>.</p><p>It should also be noted that similar percentage error results were found using other volatility coefficient values c.</p></sec><sec id="s5"><title>5. Discussion</title><p>The form of an interest rate model is crucial in the subsequent modelling of interest rate products and the accuracy of their valuations. It has been shown empirically by a number of authors that the 3/2 model (3) outperforms many of the popular interest rate models, such as the Vasicek and CIR models, in its ability to capture the actual behaviour of the interest rate. Including a free function of time in the drift further enhances the model’s ability to capture the interest rate dynamics. In this paper we have assumed the risk-neutral interest rate model (3) and extended the results in [<xref ref-type="bibr" rid="scirp.57255-ref6">6</xref>] by finding an exact solution for the value of in-arrears swaps and approximate values for caplets and floorlets with short times to expiry. As noted previously, caplets and floorlets have characteristically short tenors especially when the maturity of the cap/floor to which they belong, is about one year. The approximate option values have been shown to produce small percentage errors and in particular the parity values “caplet = floorlet + swap” and “floorlet = caplet − swap” produce best results for ATM and ITM caplets and ITM floorlets.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.57255-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Chen, A. and Sandmann, K. (2009) In Arrear Term Structure Products: No Arbitrage Pricing Bounds and the Convexity Adjustments. http://www.finance.uni-bonn.de/pdf-datei/download-datei-11</mixed-citation></ref><ref id="scirp.57255-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Mallier, R. and Alobaidi, G. (2004) Interest Rate Swaps under CIR. Journal of Computational and Applied Mathematics, 164-165, 543-554. http://dx.doi.org/10.1016/S0377-0427(03)00490-4</mixed-citation></ref><ref id="scirp.57255-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Chan, K., Karolyi, A., Longstaff, F. and Sanders, A. (1992) Empirical Comparison of Alternate Models of the Short-Term Interest Rate. Journal of Finance, 47, 1209-1227. http://dx.doi.org/10.1111/j.1540-6261.1992.tb04011.x</mixed-citation></ref><ref id="scirp.57255-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Campbell, J.Y., Lo, A.W. and MacKinlay, A.C. (1996) The Econometrics of Financial Markets. Princeton University Press, Princeton.</mixed-citation></ref><ref id="scirp.57255-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Ahn, D. and Gao, B. (1999) A Parametric Nonlinear Model of Term Structure Dynamics. Review of Financial Studies, 12, 721-762. http://dx.doi.org/10.1093/rfs/12.4.721</mixed-citation></ref><ref id="scirp.57255-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Goard, J. (2000) New Solutions to the Bond-Pricing Equation via Lie’s Classical Method. Mathematical and Computer Modelling, 32, 299-313. http://dx.doi.org/10.1016/S0895-7177(00)00136-9</mixed-citation></ref><ref id="scirp.57255-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Goard, J.M. and Hansen, N. (2004) Comparison of the Performance of a Time-Dependent Short-Interest Rate Model with Time-Dependent Models. Applied Mathematical Finance, 11, 147-164.  
http://dx.doi.org/10.1080/13504860410001686034</mixed-citation></ref><ref id="scirp.57255-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Abramowitz, M. and Stegun, I.A. (1965) Handbook of Mathematical Functions. Dover Publications, New York.</mixed-citation></ref><ref id="scirp.57255-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Bluman, G.W. and Kumei, S. (1989) Symmetries and Differential Equations. Springer-Verlag, New York. 
http://dx.doi.org/10.1007/978-1-4757-4307-4</mixed-citation></ref><ref id="scirp.57255-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Goard, J.M. (2003) Noninvariant Boundary Conditions. Applicable Analysis, 82, 473-481.  
http://dx.doi.org/10.1080/0003681031000109639</mixed-citation></ref><ref id="scirp.57255-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Wilmott, P. (1997) Derivatives: The Theory and Practice of Financial Engineering. John Wiley and Sons, New York.</mixed-citation></ref><ref id="scirp.57255-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Sherring, J. (1993) DIMSYM Users Manual. La Trobe University, Melbourne.</mixed-citation></ref><ref id="scirp.57255-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Black, F. (1976) The Pricing of Commodity Contracts. Journal of Financial Economics, 3, 167-179. 
http://dx.doi.org/10.1016/0304-405X(76)90024-6</mixed-citation></ref><ref id="scirp.57255-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Howison, S. (2005) Matched Asymptotic Expansions in Financial Engineering. Journal of Engineering Mathematics, 53, 385-406. http://dx.doi.org/10.1007/s10665-005-7716-z</mixed-citation></ref><ref id="scirp.57255-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Maplesoft (2008) Maple 12 Users Manual. Maplesoft, Waterloo.</mixed-citation></ref></ref-list></back></article>