<?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">OJS</journal-id><journal-title-group><journal-title>Open Journal of Statistics</journal-title></journal-title-group><issn pub-type="epub">2161-718X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojs.2012.25067</article-id><article-id pub-id-type="publisher-id">OJS-25549</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Effective Truncation of a Student’s &lt;i&gt;t&lt;/i&gt;-Distribution by Truncation of the Chi Distribution in a Chi-Normal Mixture
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>aniel</surname><given-names>T. Cassidy</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Engineering Physics, McMaster University, Hamilton, Canada</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>cassidy@mcmaster.ca</email></corresp></author-notes><pub-date pub-type="epub"><day>13</day><month>12</month><year>2012</year></pub-date><volume>02</volume><issue>05</issue><fpage>519</fpage><lpage>525</lpage><history><date date-type="received"><day>September</day>	<month>25,</month>	<year>2012</year></date><date date-type="rev-recd"><day>October</day>	<month>27,</month>	<year>2012</year>	</date><date date-type="accepted"><day>November</day>	<month>10,</month>	<year>2012</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  A Student’s 
  t-distribution is obtained from a weighted average over the standard deviation of a normal distribution, σ, when 1/σ is distributed as chi. Left truncation at q of the chi distribution in the mixing integral leads to an effectively truncated Student’s 
  t-distribution with tails that decay as exp (-q
  <sup>2</sup>t
  <sup>2</sup>). The effect of truncation of the chi distribution in a chi-normal mixture is investigated and expressions for the pdf, the variance, and the kurtosis of the t-like distribution that arises from the mixture of a left-truncated chi and a normal distribution are given for selected degrees of freedom 
  <u>&lt;</u>5. This work has value in pricing financial assets, in understanding the Student’s 
  t--distribution, in statistical inference, and in analysis of data.
 
</p></abstract><kwd-group><kwd>Asset Pricing; Student’s &lt;i&gt;t&lt;/i&gt;-Distribution; Cauchy; Truncation; Moments; Kurtosis</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>A Student’s t-distribution is used for statistical inference for small sample sizes [1,2]. Nadarajah [<xref ref-type="bibr" rid="scirp.25549-ref3">3</xref>] states that the Student’s t-distribution is the second most popular distribution, second in popularity only to the normal distribution.</p><p>In addition to statistical inference, the Student’s t-distribution has application in finance, wherein the t-distribution is found to fit the distribution of the logarithms of daily returns better than a normal distribution or indeed better than most any other distribution [4-9]. The number of degrees of freedom, <img src="9-1240148\411151a8-e907-4e97-aafd-b74af3242fd0.jpg" />, is found by least squares fitting to historical returns to be around 3 for daily returns of the DJIA and S&amp;P 500 indices [<xref ref-type="bibr" rid="scirp.25549-ref9">9</xref>], with increasing <img src="9-1240148\75124038-aba6-41fb-9a5c-b0948cbad465.jpg" /> for n-day returns,<img src="9-1240148\a2e0e6ae-6e69-4994-86af-c0de587f1d62.jpg" />.</p><p>The Student’s t-distribution also has application wherever a Cauchy (Lorentzian) distribution is employed, since a Student’s t-distribution with one degree of freedom is a Cauchy distribution.</p><p>The Student’s t-distribution offers support from <img src="9-1240148\e5621568-58d7-4bfd-82f9-a825e5b60235.jpg" /> to <img src="9-1240148\a7988578-0b3a-4710-9abb-6132259ec8eb.jpg" /> and has tails that decrease as <img src="9-1240148\8cbc6fe0-0f34-433f-b841-0a771ba57e78.jpg" /> for<img src="9-1240148\244d5eee-438c-4261-9c7f-93e52b5d23d4.jpg" />. This causes problems in finance as integrals needed to price financial instruments diverge for the logarithm of returns distributed as a Student’s t-distribution [9-11] and the frequency of occurrence of the logarithms of daily returns is fit well by Student’s t-distribution.</p><p>Truncation, capping, and modification of the t-distribution have been put forth as means to deal with the divergence [8,9,12]. Moriconi [<xref ref-type="bibr" rid="scirp.25549-ref8">8</xref>] multiplied the Student’s t-distribution by an exp<img src="9-1240148\03c3417b-c2d5-4c63-9124-aa57c2edd04c.jpg" /> to keep integrals finite in pricing options. Lim et al. [<xref ref-type="bibr" rid="scirp.25549-ref12">12</xref>] used a generalized t-distribution [<xref ref-type="bibr" rid="scirp.25549-ref13">13</xref>], which has a multiplicative term of exp<img src="9-1240148\d6e4d1bc-2c72-4ad8-a7c1-5a70038cb11c.jpg" />. Lim et al. [<xref ref-type="bibr" rid="scirp.25549-ref12">12</xref>] reported that the generalized t-distribution fit currency options better than any other probability density function (pdf) that was used. The results presented here provide a physical basis for understanding the origin of a multiplicative factor.</p><p>Praetz [<xref ref-type="bibr" rid="scirp.25549-ref4">4</xref>] and Gerig et al. [<xref ref-type="bibr" rid="scirp.25549-ref7">7</xref>] pointed out that a Student’s t-distribution is obtained from a mixture of a normal distribution with a standard deviation <img src="9-1240148\6aa0ab5f-078b-4f0f-918e-77d67f50ea39.jpg" /> that is distributed as an inverse chi distribution. If the support for the inverse chi distribution is taken to be zero to infinity, then a Student’s t-distribution is obtained from the mixture. For convenience, in this paper the reciprocal of <img src="9-1240148\57d460db-247c-4fac-a523-7c8bde18aadb.jpg" /> is denoted as<img src="9-1240148\95d88986-6b2a-4aea-822c-85474484c789.jpg" />, <img src="9-1240148\36773f86-cd4c-44f6-83a0-e4ad02f877b6.jpg" />, and <img src="9-1240148\60152dd4-7550-4246-ab8e-8ee3d6b8cb33.jpg" /> is distributed as chi,<img src="9-1240148\4679d6d4-4eb7-4b3a-a476-f9c815a77dcd.jpg" />:</p><disp-formula id="scirp.25549-formula148690"><label>(1)</label><graphic position="anchor" xlink:href="9-1240148\f13c688d-e937-4886-a0bf-7ac0593b3420.jpg"  xlink:type="simple"/></disp-formula><p>Using chi as defined above and a normal distribution with zero mean and standard deviation of<img src="9-1240148\895f5a48-d625-452e-b8b6-af0ea6e84898.jpg" />, the mixing integral, when evaluated from <img src="9-1240148\af33a945-7ee9-4968-83c1-49b5bc5c436a.jpg" /> to <img src="9-1240148\f29ff735-da86-4714-b67b-7b0e2f863773.jpg" /> yields a Student’s t-distribution</p><disp-formula id="scirp.25549-formula148691"><label>(2)</label><graphic position="anchor" xlink:href="9-1240148\8b19263e-bdb1-4081-8aef-d77d624c0063.jpg"  xlink:type="simple"/></disp-formula><p>with a mean of zero, <img src="9-1240148\f12cd8ce-098b-47dc-a38e-d4bc926fc46b.jpg" />degrees of freedom, and a scale parameter of<img src="9-1240148\674f4ffc-54b0-4c57-9077-6eaf1a0ba247.jpg" />. The parameters for the chi distribution were chosen to yield a Student’s t-distribution, <img src="9-1240148\4c2794fc-7355-4fb0-b4eb-c9b858f22218.jpg" />, with a mean of zero, <img src="9-1240148\e5aa8c1e-e70a-4b7f-bad2-17138028785d.jpg" />degrees of freedom, and a scale parameter of<img src="9-1240148\d5556dc4-2ce6-4256-806c-41a9cebbae81.jpg" />.</p><p>If a chi distribution for the reciprocal of <img src="9-1240148\183aa790-874f-414e-a388-59ee243d3e2b.jpg" /> is left truncated, then the result of the mixing integral with the left-truncated chi distribution is a t-like distribution that has exponentially decaying tails. This result is demonstrated for<img src="9-1240148\c35164d3-5817-4e39-90f5-ef44ccc545b8.jpg" />. The integrals involved can be evaluated analytically for odd<img src="9-1240148\6785098b-0467-435c-b820-cbed91e51077.jpg" />. Small values of <img src="9-1240148\a75e62fb-df03-4159-95a5-c23ca7c902f9.jpg" /> are of interest.</p><p>The contribution to a <img src="9-1240148\683c8bbc-cec8-4070-a8eb-55f1a8713cac.jpg" /> Student’s t-distribution, <img src="9-1240148\9d918504-723c-47cb-8086-f32fbc9eb30c.jpg" />, from values in the left-hand wing of the chi distribution for <img src="9-1240148\67c23c13-a6b1-44a6-b48a-0700438ddc7a.jpg" /> is given by</p><p><img src="9-1240148\8032a2bd-e61a-4071-b734-7821d42dd02a.jpg" />(3)</p><p>whereas the contribution from values in the right-hand wing of the chi distribution for <img src="9-1240148\16a6eb38-55c1-46c1-b98f-9eb91f328762.jpg" /> is given by</p><disp-formula id="scirp.25549-formula148692"><label>(4)</label><graphic position="anchor" xlink:href="9-1240148\ef4d7152-7646-42b3-a57a-f7bac84a2c0e.jpg"  xlink:type="simple"/></disp-formula><p>It is interesting to note that the sum of the contributions from Equations (3) and (4) form a full Student’s t-distribution (in this case the mixing integral has been written as the sum of two exhaustive and exclusive regions: <img src="9-1240148\20a273a5-1975-402f-b625-60c81fe8b9ac.jpg" />and<img src="9-1240148\b2474fef-c63c-412c-a661-3bc9bf938201.jpg" />), and that the right-hand contribution has an exponentially decaying tail. As a result, any pdf that does not include the left-hand contribution from the chi distribution for the reciprocal of the standard deviation in a chi-normal mixture will have tails that decay as exp<img src="9-1240148\7d6da9d9-7576-43e7-bfa0-865e878a8705.jpg" />.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref> is a plot of a Student’s t-distribution with <img src="9-1240148\6be04f72-21e3-470e-a349-94f81370d819.jpg" /> degrees of freedom and the contributions to the t-distribution from the right-hand wing of the chi distribution and from the left-hand wing of the chi dis-</p><p>tribution. <xref ref-type="fig" rid="fig1">Figure 1</xref> clearly shows that large values of the standard deviation <img src="9-1240148\090ec42e-a7e2-4cfb-8aa0-40cbb7f535ed.jpg" /> in the mixture give rise to the fat tails of the t-distribution. The large values of the standard deviation occur for small values of the reciprocal of the standard deviation. For <xref ref-type="fig" rid="fig1">Figure 1</xref>, the wing of the chi distribution was truncated for an area of 0.01 in the wing. The small values of the standard deviation (large reciprocal; right wing) make a negligible contribution to the value of the Student’s t-distribution. The long tic mark at <img src="9-1240148\b134c8f0-5a5d-4eaa-9e3b-3835708f3e98.jpg" /> marks the point where the area in each tail of the Student’s t-distribution equals 0.005, for a total area of 0.01.</p><p>The slowly decaying power tails of the t-distribution with increasing t results in the divergence of moments and of integrals required to price financial instruments that are based on a log Student’s t-distribution. The results presented in <xref ref-type="fig" rid="fig1">Figure 1</xref> are interesting on two levels. One level is intrinsic interest in understanding the Student’s t-distribution and the other level is use. The results show the origins of the slowly decaying power tails of Student’s t-distributions and suggest an approach to deal with the divergence of moments and integrals based on the t-distribution.</p><p>Left truncation of the chi distribution for the reciprocal of the standard deviation to allow for only physically possible values of the standard deviation <img src="9-1240148\426e1d2e-9fa7-4e92-9c28-78da98189f74.jpg" /> will impart exponentially decaying tails to the resulting t-like distribution from the chi-normal mixture. It is unlikely that<img src="9-1240148\53d90137-ee3b-4c6c-a535-d427edb54bfe.jpg" />. A value of <img src="9-1240148\a2c89887-1be9-4cef-a96e-443422a4f7a1.jpg" /> implies no variability and a value of <img src="9-1240148\bef2628f-e158-47cd-b586-022ac9e8f53b.jpg" /> implies infinite variability.</p><p>In the following sections, expressions for the probability density function (pdf), the variance, and the kurtosis are given for several small values of <img src="9-1240148\3427fcb8-9ddc-456c-9475-519050b3e494.jpg" /> for t-like distributions that are obtained by left truncation of a chinormal mixture. In addition, the first several terms for power series expansions of the variance and kurtosis are given. These power series demonstrate the effect of the left truncation on the moments. Since the power series are valid only for small amounts of truncation, <xref ref-type="fig" rid="fig2">Figure 2</xref> is presented. This figure shows the magnitude of the parameters involved for a left truncation of the chi distribution,<img src="9-1240148\f9719f1a-12c0-477e-b621-6cf973d8eee8.jpg" />. After <xref ref-type="fig" rid="fig2">Figure 2</xref>, some general definitions are given.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> plots the cumulative density function (CDF)</p><p><img src="9-1240148\78602ea1-a7f5-44f9-a2f6-4c08aadbac80.jpg" />for small values of the independent variable <img src="9-1240148\e9bcda77-9d4a-478c-b2ac-6e3e7ca36fc6.jpg" /> for the chi distribution in the mixing integral that yields a Student’s t-distribution with v = 1, 2, 3, 5 and 9 degrees of freedom. The long tic marks give the values (q = 0.0125, 0.10, 0.196, 0.333, 0.482) for which the CDF<img src="9-1240148\634d0a05-d7dd-4f8d-9166-128dfc8c373f.jpg" />. <xref ref-type="fig" rid="fig2">Figure 2</xref> allows an appreciation of the differences amongst the chi distributions for different degrees of freedom and of the magnitudes of the numbers involved.</p><p>The probability that<img src="9-1240148\d73e26ec-16f5-4f87-a964-a02f9b5064c4.jpg" />, <img src="9-1240148\9516512c-341d-43d2-a2ed-8e6ba2f7572c.jpg" />, is needed to normalize properly a truncated chi distribution. A left-truncated chi distribution <img src="9-1240148\f0ceceb2-f406-4b9e-92d7-fdd0a2aa6795.jpg" /> is zero for values<img src="9-1240148\db03686b-c45a-45be-b038-87d942eb8a4c.jpg" />:</p><disp-formula id="scirp.25549-formula148693"><label>(5)</label><graphic position="anchor" xlink:href="9-1240148\b110a5ac-20f0-4877-ac63-8353023b1ac6.jpg"  xlink:type="simple"/></disp-formula><p><img src="9-1240148\94defcb8-88c6-40a9-87b1-b408d79b49cd.jpg" />is the pdf for a mixture of a left-truncated chi and normal distribution. If <img src="9-1240148\13ae0d18-7444-4900-a35a-d01c3962ddaa.jpg" /> then <img src="9-1240148\f827729f-488a-406f-8858-b27ce57625f1.jpg" /> would be a Student’s t-distribution with <img src="9-1240148\83bad901-f352-4705-bcbc-6d7b98b4df9f.jpg" /> degrees of freedom and scale parameter<img src="9-1240148\21a55a37-3593-40f4-9592-e3aca4240d50.jpg" />. An explicit expression for <img src="9-1240148\b0f0c263-0672-4125-b97e-3ee2278d63fe.jpg" /> is</p><disp-formula id="scirp.25549-formula148694"><label>(6)</label><graphic position="anchor" xlink:href="9-1240148\72e73d19-b325-4653-ae5b-ee2f140ffd63.jpg"  xlink:type="simple"/></disp-formula><p><img src="9-1240148\a62c9021-7ed6-40d0-9413-afe99d37b380.jpg" />is the variance of the pdf<img src="9-1240148\8f6fe046-5070-4feb-bafa-8c9b35cc7db0.jpg" />,</p><disp-formula id="scirp.25549-formula148695"><label>(7)</label><graphic position="anchor" xlink:href="9-1240148\b9ad1293-8d56-48c6-9e6c-8c24eef99b7f.jpg"  xlink:type="simple"/></disp-formula><p>and <img src="9-1240148\8597e5db-da32-4709-b884-81e946953635.jpg" /> is the kurtosis of the pdf<img src="9-1240148\e5aa0929-4ebe-453d-a5fc-81b7c7ad790f.jpg" />,</p><disp-formula id="scirp.25549-formula148696"><label>(8)</label><graphic position="anchor" xlink:href="9-1240148\67cb2bde-934c-45e2-a060-2857839b43b7.jpg"  xlink:type="simple"/></disp-formula><p>This paper provides information on the effective truncation of a Student’s t-like distribution when the chi distribution for the reciprocal of the standard deviation is left-truncated. It is shown that the tails of the effectively truncated t-distribution go as exp<img src="9-1240148\6575f7b8-abdb-42a1-bc59-189f0c123531.jpg" />. The contribution <img src="9-1240148\886ba9a0-1c4f-4907-8540-e88031ebabc4.jpg" /> to an odd <img src="9-1240148\a1cc1981-6254-4c34-bd28-b69337fff552.jpg" /> Student’s t-distribution from values of <img src="9-1240148\43ef3a6f-dd88-4bed-a5bb-0f0141c32252.jpg" /> for a chi-normal mixture, i.e., Equation (4) evaluated for odd<img src="9-1240148\554414aa-ff7b-4b46-a697-289e14342f9e.jpg" />, is given by (see Equation (9) below).</p><p>The expression, which decreases with t as exp<img src="9-1240148\9e26ec0b-3b9a-4658-b026-484d67cc6b17.jpg" />, was obtained from an examination of the expressions for <img src="9-1240148\348ccdf6-9a12-43e4-9a0b-fd287e3288f1.jpg" /> for <img src="9-1240148\547946f0-bb4f-425d-9c71-7f6269272714.jpg" /> and by comparison with the general case for odd<img src="9-1240148\9b763c9a-aeb6-4d0b-8002-8f96c2cd7ccc.jpg" />. Clearly, left truncation of the chi distribution for the reciprocal of the standard deviation in a chi-normal mixture removes the fat tails of the Student’s t-distribution.</p></sec><sec id="s2"><title>2. Results</title><p>Expressions for some of the low<img src="9-1240148\90c89392-b229-46c7-8972-8f8f5dc6b4ce.jpg" />, effectively truncated Student’s t-distributions and moments are given in the following subsections. For a Student’s t-distribution the variance equals <img src="9-1240148\edeed404-6511-4158-8edc-61246e4d33fd.jpg" /> and exists only for<img src="9-1240148\e88ce4ef-bfed-4659-8469-eb0f1db968b4.jpg" />. The kurtosis equals <img src="9-1240148\0237d9db-aec3-4e46-94f7-cac7275d7f40.jpg" /> and exists only for<img src="9-1240148\164929db-d7d5-4165-ae8d-0998d9fb0af4.jpg" />. For effectively truncated Student’s t-distributions (i.e., truncation of the large values of the standard deviation in the chi mixing distribution), the moments exist for all<img src="9-1240148\d4661e92-b87c-4c38-a5a7-fe206858b468.jpg" />.</p><sec id="s2_1"><title>2.1. v = 1 (Cauchy or Lorentzian Distribution)</title><p>The pdf for a mixture of a left-truncated chi distribution for <img src="9-1240148\ab89994f-e220-49b4-9481-2d4d0928d0b5.jpg" /> and <img src="9-1240148\06391810-ced0-4e55-91de-5075d1c3c937.jpg" /> and a normal distribution is</p><disp-formula id="scirp.25549-formula148697"><label>(10)</label><graphic position="anchor" xlink:href="9-1240148\48da50be-0d03-4170-9553-56a02049d4ef.jpg"  xlink:type="simple"/></disp-formula><p>The tails of the pdf decrease as exp<img src="9-1240148\5f990814-d762-40e7-854c-e46e44a3b5a0.jpg" /> for non-zero<img src="9-1240148\301643a7-b8c6-4af3-8cc6-4e4bba6563f4.jpg" />.</p><disp-formula id="scirp.25549-formula148698"><label>(9)</label><graphic position="anchor" xlink:href="9-1240148\bc59b66d-c7dc-46b5-ba39-20f154edd4b6.jpg"  xlink:type="simple"/></disp-formula><p>The first moment for <img src="9-1240148\68d2128f-c888-48aa-a96f-4702ca76a1bf.jpg" /> exists for the effectively truncated <img src="9-1240148\3ed04a1e-5854-448b-9831-e456a668a349.jpg" /> t-distribution and is given by</p><disp-formula id="scirp.25549-formula148699"><label>(11)</label><graphic position="anchor" xlink:href="9-1240148\c4b8bcc4-7d4b-4a86-9507-a7dcdff77e91.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="9-1240148\0d43d7bd-64f4-4a77-993b-d132df6d2230.jpg" /> is Euler’s contant and Ei() is the exponential integral. The series expansion is valid for<img src="9-1240148\4f8c2340-a563-4f3c-9fc3-de55f36d8bc8.jpg" />. The series expansion shows a logarithmic divergence as <img src="9-1240148\d5ee1373-0dd7-4937-a9c0-e0389230571c.jpg" /> approaches zero, as expected for a Cauchy distribution.</p><p>The <img src="9-1240148\f5a026d5-f6d6-46d8-9518-ee86ca78e51a.jpg" /> variance is given by</p><disp-formula id="scirp.25549-formula148700"><label>(12)</label><graphic position="anchor" xlink:href="9-1240148\987c425e-58a9-4737-a82a-dda8d32f5326.jpg"  xlink:type="simple"/></disp-formula><p>is proportional to<img src="9-1240148\e39b23b8-a948-4023-b5f2-3cc1a231c984.jpg" />, remains finite for<img src="9-1240148\11f2ec6e-3b39-4a66-9040-9297a21e4a7b.jpg" />, and diverges as <img src="9-1240148\bc85245a-b828-4075-bdbd-c433548b4d9f.jpg" /> as <img src="9-1240148\4e515c92-29de-4c97-86f3-a547b0e6076a.jpg" /> approaches zero.</p><p>An exact expression for the <img src="9-1240148\f1ba020c-7b85-4a4b-a86a-2c8d75b00389.jpg" /> kurtosis can be found, but the expression is long and cumbersome. The series expansion</p><disp-formula id="scirp.25549-formula148701"><label>(13)</label><graphic position="anchor" xlink:href="9-1240148\3264aad5-1d76-4b6a-95c6-f0ebd7b58ca5.jpg"  xlink:type="simple"/></disp-formula><p>shows that the <img src="9-1240148\3ee30d1f-a863-4be7-82bb-00362abb4828.jpg" /> kurtosis is proportional to <img src="9-1240148\ca8cbde5-7597-49e5-b408-6a428617700a.jpg" /> and hence stays finite for<img src="9-1240148\d762cbd9-c266-44cf-a438-7b239c4003d4.jpg" />. Both the variance and the kurtosis are not defined for a Cauchy distribution, i.e., for a Student’s t-distribution with <img src="9-1240148\c674be0a-e276-47df-b1c5-b9cb9d96017a.jpg" /> and a region of support from <img src="9-1240148\ec1bdfaf-5158-475b-9fb7-8d18c817b386.jpg" /> to<img src="9-1240148\2a5f80d2-5ca0-4e9b-b9a3-ddeaff747ace.jpg" />.</p></sec><sec id="s2_2"><title>2.2. v = 2</title><p>The pdf, <img src="9-1240148\aa7a4d77-adc2-48d0-a940-be12441b9132.jpg" />, for a mixture of a left-truncated chi distribution for <img src="9-1240148\d100e52d-31a5-4862-a285-02f9c62d2a47.jpg" /> and <img src="9-1240148\042a617c-3232-4e58-b296-89b8c34ed5d7.jpg" /> with a normal pdf is</p><disp-formula id="scirp.25549-formula148702"><label>(14)</label><graphic position="anchor" xlink:href="9-1240148\810a5421-fa42-402d-866b-0ca07a311a0a.jpg"  xlink:type="simple"/></disp-formula><p>The first term in the series expansion is equal to<img src="9-1240148\4cc26edf-0ede-47ba-9aa7-3468430cd2ec.jpg" />.</p><p><img src="9-1240148\a2c90462-87eb-45bd-9143-157b78472a02.jpg" />has tails that decrease as exp<img src="9-1240148\e4f5504b-e8de-46f9-b520-bdb4f3fe6c16.jpg" /> for non-zero<img src="9-1240148\f7614a1e-7066-46dc-9f50-7df7d55999c0.jpg" />, since <img src="9-1240148\1276e943-88f9-4316-8a23-7eac225a91e7.jpg" /> for large x. For large qt,</p><disp-formula id="scirp.25549-formula148703"><label>(15)</label><graphic position="anchor" xlink:href="9-1240148\91285b23-3847-482a-b982-7b0f27d2ccde.jpg"  xlink:type="simple"/></disp-formula><p>Simple, analytic expression for the moments for even values of v could not be found.</p></sec><sec id="s2_3"><title>2.3. v = 3</title><p>The <img src="9-1240148\1362e5a1-ef75-4f5a-b578-752628fb8a8f.jpg" /> pdf, <img src="9-1240148\392705c2-a028-4247-813d-fdb40669d669.jpg" />, equals</p><disp-formula id="scirp.25549-formula148704"><label>(16)</label><graphic position="anchor" xlink:href="9-1240148\a8746182-ebfb-44ef-8a0b-90eb75d05d7f.jpg"  xlink:type="simple"/></disp-formula><p>and has tails that decrease as exp<img src="9-1240148\096ebf5b-303c-4799-b327-8ece4291baef.jpg" /> for non-zero q.</p><p>The <img src="9-1240148\95371ba7-a520-4799-9d4b-b447cc5e3c1f.jpg" /> variance is given by</p><disp-formula id="scirp.25549-formula148705"><label>(17)</label><graphic position="anchor" xlink:href="9-1240148\3d15fea1-b8b5-4172-8d71-1b9d9ccf36bf.jpg"  xlink:type="simple"/></disp-formula><p>and approaches <img src="9-1240148\f6bd1b90-646d-4748-8d71-b8ba197cbeb9.jpg" /> as q approaches zero. This is expected since the variance for a Student’s t-distribution exists for <img src="9-1240148\997e68f5-d1a2-4a5f-b214-ae3b190f91f9.jpg" /> and equals <img src="9-1240148\a5f1420e-4430-4452-9b91-28d2b55b0eeb.jpg" /> or <img src="9-1240148\7a62067d-d2de-4b3a-82b3-eb9717a82b3b.jpg" /> for v = 3.</p><p>A series expansion for the <img src="9-1240148\b9ffd641-e270-4248-98f7-68772087c656.jpg" /> kurtosis (the exact expression is long and cumbersome) is</p><disp-formula id="scirp.25549-formula148706"><label>(18)</label><graphic position="anchor" xlink:href="9-1240148\0af45ee4-eaa4-48bc-a501-cb24ae6a567f.jpg"  xlink:type="simple"/></disp-formula><p>and diverges as <img src="9-1240148\318f87f6-a516-418d-8041-600b2912027f.jpg" /> as q approaches zero. The kurtosis for a Student’s t-distribution is defined only for<img src="9-1240148\881831bc-c7dc-40c5-bdf1-a2961b554412.jpg" />.</p></sec><sec id="s2_4"><title>2.4. v = 5</title><p>The series expansion for the <img src="9-1240148\daedbaf9-aaae-4532-a574-c76485c54d2c.jpg" /> variance shows a weak dependence on the left truncation. To lowest order in q, the <img src="9-1240148\533c48ab-7867-4277-847b-ff81d9145185.jpg" /> variance has a cubic dependence on q. The curves of <xref ref-type="fig" rid="fig2">Figure 2</xref> show that the chi distribution has decreasing area in the left for small q as v increases.</p><disp-formula id="scirp.25549-formula148707"><label>(19)</label><graphic position="anchor" xlink:href="9-1240148\4c4a6f3f-d6e7-462e-be61-d9b8b00d3bc0.jpg"  xlink:type="simple"/></disp-formula><p>The series expansions for the <img src="9-1240148\0d448604-0b77-4614-b79b-573964d756d7.jpg" /> kurtosis is given by</p><disp-formula id="scirp.25549-formula148708"><label>(20)</label><graphic position="anchor" xlink:href="9-1240148\42fbb2db-0d91-4af3-9218-a0e03aafff30.jpg"  xlink:type="simple"/></disp-formula><p>The <img src="9-1240148\ffc78896-7941-4dd5-8902-e3bd0f99393b.jpg" /> kurtosis is finite for<img src="9-1240148\781b874a-2e06-4034-8375-95dbb113f4eb.jpg" />. The series expansion is a linear decrease in q for small q.</p><p>For<img src="9-1240148\bc8313b5-44b4-49d6-b549-1e970c10c1e0.jpg" />, the first two terms of the alternating series for the expansion of the kurtosis are<img src="9-1240148\cf50c696-121a-427b-8c61-3922d5216ef2.jpg" />. For <img src="9-1240148\ff4ad96d-7f64-4faa-84c2-87d1774870f7.jpg" /> the kurtosis is not impacted by a truncation for small<img src="9-1240148\9ae35b84-74e7-45cf-ad88-41613c1fb0f0.jpg" />.</p></sec></sec><sec id="s3"><title>3. Application</title><p>Application of the effectively truncated Student’s t-distribution to pricing a European call option is given in this section.</p><p>The value of a European call option at the time of expiration, <img src="9-1240148\e74ba393-314d-4283-b842-a50245bdcec6.jpg" />, is the expectation of the maximum value of<img src="9-1240148\29be4f95-14c3-422e-8ff6-74c869978cc5.jpg" />, <img src="9-1240148\1e567195-13a2-4b69-98b0-5ef126a8cbf0.jpg" />, where <img src="9-1240148\bded8b3c-1b29-4e70-ada4-5db353ba95c6.jpg" /> is the price of a stock at time T, <img src="9-1240148\8721d75d-0523-4ad0-8986-4605b73a1adf.jpg" />is the strike price at time T, T is the time when the option expires, and <img src="9-1240148\af2fd644-38da-47d8-a878-8fda0d7c4da7.jpg" /> is the expectation operator [<xref ref-type="bibr" rid="scirp.25549-ref9">9</xref>]. It is not necessary to solve a partial differential equation to find the price of an option [9-11]. The desired quantity<img src="9-1240148\ad158f12-9414-4b0f-b822-9d585c48ed10.jpg" />, which is the value of the option at time<img src="9-1240148\85471bf0-23a6-439e-b467-0a9ea19d7961.jpg" />, is obtained from the expected time value of money. If <img src="9-1240148\31491cf1-7e07-49c2-83a0-b0a6c7c25414.jpg" /> is the risk free rate as a function of time t, then <img src="9-1240148\88dd0437-4b59-4533-943d-652270a89f21.jpg" /> when the risk free rate is assumed to be time independent. This is a standard assumption in the derivation of the Black-Scholes formula.</p><p>Let <img src="9-1240148\b3cbc159-20a7-453a-b956-fc595412a3e5.jpg" /> be the value of the stock at time T where <img src="9-1240148\77b2f260-116e-41d3-b222-a9d3a918f669.jpg" /> is a random variable, and where both <img src="9-1240148\8a052103-c0ae-4233-8cc0-389a7baa0616.jpg" /> and the volatility <img src="9-1240148\7da24904-a22f-4caf-90d9-74ceeb92994c.jpg" /> do not depend on the random variable<img src="9-1240148\756a22d4-be15-45d1-9688-3c33f2c135ed.jpg" />.</p><p>In terms of the pdf for<img src="9-1240148\25abc898-ad78-4f80-8c31-52d4d65304fe.jpg" />, <img src="9-1240148\b934e05c-4b8d-429f-8ace-4ba744427b5d.jpg" />, the value of the option at time T is</p><disp-formula id="scirp.25549-formula148709"><label>(21)</label><graphic position="anchor" xlink:href="9-1240148\9d2fbc6d-c2c7-45cf-958e-ac7aab3becd5.jpg"  xlink:type="simple"/></disp-formula><p>The value of <img src="9-1240148\fce446d6-e186-4fa9-93e6-4153ecf256e1.jpg" /> is determined by the requirements that the process be fair (i.e., the process is a martingale) and that the development in time of the price include the time value of money [<xref ref-type="bibr" rid="scirp.25549-ref9">9</xref>]. This requires that</p><p><img src="9-1240148\e49b42fd-deb7-4c2c-91d5-49741c772d78.jpg" />where <img src="9-1240148\c86b5a17-e9d2-4dcf-8b08-9970f94f209b.jpg" /> is the value of the stock at time 0.</p><p>If <img src="9-1240148\bb42afd5-4dd1-45e3-86e8-5882249a3dd0.jpg" /> is normally distributed, then <img src="9-1240148\6070c28b-3712-49f2-a880-84b81c67a01a.jpg" /> follows a log normal distribution, <img src="9-1240148\694d1c1e-1c15-4b74-b65e-7b5704ee3997.jpg" />, and the price for the option is given by the Black-Scholes formula.</p><p>If <img src="9-1240148\1568c460-611e-426f-8bc7-15d41999d9c6.jpg" /> follows a Student’s t-distribution, then <img src="9-1240148\c936f957-0300-4a10-abd2-cad0cd03d47b.jpg" /> is infinite. The exponential growth of <img src="9-1240148\fed9eb3f-b366-4eab-b6c8-68822b529840.jpg" /> with <img src="9-1240148\5fd2daf7-e343-4e7e-91bc-5a40aa79c82a.jpg" /> dominates the <img src="9-1240148\16ab88b1-90ab-4b7a-b1c9-c8d35ae68d71.jpg" /> tails of the Student’s distribution, Equation (2). However, if an effectively truncated Student’s t-distribution is used, then the tails of the effectively truncated t-distribution diminish with <img src="9-1240148\b19e0305-983b-4fea-9ab5-611406e48326.jpg" /> as<img src="9-1240148\01b4e696-d894-46aa-8277-8cf206a02337.jpg" />, and the value of the European call option remains finite. Both the effectively truncated Student’s t-distribution and the normal distribution have a multiplicative <img src="9-1240148\3e88b3a3-f246-4bb9-8632-a2e5966c15f7.jpg" /> factor that dominates the exponential growth of <img src="9-1240148\da96bb5a-9e25-4618-9d2d-609c2b6e9dda.jpg" /> for large<img src="9-1240148\15eca854-9c8b-4e11-acb1-4cf05204f07b.jpg" />. In general, the integral to price the European call option must be evaluated numerically. Equation (21) is perhaps the simplest manner in which to write the cost of the call option.</p><p>The Student’s t-distribution is found (over the subinterval of the infinite region of support where returns are observed) to fit the distribution of the logarithms of daily returns better than a normal distribution or indeed better than most any other distribution [4-9]. It would be prudent to price options using a distribution that matches the data. The effectively truncated t-distribution that is described in this paper is a distribution that matches the observed data, as demonstrated in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p>Adaptive bins widths were used to generate the frequency of occurrence data for <xref ref-type="fig" rid="fig3">Figure 3</xref>. The bin width was increased until at least 5 counts were obtained in the bin. The normal distribution fits the data well only in the neighbourhood of <img src="9-1240148\8779f48f-fd85-4059-a838-4e4a47ec669e.jpg" /> and does not fit the fat tails of the data. The quality of the fit of a Student’s t-distribution to the 15 491 data points that constitute the frequency of occurrence of ranges of values for the logarithms of the daily returns is remarkably good over all the returns, including the infrequent, low-probability events in the tails.</p><p>A fit of a Student’s t-distribution to the logarithm of the daily returns over the period of January 1950 to 27 July 2011 for the S&amp;P 500 Index gives <img src="9-1240148\5b80d9d6-744e-4c6e-9bd6-f54af54e2d56.jpg" /> and a scale parameter<img src="9-1240148\a111ebb5-b150-4ba0-9741-2cc9d7fcb212.jpg" />. The data show a kurtosis of 25 and a maximum 22-day volatility of<img src="9-1240148\67bcecd2-0bd4-4496-b9ff-e58295e6320b.jpg" />. The approximation for the kurtosis for a <img src="9-1240148\4f17a9d2-1b80-48a9-9e92-0b0abceed8a8.jpg" /> effectively truncated t-distribution equal to 25, <img src="9-1240148\fb6ebe9e-b818-4adf-b3f7-de1f2feae153.jpg" />, is solved for<img src="9-1240148\1e803860-4902-4960-8261-d58df7efdeb0.jpg" />. The chi distribution in the mixing integral is, assuming that<img src="9-1240148\7a88d7c1-4f05-405f-af9e-2bf9453aa9b6.jpg" />, truncated for volatilities <img src="9-1240148\9a44d0ec-415a-4c83-8774-173da722f90c.jpg" /> to obtain the same kurtosis as the data. This level of truncation is roughly twice the maximum 22-day volatility of <img src="9-1240148\2bf4b8e7-f04b-4fda-8e9c-a0a5772e18d0.jpg" /> that was obtained from the daily returns. Note that the kurtosis exists only for <img src="9-1240148\7c087e0a-46bf-45ab-bda2-63b45175f79a.jpg" /> for Student’s tdistributions. In contrast, the kurtosis is defined for <img src="9-1240148\9ddac4de-e485-403f-ab71-dafc3f8f32b7.jpg" /> for an effectively truncated t-distribution, in agreement with the data.</p><p>The area in the left wing for truncation of the chi distribution at <img src="9-1240148\ba770ef5-059b-4a0a-9969-f8e150171645.jpg" /> to match the kurtosis of the observed daily returns of 25 is<img src="9-1240148\18e78c77-4eff-480a-84c0-76bb0ea97bca.jpg" />. This level of truncation of the chi distribution has a minor effect on the effectively truncated Student’s t-distribution for<img src="9-1240148\6d116877-1997-472e-a11e-eb2734bb7f36.jpg" />, as can be observed in <xref ref-type="fig" rid="fig4">Figure 4</xref>. This is consistent with the data; all 15 491 data points lie in the interval −0.205 to +0.116. When the scale parameter <img src="9-1240148\3aba9048-4125-4998-a5e6-b150063199a8.jpg" /> is taken into account, the data lie in the region <img src="9-1240148\c89242d1-9fc8-4398-9769-3957b8fe0979.jpg" /> The truncation to match the kurtosis is not severe (c.f. <xref ref-type="fig" rid="fig4">Figure 4</xref>), but the truncation is sufficient to keep finite the integrals required to price options with a log Student’s t-distribution.</p></sec><sec id="s4"><title>4. Conclusions</title><p>A Student’s t-distribution arises from an averaging over the standard deviation of a normal distribution when the reciprocal of the standard deviation is distributed as chi. The Student’s t-distribution offers support over <img src="9-1240148\1d7c2c94-0274-4699-81fe-4aa484ca82a6.jpg" /> to<img src="9-1240148\da27a16d-e110-42ba-a735-0b4fb5614cce.jpg" />. The slowly decaying power tails and infinite support region mean some moments for the Student’s t-distribution do not exist. This divergence of integrals</p><p>can cause problems, particularly in the pricing of options where the logarithm of returns is distributed as a Student’s t-distribution. One approach to deal with the divergence is to truncate the Student’s t-distribution [<xref ref-type="bibr" rid="scirp.25549-ref9">9</xref>]. Data typically fit well to the central region of the t-distribution and are nonexistent far from the central region of the Student’s t-distribution. Other approaches are to multiply the t-distribution by an envelope function that reduces the impact of the tails [<xref ref-type="bibr" rid="scirp.25549-ref8">8</xref>] or to use a generalized form that includes an envelope function that reduces the impact of the tails [<xref ref-type="bibr" rid="scirp.25549-ref12">12</xref>]. The approach presented here is to left-truncate a chi distribution for the reciprocal of the standard deviation. The chi distribution is used in a mixing integral with a normal distribution to yield an effectively truncated Student’s t-distribution. Left truncation of the chi distribution at q yields tails for the effectively truncated Student’s t-distribution that decay with increasing t as<img src="9-1240148\f70b72f6-c20f-4af8-9a5c-dd9c933b86fe.jpg" />. The approach adopted here supports the envelope multiplication of Moriconi [<xref ref-type="bibr" rid="scirp.25549-ref8">8</xref>] by showing that the envelope modification is similar in effect to a left truncation of a chi distribution for the reciprocal of the standard deviation, and then mixing the truncated chi distribution with a normal distribution of the same standard deviation.</p><p>Expressions or power series expressions for the pdf, variance, and kurtosis for several low number of degrees of freedom, effectively truncated Student’s t-distributions are given. These expressions demonstrate the exponential tails of the effectively truncated t-distribution and show that the variance and kurtosis remain remain finite for the effectively truncated distributions. In addition, it is shown that it is the large values of the standard deviation in the mixing integral that give rise to the fat tails of the Student’s t-distribution. The small values of the standard deviation in the mixing integral do not contribute to the tails of the Student’s t-distribution and only weakly contribute to the core of the Student’s t-distribution.</p><p>The effective truncation of the Student’s t-distribution means that integrals required to price financial instruments such as European call options remain finite. This permits pricing with a distribution, the log Student’s t-distribution, that describes well returns for stocks.</p><p>Simple expressions were not found for the effectively truncated t-distributions with even numbers of degrees of freedom. Given the importance of the Student’s t-distribution in the description of returns and data in general, it would be helpful to find accurate approximations that smoothly approach the expressions for the odd numbers of degrees of freedom. These approximations could then be used to model data where it is unphysical to assume support over <img src="9-1240148\400dcf3b-bffd-42a9-83fc-28032d226b5a.jpg" /> to<img src="9-1240148\6d0a148b-64f2-4750-9025-d48c56cd8e1b.jpg" />. The <img src="9-1240148\30e373bc-2bd2-4492-85fd-72e8220f45ba.jpg" /> envelope modification of Moriconi [<xref ref-type="bibr" rid="scirp.25549-ref8">8</xref>] might be a sufficiently good approximation for all degrees of freedom. It is shown that the envelope modification of Moriconi is functionally equivalent to a truncation of large values of the volatility (standard deviation) in the chi distribution of the chi-normal mixing integral that leads to a Student’s t-distribution.</p></sec><sec id="s5"><title>5. Acknowledgements</title><p>This work was funded by the Natural Science and Engineering Research Council (NSERC) Canada.</p></sec><sec id="s6"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.25549-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Student, “The Probable Error of a Mean,” Biometrika, Vol. 6, No. 1, 1908, pp. 1-25.</mixed-citation></ref><ref id="scirp.25549-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">S. L. Zabell, “On Student’s 1908 Article ‘The Probable Error of a Mean’,” Journal of the American Statistical Association, Vol. 103, No. 481, 2008, pp. 1-7. 
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