<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2015.64066</article-id><article-id pub-id-type="publisher-id">AM-56015</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>
 
 
  High Moments Jarque-Bera Tests for Arbitrary Distribution Functions
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ane</surname><given-names>Samb Lo</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Oumar</surname><given-names>Thiam</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mohamed</surname><given-names>Cheikh Haidara</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Laboratoire de Statistique Théorique et Appliquée (LSTA), Université Pierre et Marie Curie, Paris, France</addr-line></aff><aff id="aff2"><addr-line>LERSTAD, Université Gaston Berger de Saint-Louis, Saint-Louis, Senegal</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>gane-samb.lo@ugb.edu.sn(ASL)</email>;<email>ganesamblo@ganesamblo.net(OT)</email>;<email>othiam@univi.net(MCH)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>10</day><month>04</month><year>2015</year></pub-date><volume>06</volume><issue>04</issue><fpage>707</fpage><lpage>716</lpage><history><date date-type="received"><day>5</day>	<month>February</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>27</month>	<year>April</year>	</date><date date-type="accepted"><day>28</day>	<month>April</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>
 
 
  The Jarque-Bera’s fitting test for normality is a celebrated and powerful one. In this paper, we consider general Jarque-Bera tests for any distribution function (
  <em>df</em>) having at least 4
  <em>k</em> finite moments for 
  <em>k</em> ≥ 2. The tests use as many moments as possible whereas the JB classical test is supposed to test only skewness and kurtosis for normal variates. But our results unveil the relations between the coeffients in the JB classical test and the moments, showing that it really depends on the first eight moments. This is a new explanation for the powerfulness of such tests. General Chi-square tests for an arbitrary model, not only normal, are also derived. We make use of the modern functional empirical processes approach that makes it easier to handle statistics based on the high moments and allows the generalization of the JB test both in the number of involved moments and in the underlying distribution. Simulation studies are provided and comparison cases with the Kolmogorov-Smirnov’s tests and the classical JB test are given.
 
</p></abstract><kwd-group><kwd>Asymptotic Distribution</kwd><kwd> Asymptotic Statistical Tests</kwd><kwd> Normality Tests</kwd><kwd> Functional Empirical Processes</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In this paper, we are concerned with generalizations of Jarque-Bera’s (JB) [<xref ref-type="bibr" rid="scirp.56015-ref1">1</xref>] tests based on arbitrary first (4k) moments, k ≥ 2, rather than on the first eight ones as usual. (See [<xref ref-type="bibr" rid="scirp.56015-ref2">2</xref>] for a reminder of JB tests, page 69). We obtain general statistics that allow statistical tests for any distribution function G provided it has enough moments. For a reminder, the classical JB test belongs to the class of omnibus moment tests, i.e. those which assess simultaneously whether the skewness and kurtosis of the data are consistent with a Gaussian model. This test proves optimum asymptotic power and good finite sample properties (see [<xref ref-type="bibr" rid="scirp.56015-ref1">1</xref>] ). A detailed description of that test and related indepth analyses can be found in Bowman and Shenton, D’Agosto, D’Agostino et al., etc. (see [<xref ref-type="bibr" rid="scirp.56015-ref3">3</xref>] -[<xref ref-type="bibr" rid="scirp.56015-ref5">5</xref>] and [<xref ref-type="bibr" rid="scirp.56015-ref6">6</xref>] ).</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x5.png" xlink:type="simple"/></inline-formula> be a sequence of independent and identically distributed random variables (r.v.’s) defined on the same probability space<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x6.png" xlink:type="simple"/></inline-formula>. For each<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x7.png" xlink:type="simple"/></inline-formula>, the skewness and kurtosis coefficients related to the sample <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x8.png" xlink:type="simple"/></inline-formula> are defined by.</p><disp-formula id="scirp.56015-formula875"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x9.png"  xlink:type="simple"/></disp-formula><p>These statistics are designed to estimate the theoretical skewness and kurtosis given by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x10.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x11.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x12.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x13.png" xlink:type="simple"/></inline-formula> respectively denote the mean and the variance of X that is supposed to be nondegenerated. Here and in all the sequel, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x14.png" xlink:type="simple"/></inline-formula>stands for the mathematical expectation with respect to the probability<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x15.png" xlink:type="simple"/></inline-formula>. Now, under the hypothesis:</p><p>H0: X follows a Gaussian normal law, we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x16.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x17.png" xlink:type="simple"/></inline-formula> and the JB statistic</p><disp-formula id="scirp.56015-formula876"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x18.png"  xlink:type="simple"/></disp-formula><p>has an asymptotic chi-square distribution with two degrees of freedom under the null hypothesis of normality. Jarque-Bera’s test consists in rejecting H0 when T<sub>n</sub> is far from zero. We will find below that the constants 6 and 24 used in (2), actually, are closely related to the first four even moments of a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x19.png" xlink:type="simple"/></inline-formula> random variable which are 1, 3, 15 and 105 and a more convenient form of (2) is</p><disp-formula id="scirp.56015-formula877"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x20.png"  xlink:type="simple"/></disp-formula><p>Our objective here is to generalize JB’s test to a general df G by considering high moments<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x21.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x22.png" xlink:type="simple"/></inline-formula>, with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x23.png" xlink:type="simple"/></inline-formula>, instead of the first eight moments only. We base our methods on the remark that for a random variable<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x24.png" xlink:type="simple"/></inline-formula>, one has</p><disp-formula id="scirp.56015-formula878"><label>. (H1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x25.png"  xlink:type="simple"/></disp-formula><p>Actually, JB’s test only checks the third and fourth moments of X while the coefficients of the JB statistic (2) uses the first eight moments of X. Our guess is that we would have better tests if we are able to simultaneously check all the first (2k) moments for some k ≥ 2. To this purpose, we consider the following statistics, that is the normalized centered empirical moments (NCEM),</p><disp-formula id="scirp.56015-formula879"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x26.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.56015-formula880"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x27.png"  xlink:type="simple"/></disp-formula><p>are the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x28.png" xlink:type="simple"/></inline-formula> non-centered and the centered empirical moments. By the classical law of large numbers, the statistics in (3) are, for each fixed p, asymptotic estimators of</p><disp-formula id="scirp.56015-formula881"><label>, (4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x29.png"  xlink:type="simple"/></disp-formula><p>whenever the (4p)<sup>th</sup> moment exists. Finally we consider C<sup>1</sup>-class functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x30.png" xlink:type="simple"/></inline-formula> et <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x31.png" xlink:type="simple"/></inline-formula> and denote <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x32.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x33.png" xlink:type="simple"/></inline-formula>.</p><p>Our general test is based on the following statistics, for k ≥ 2,</p><disp-formula id="scirp.56015-formula882"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x34.png"  xlink:type="simple"/></disp-formula><p>which almost-surely <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x35.png" xlink:type="simple"/></inline-formula> tends to</p><disp-formula id="scirp.56015-formula883"><label>, (6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x36.png"  xlink:type="simple"/></disp-formula><p>as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x37.png" xlink:type="simple"/></inline-formula>. For an independent and identically distributed sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x38.png" xlink:type="simple"/></inline-formula> of r.v.’s associated with a distribution function G having a finite 2k-moment, we will have by Theorem 1 below that</p><disp-formula id="scirp.56015-formula884"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x39.png"  xlink:type="simple"/></disp-formula><p>From such a general result, we are able to derive a normality test by using it with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x40.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x41.png" xlink:type="simple"/></inline-formula>for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x42.png" xlink:type="simple"/></inline-formula>, and rejects normality for a large value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x43.png" xlink:type="simple"/></inline-formula>.</p><p>We are going to establish a general asymptotic normality of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x44.png" xlink:type="simple"/></inline-formula> for any df’s G with 4k finite moments. These results provide themselves efficient tests for an arbitrary d.f. Next, we will derive chi-square tests that generalize JB’s test for higher moments and for arbitrary df’s too.</p><p>Our results will show that these tests based on the 2k moments, need, in fact, the eight 4k moments for computing the variance. This unveils that the classical JB’s test is not based only on the kurtosis and the skewness but also on the sixth and the eighth moments. To describe the complete form of the Jarque-Bera method, put</p><disp-formula id="scirp.56015-formula885"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x45.png"  xlink:type="simple"/></disp-formula><p>The JB’s test for a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x46.png" xlink:type="simple"/></inline-formula> r.v. will be showed to derive from the following general law</p><disp-formula id="scirp.56015-formula886"><label>. (7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x47.png"  xlink:type="simple"/></disp-formula><p>with the particular coefficients<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x48.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x49.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x50.png" xlink:type="simple"/></inline-formula>. This may be a new explanation of the powerfulness of the JB classical tests since a successful test of normality means that the sample is from a df having same first eight moments as the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x51.png" xlink:type="simple"/></inline-formula> r.v., and this is very highly improbable for a non normal r.v..</p><p>As an illustration of what proceeds, consider a distribution following a double-gamma distribution</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x52.png" xlink:type="simple"/></inline-formula>of density probability <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x53.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x54.png" xlink:type="simple"/></inline-formula>. This rv is</p><p>centered and has a kurtosis coefficient equal to 3. It is rejected from normality by the JB test. If only the skewned and kurtosis do matter, it would not be the case. Actually, the rejection comes from the parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x55.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x56.png" xlink:type="simple"/></inline-formula> that are very different from a standard normal distribution to this specific distribution.</p><p>The rest of the paper is organized as follows. In Subsection 2.1 of Section 2, we begin to give a concise of reminder the modern theory of functional empirical processes that is the main theoretical tool we use for finding the asymptotic law of (5). Next in Subsection 2.2, we establish general results of the consistency of (5) and its asymptotic law, consider particular cases in Subsection 2.3, propose chi-square universal tests in Subsection 2.4 and finally state the proofs in Subsection 2.5. We end the paper by Section 3 where simulation results concerning the normal and double-exponential models are given.</p><p>We here express that in all the sequel the limits are meant as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x57.png" xlink:type="simple"/></inline-formula> and this will not be written again unless it is necessary.</p></sec><sec id="s2"><title>2. Results and Proofs</title><sec id="s2_1"><title>2.1. A Reminder of Functional Empirical Process</title><p>Since the empirical functional process is our key tool here, we are going to make a brief reminder on this process associated with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x58.png" xlink:type="simple"/></inline-formula>, and defined for each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x59.png" xlink:type="simple"/></inline-formula> by</p><disp-formula id="scirp.56015-formula887"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x60.png"  xlink:type="simple"/></disp-formula><p>where f is a real measurable function defined on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x61.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.56015-formula888"><label>, (8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x62.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.56015-formula889"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x63.png"  xlink:type="simple"/></disp-formula><p>It is known (see van der Vaart [<xref ref-type="bibr" rid="scirp.56015-ref7">7</xref>] , pages 81-93) that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x64.png" xlink:type="simple"/></inline-formula> converges to a functional Gaussian process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x65.png" xlink:type="simple"/></inline-formula> with covariance function</p><disp-formula id="scirp.56015-formula890"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x66.png"  xlink:type="simple"/></disp-formula><p>at least in finite distributions. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x67.png" xlink:type="simple"/></inline-formula>is linear, that is, for f and g satisfying (9) and for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x68.png" xlink:type="simple"/></inline-formula>, we have</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x69.png" xlink:type="simple"/></inline-formula>.</p><p>This linearity will be useful for our proofs. We are now in position to state our main results.</p></sec><sec id="s2_2"><title>2.2. Statements of Results</title><p>First introduce this notation for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x70.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x71.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x72.png" xlink:type="simple"/></inline-formula>. Let f<sub>i</sub> and g<sub>i</sub>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x73.png" xlink:type="simple"/></inline-formula>be C<sup>1</sup>-functions with values in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x74.png" xlink:type="simple"/></inline-formula>. Put <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x75.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x76.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x77.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x78.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.56015-formula891"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x79.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56015-formula892"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x80.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.56015-formula893"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x81.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.56015-formula894"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x82.png"  xlink:type="simple"/></disp-formula><p>Here are our main results.</p><p>Theorem 1 Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x83.png" xlink:type="simple"/></inline-formula>, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x84.png" xlink:type="simple"/></inline-formula>. Then</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x85.png" xlink:type="simple"/></inline-formula>,</p><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x86.png" xlink:type="simple"/></inline-formula>.</p><p>Corollary 1 (Normality test). Let X be a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x87.png" xlink:type="simple"/></inline-formula> r.v. and let, for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x88.png" xlink:type="simple"/></inline-formula></p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x89.png" xlink:type="simple"/></inline-formula>,</p><p>Then</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x90.png" xlink:type="simple"/></inline-formula>,</p><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x91.png" xlink:type="simple"/></inline-formula>,</p><p>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x92.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s2_3"><title>2.3. Particular Cases and Consequences</title><sec id="s2_3_1"><title>2.3.1. A General Test</title><p>Let G be an arbitrary df with a 4k<sup>th</sup> finite moment for k ≥ 2, this is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x93.png" xlink:type="simple"/></inline-formula>. We want to check whether a sample <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x94.png" xlink:type="simple"/></inline-formula> is from G. We then select C<sup>1</sup>-functions f<sub>i</sub> and g<sub>i</sub>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x95.png" xlink:type="simple"/></inline-formula>and compute the observed</p><p>value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x96.png" xlink:type="simple"/></inline-formula> of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x97.png" xlink:type="simple"/></inline-formula> and report the p-value of the test, that is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x98.png" xlink:type="simple"/></inline-formula>where s<sup>2</sup> is either the exact variance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x99.png" xlink:type="simple"/></inline-formula> or its plug-in estimator</p><disp-formula id="scirp.56015-formula895"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x100.png"  xlink:type="simple"/></disp-formula><p>Our guess is that using a greater value of k makes the test more powerful since the equality in distribution of univariate r.v.’s means equality of all moments when they exist (see page 213 in [<xref ref-type="bibr" rid="scirp.56015-ref8">8</xref>] ). For k = 2, this result depends on the first eight moments. Then to find another df G<sub>1</sub> for which the p-value exceeds 5% would suggest it has the same eight moments as G, which is highly improbable. Simulation studies in Section 0 support our findings. Remark that we have as many choices as possible for the functions the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x101.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x102.png" xlink:type="simple"/></inline-formula>.</p><p>Unfortunately, in the simulation studies reported below, we noticed that the plug-in estimator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x103.png" xlink:type="simple"/></inline-formula> may hugely over estimate the exact variance and leads to accepting any data to follow that model, or significantly underestimate it and leads to reject data from the model itself. This is why we only use the exact variance here.</p><p>Now let us show how to derive chi-square tests from Theorem 1.</p></sec><sec id="s2_3_2"><title>2.3.2. Generalized JB Test and Tests for Symmetrical df’s</title><p>Suppose that X is a symmetrical distribution. We have from Theorem 1 that</p><disp-formula id="scirp.56015-formula896"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x104.png"  xlink:type="simple"/></disp-formula><p>Since X is symmetrical, that is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x105.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x106.png" xlink:type="simple"/></inline-formula>, we may without loss of generality suppose that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x107.png" xlink:type="simple"/></inline-formula> since replacing X by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x108.png" xlink:type="simple"/></inline-formula> does affect neither the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x109.png" xlink:type="simple"/></inline-formula> nor the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x110.png" xlink:type="simple"/></inline-formula>. Then we have from (11) and (12) that</p><disp-formula id="scirp.56015-formula897"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x111.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.56015-formula898"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x112.png"  xlink:type="simple"/></disp-formula><p>By reminding that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x113.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x114.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x115.png" xlink:type="simple"/></inline-formula>, we observe that the product <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x116.png" xlink:type="simple"/></inline-formula> only includes functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x117.png" xlink:type="simple"/></inline-formula> with odd <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x118.png" xlink:type="simple"/></inline-formula> and then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x119.png" xlink:type="simple"/></inline-formula>. Thus</p><disp-formula id="scirp.56015-formula899"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x120.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x121.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x122.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x123.png" xlink:type="simple"/></inline-formula>. We get</p><p>Corollary 2 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x124.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x125.png" xlink:type="simple"/></inline-formula> and G be a symmetrical df. We have</p><disp-formula id="scirp.56015-formula900"><label>. (16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x126.png"  xlink:type="simple"/></disp-formula><p>For a standard normal random variable, we get <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x127.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x128.png" xlink:type="simple"/></inline-formula> and the normality JB’s test becomes a particular case of (16), which is a general chi-square test for an arbitrary df with 2p-finite moments.</p><p>Corollary 3 Let G be a Gaussian df. Then</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x129.png" xlink:type="simple"/></inline-formula>.</p><p>We see that we obtain an infinite number of tests for the normality. For example, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x130.png" xlink:type="simple"/></inline-formula>, we have,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x131.png" xlink:type="simple"/></inline-formula>, etc.</p></sec></sec><sec id="s2_4"><title>2.4. A General Chi-Square Test</title><p>Consider (15) and put <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x132.png" xlink:type="simple"/></inline-formula> and suppose that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x133.png" xlink:type="simple"/></inline-formula>. We have</p><p>Corollary 4 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x134.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x135.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x136.png" xlink:type="simple"/></inline-formula>. Then</p><disp-formula id="scirp.56015-formula901"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x137.png"  xlink:type="simple"/></disp-formula><p>converges in law to a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x138.png" xlink:type="simple"/></inline-formula> r.v..</p><p>It is now time to prove Theorem 1 before considering the simulation studies.</p></sec><sec id="s2_5"><title>2.5. Proofs</title><p>Since G has at least first 4k moments finite, we are entitled to use the finite-distribution convergence of the empirical function process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x139.png" xlink:type="simple"/></inline-formula> as below. Let us begin to give the asymptotic law of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x140.png" xlink:type="simple"/></inline-formula>. By denoting<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x141.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.56015-formula902"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x142.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x143.png" xlink:type="simple"/></inline-formula> is defined in (11) and where we used that the linearity of the empirical functional process. By observing that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x144.png" xlink:type="simple"/></inline-formula>, we finally obtain</p><disp-formula id="scirp.56015-formula903"><label>. (17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7402640x145.png"  xlink:type="simple"/></disp-formula><p>Now the law of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x146.png" xlink:type="simple"/></inline-formula> is given by</p><disp-formula id="scirp.56015-formula904"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x147.png"  xlink:type="simple"/></disp-formula><p>By the delta-method, we have</p><disp-formula id="scirp.56015-formula905"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x148.png"  xlink:type="simple"/></disp-formula><p>and then</p><disp-formula id="scirp.56015-formula906"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x149.png"  xlink:type="simple"/></disp-formula><p>and next, by noticing from 17 that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x150.png" xlink:type="simple"/></inline-formula> for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x151.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x152.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x153.png" xlink:type="simple"/></inline-formula>,</p><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x154.png" xlink:type="simple"/></inline-formula> is given in (12). By the very same methods, we have</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x155.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x156.png" xlink:type="simple"/></inline-formula>is stated in (13). The delta-method also yields</p><disp-formula id="scirp.56015-formula907"><graphic  xlink:href="http://html.scirp.org/file/9-7402640x157.png"  xlink:type="simple"/></disp-formula><p>This completes the proof of the theorem. The proof of the corollary is a simple consequence of the theorem.</p></sec></sec><sec id="s3"><title>3. Simulation and Applications</title><sec id="s3_1"><title>3.1. Scope the Study</title><p>We want to focus on illustrating how performs the general test for usual laws such as Normal and Double Gamma ones. It is clear that the generality of our results that are applicable to arbitrary d.f.’s with some finite k<sup>th</sup>-moment <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x158.png" xlink:type="simple"/></inline-formula> deserves extended simulation studies for different classes of df’s. We particularly have to pay attention to the choice of k and of the functions fi and gi, depending on the specific model we want to test.</p><p>In this paper, we want to set a general and workable method to simulate and test two symmetrical models. The normal and the double-exponential one with density<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x159.png" xlink:type="simple"/></inline-formula>. We expect to find a test that accepts normality for normal data and rejects double-exponential data and to confirm this by the Jarque-Berra test, and to have another test that exactly does the contrary.</p><p>Once these results are achieved, we would be in position to handle a larger scale simulation research following the outlined method. Specially, fitting financial data to the generalized hyperbolic model is one the most interesting applications of our results.</p></sec><sec id="s3_2"><title>3.2. The Frame</title><p>We first choose all the functions f<sub>i</sub> equal to f<sub>0</sub> and all the functions g<sub>i</sub> equal to g<sub>0</sub>. We fix k = 3, that is we work with the first twelve moments. As a general method, we consider two df’s G<sub>1</sub> and G<sub>2</sub>. We fix one of them say G<sub>1</sub> and compute <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x160.png" xlink:type="simple"/></inline-formula> and the variance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x161.png" xlink:type="simple"/></inline-formula> from the exact distribution function G<sub>1</sub>. We generate samples of size n from one the df’s (either G<sub>1</sub> or G<sub>2</sub>) and compute<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x162.png" xlink:type="simple"/></inline-formula>. We repeat this B times</p><p>and report the mean value t<sup>*</sup> of the replicated values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x163.png" xlink:type="simple"/></inline-formula> and report the</p><p>p-value<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x164.png" xlink:type="simple"/></inline-formula>. The simulation outcomes will be considered as conclusive if p is high for samples from G<sub>1</sub> and low for samples from G<sub>2</sub>. The results are compared with those given by the Kolmogorov- Smirnov test (KST) and when the data are Gaussian, they are compared with the outcomes from JB’s classical test.</p></sec><sec id="s3_3"><title>3.3. The Results</title><p>We consider the following cases: G<sub>1</sub> is a Gaussian r.v<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x165.png" xlink:type="simple"/></inline-formula>; G<sub>2</sub> is double-exponential law <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x166.png" xlink:type="simple"/></inline-formula> with density probability <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x167.png" xlink:type="simple"/></inline-formula> and G<sub>3</sub> is a double-gamma law <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x168.png" xlink:type="simple"/></inline-formula> with probability den-</p><p>sity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x169.png" xlink:type="simple"/></inline-formula>.</p>Normal Model <img data-original="http://html.scirp.org/file/9-7402640x170.png" /><p>The choice <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x171.png" xlink:type="simple"/></inline-formula> is natural since the Jarque-Berra test may be derived for our result for these functions and for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x172.png" xlink:type="simple"/></inline-formula>. The model is determined by these following parameters:</p><p>We recall that the variance of our statistic depends on the first 4k moments.</p><p>Simulation study.</p><p>Testing the model with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x177.png" xlink:type="simple"/></inline-formula> data gives the following outcomes for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x178.png" xlink:type="simple"/></inline-formula></p><p>and for n = 100,</p><p>and for n = 1000,</p><p>where JB is the classical Jarque-Berra statistic, pJB is the p-value of the JB test, KS is the Kolmogorov-smirnov statistic and pKS is the related p-value. Our model accepts the normality and this is confirmed by JB’s test and by the Klmogorov-Smirnov test (KST). The simulation results are very stable and constantly suggest acceptance.</p><p>Testing the double-exponential versus the normal model.</p><p>Recall that the values <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x188.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x189.png" xlink:type="simple"/></inline-formula> are<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x190.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x191.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x192.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x193.png" xlink:type="simple"/></inline-formula>. Comparing these values with those of a normal model, it is natural to think that the test will fail since only the b<sub>p</sub> coincide and the test is only based on the moments. Indeed, using data from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x193.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x194.png" xlink:type="simple"/></inline-formula> gives for n = 11</p><p>and for n = 22</p><p>Our test rejects the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x201.png" xlink:type="simple"/></inline-formula> model for n = 11 and JB’s test rejects it only for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x202.png" xlink:type="simple"/></inline-formula>. We see here the advantage brought by the value k = 3 in our statistic. The KST has problems in rejecting the false <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x203.png" xlink:type="simple"/></inline-formula> even for n = 1000 that of Jarque-Berra.</p><p>Testing the double-gamma versus the normal model.</p><p>Let use <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x204.png" xlink:type="simple"/></inline-formula> data with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x205.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x206.png" xlink:type="simple"/></inline-formula>. We have the outcomes for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x207.png" xlink:type="simple"/></inline-formula></p><p>and for n = 22</p><p>We have similar results. Ou test rejects the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x214.png" xlink:type="simple"/></inline-formula> model for n = 12 and JB’s test rejects it only for n ≥ 18. We see here the advantage brought by the value k = 3 in our statistic. Although the first four moments of a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x215.png" xlink:type="simple"/></inline-formula> are 0, 1, 0 and 3, that is, the same of those of standard normal rv, this model is rejected. We already pointed out that the coefficients 4 and 6 are in fact based on the first eight moments and the discrepancy of moments higher than 4 results in the rejection.</p><p>Analysing the tables above, we conclude that our test performs better the JB’s test against a double-gamma df with same skewness and kurtosis than a normal df for small sample sizes around ten and this is real advantage for small data sizes. Even for k = 2, our test is performant for the small values n = 11 and n = 12.</p><p>Double-exponential model<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x216.png" xlink:type="simple"/></inline-formula>.</p><p>We point out that the statistic <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x217.png" xlink:type="simple"/></inline-formula> does not depend on the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x217.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x218.png" xlink:type="simple"/></inline-formula>. Then we only consider <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x217.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x218.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x219.png" xlink:type="simple"/></inline-formula> in the following. We always use<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x217.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x218.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x219.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x220.png" xlink:type="simple"/></inline-formula>. The model is determined by the following values.</p><p>Here, we do not have the Jarque-Berra test to confirm the results.</p><p>Simulation. Testing the model with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x226.png" xlink:type="simple"/></inline-formula> data gives the following outcomes, for n = 800.</p><p>The simulation results are very stable and constantly suggest acceptance.</p><p>Testing normal data. Using normal data gives</p><p>The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x233.png" xlink:type="simple"/></inline-formula> model is rejected. We noticed that the rejection of normal data is automatically obtained for large sizes here, when n is greater than 900. For n between 500 and 900, rejection is frequent but acceptance occurs now and then. Whe also noticed that the variance of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x234.png" xlink:type="simple"/></inline-formula> are high and do not allow to reject normal data for small sizes. This leads us to consider other functions. Now consider the classes of functions</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x235.png" xlink:type="simple"/></inline-formula>.</p><p>We obtain good results for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x236.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x236.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x237.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x236.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x238.png" xlink:type="simple"/></inline-formula>. In this case, the exact value of the statistic is 11.600. The double-exponential <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x236.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x238.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x239.png" xlink:type="simple"/></inline-formula> model is confirmed according to the following table</p><p>while the normal model is rejected as illustrated below:</p><p>It is important to mention here that the KST is very powerful is rejecting the normal model with double-ex- ponential and double-gamma data with extremely low p-value’s.</p></sec><sec id="s3_4"><title>3.4. Conclusion and Perspectives</title><p>We propose a general test for an arbitrary model. The methods are based on functional empirical processes theory that readily provides asymptotic laws from which statistical tests are derived. They depend on an integer k such that the pertaining df has 4k first finite moments. We get two kinds of tests. A general one based on functions f<sub>i</sub> and g<sub>i</sub>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7402640x246.png" xlink:type="simple"/></inline-formula>, with an asymptotic normal law. We derive from these results chi-square tests that are valid for general df’s and that includes the Jarque-Berra test of normality. Both tests use arbitrary moments. We only undergo simulation studies for the first kind of test. Our simulation studies show high performance for nor- mality against other symmetrical laws such as double-exponential or double-gamma ones. For suitable choices of f<sub>i</sub>, g<sub>i</sub>, and k, the test performs well for small samples (n = 20) both for accepting the normal model and rejecting other models. We also show that for suitable choice of f<sub>i</sub> and g<sub>i</sub>, the test for the double-exponential model is also successful, but for sizes greater that n = 150. In upcoming papers, we will focus on detailed results on specific models and try to found out, for each case, suitable value of the parameters of the tests ensuring good performances for small data. A paper is also to be devoted to simulation studies for the khi-square tests and their applications to financial data.</p></sec></sec></body><back><ref-list><title>References</title><ref id="scirp.56015-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Jarque, C.M. and Bera, A.K. (1987) A Test for Normality of Observations and Regression Residuals. International Statistical Review, 55, 163-172.  
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