<?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.2019.94028</article-id><article-id pub-id-type="publisher-id">OJS-94146</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>
 
 
  Robust Continuous Quadratic Distance Estimation Using Quantiles for Fitting Continuous Distributions
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Andrew</surname><given-names>Luong</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>école d’actuariat, Université Laval, Ste Foy, Québec, Canada</addr-line></aff><pub-date pub-type="epub"><day>05</day><month>08</month><year>2019</year></pub-date><volume>09</volume><issue>04</issue><fpage>421</fpage><lpage>435</lpage><history><date date-type="received"><day>19,</day>	<month>June</month>	<year>2019</year></date><date date-type="rev-recd"><day>3,</day>	<month>August</month>	<year>2019</year>	</date><date date-type="accepted"><day>6,</day>	<month>August</month>	<year>2019</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>
 
 
  Quadratic distance estimation making use of the sample quantile function over a continuous range is introduced. It extends previous methods which are based only on a few sample quantiles and it parallels the continuous GMM method. Asymptotic properties are established for the continuous quadratic distance estimators (CQDE) and the implementation of the methods are discussed. The methods appear to be useful for balancing robustness and efficiency and useful for fitting distribution with model quantile function being simpler than its density function or distribution function.
 
</p></abstract><kwd-group><kwd>Covariance Kernel</kwd><kwd> Influence Function</kwd><kwd> Hilbert Space</kwd><kwd> Linear Operator</kwd><kwd> GMM Estimation</kwd><kwd> Spectral Decomposition</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>For estimation in a classical setup, we often assume to have n independent, identically distributed observations X 1 , ⋯ , X n from a continuous density f θ 0 ( x ) which belongs to a parametric family { f θ } , i.e., f θ 0 ( x ) ∈ { f θ } where θ = ( θ 1 , ⋯ , θ m ) ′ , θ ∈ Ω and θ 0 is the true vector of parameters, Ω is assumed to be compact. One of the main objectives of inferences is to be able to estimate θ 0 . In an actuarial context, the sample observations might represent losses of a certain type of contracts and an estimate of θ 0 is necessary if we want to make rates or premiums for the type of contract where we have observations.</p><p>Maximum likelihood (ML) estimation are density based and often the domain of the density function must not depend on the parameters is one of the regularity conditions so that ML estimators attain the lower bound as given by the information matrix. In many applications, this condition is not met. We can consider the following example which gives the Generalized Pareto distribution (GPD) and draw the attention on the properties of the model quantile function which appears to have nicer properties than the density function and hence motivate us to develop continuous quadratic distance (CQD) estimation using quantiles on a continuum range which generalizes the quadratic distance (QD) methods based on few quantiles as proposed by LaRiccia and Wehrly [<xref ref-type="bibr" rid="scirp.94146-ref1">1</xref>] which can be viewed as based on a discrete range and hence CQD estimation might overcome the arbitrary choice of quantiles of QD as CQD will essentially make use of all the quantiles over the range with 0 &lt; p &lt; 1 .</p><p>Example (GPD).</p><p>The GP family is a two parameters family with the vector of parameter θ = ( λ , κ ) ′ .</p><p>The density, distribution function and quantile function are given respectively by</p><p>f ( x ; λ , κ ) = 1 λ ( 1 − κ x λ ) 1 κ − 1 , 1 − κ x λ ≥ 0 , κ ≠ 0 , λ &gt; 0 and</p><p>f ( x ; λ ) = 1 λ e − x / λ , x ≥ 0 , κ = 0 , λ &gt; 0 ,</p><p>the distribution function is given by</p><p>F ( x ; λ , κ ) = 1 − ( 1 − κ x λ ) 1 κ , 1 − κ x λ ≥ 0 , κ ≠ 0 , λ &gt; 0 and</p><p>F ( x ; λ ) = 1 − e − x / λ , x ≥ 0 , κ = 0 , λ &gt; 0 ,</p><p>the quantile function is given by</p><p>F − 1 ( t ; λ , κ ) = λ ( 1 − ( 1 − t ) k ) / k , 0 &lt; t &lt; 1 , κ ≠ 0 , λ &gt; 0 and</p><p>F − 1 ( t ; λ ) = − λ log ( 1 − t ) , κ = 0 , λ &gt; 0 , 0 &lt; t &lt; 1</p><p>These functions can be found in Castillo et al. [<xref ref-type="bibr" rid="scirp.94146-ref2">2</xref>] (pages 65-66). Among these functions only the domain of the quantile function F − 1 ( t ; λ , κ ) does not depend on the parameters and naturally if the model quantile function satisfies some additional conditions such as differentiability, it is natural to develop statistical inference methods using the sample quantile function F n − 1 ( t ) instead of the sample distribution function F n ( x ) which are defined respectively as</p><p>F n − 1 ( t ) = inf { x | F n ( x ) ≥ t } and</p><p>F n ( x ) = 1 n ∑ i = 1 n δ x i with δ x i being the degenerate distribution at x i is the commonly used sample distribution. The counterpart of F n − 1 ( t ) is the model quantile function F θ − 1 ( t ) , see Serfling [<xref ref-type="bibr" rid="scirp.94146-ref3">3</xref>] (pages 74-80).</p><p>Due to the complexity of the density function for the GP model, alternative methods to ML have been developed in the literature for example with the probability weighted moments (PWM) method proposed by Hosking and Wallis [<xref ref-type="bibr" rid="scirp.94146-ref4">4</xref>] which leads to solve moment type of equations to obtain estimators by matching selected empirical moments with their model counterpart. The drawback of the PWM method is the range of the parameters must be restricted for the selected moments to exist, see Hosking and Wallis [<xref ref-type="bibr" rid="scirp.94146-ref4">4</xref>] , Kotz and Nadarajah [<xref ref-type="bibr" rid="scirp.94146-ref5">5</xref>] (p 36). The PWM method might not be robust and some robust methods have been proposed by Dupuis [<xref ref-type="bibr" rid="scirp.94146-ref6">6</xref>] , Juarez and Schucany [<xref ref-type="bibr" rid="scirp.94146-ref7">7</xref>] for estimation for the GP model.</p><p>For estimating parameters of the GPD, the percentiles matching (PM) method for fitting loss distributions as described by Klugman et al. [<xref ref-type="bibr" rid="scirp.94146-ref8">8</xref>] (pages 256-257) can also be used. It consists of first selecting two points t 1 , t 2 , with 0 &lt; t 1 &lt; t 2 &lt; 1 as we only have two parameters and solve the following moment type of estimating equations to obtain the estimators, i.e., θ ^ P M is the vector of solutions of</p><p>F n − 1 ( t 1 ) = F θ − 1 ( t 1 ) or equivalently, F θ ( F n − 1 ( t 1 ) ) = t 1</p><p>and</p><p><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x34.png" xlink:type="simple"/></inline-formula>or equivalently,<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x35.png" xlink:type="simple"/></inline-formula>.</p><p>The method is robust but not very efficient as only two points are used here to obtain moment type of equations and there is also arbitrariness on the choice of these two points. Castillo and Hadi [<xref ref-type="bibr" rid="scirp.94146-ref9">9</xref>] have improved this method by first selecting a set of two points, <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x36.png" xlink:type="simple"/></inline-formula>and obtain a set of corresponding PM estimators and finally define the final estimators according to a rule to select from the set of PM estimators generated by the set<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x37.png" xlink:type="simple"/></inline-formula>. The question on arbitrariness on selecting the set <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x38.png" xlink:type="simple"/></inline-formula> is still not resolved with this method.</p><p>Instead of solving moment type of equations, for parametric estimation in general not necessary for the GPD with the vector of parameters<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x39.png" xlink:type="simple"/></inline-formula>, LaRiccia and Wehrly [<xref ref-type="bibr" rid="scirp.94146-ref1">1</xref>] proposed to construct quadratic distance based on the discrepancy of <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x40.png" xlink:type="simple"/></inline-formula> using <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x41.png" xlink:type="simple"/></inline-formula> selected points<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x42.png" xlink:type="simple"/></inline-formula>’s with<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x43.png" xlink:type="simple"/></inline-formula>, so that we can define the following two vectors <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x44.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x45.png" xlink:type="simple"/></inline-formula> with</p><disp-formula id="scirp.94146-formula1"><graphic  xlink:href="//html.scirp.org/file/1-1241235x46.png"  xlink:type="simple"/></disp-formula><p>which is based on the sample and its model counterpart defined as</p><p><inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x47.png" xlink:type="simple"/></inline-formula>.</p><p>This leads to a class of quadratic distance of the form</p><disp-formula id="scirp.94146-formula2"><label>(1)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x48.png"  xlink:type="simple"/></disp-formula><p>and the quadratic distance (QD) estimators are found by minimizing the objective function given by expression (1), <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x49.png" xlink:type="simple"/></inline-formula>is a class of symmetric positive definite matrix which might depend on<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x50.png" xlink:type="simple"/></inline-formula>. Goodness-of-fit test statistics can also be constructed using expression (1), see Luong and Thompson [<xref ref-type="bibr" rid="scirp.94146-ref10">10</xref>] .</p><p>By quadratic distance estimation without further specializing it is continuous we mean that it is based on quadratic form as given by expression (1), it also fits into classical minimum distance (CMD) estimation and closely related to Generalized Methods of moment (GMM) and by GMM without further specializing that it is continuous GMM, we mean GMM based on a finite number of moment conditions, see Newey and McFadden [<xref ref-type="bibr" rid="scirp.94146-ref11">11</xref>] (p 212-2128).</p><p>Using the asymptotic theory of QD estimation or CMD estimation, it is well known that by letting <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x51.png" xlink:type="simple"/></inline-formula> to be the inverse of the asymptotic covariance matrix of <inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x52.png" xlink:type="simple"/></inline-formula> under<inline-formula><inline-graphic xlink:href="/html.scirp.org/file/1-1241235x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x53.png" xlink:type="simple"/></inline-formula>, we can obtain estimators which are the most efficient within the class being considered as given by expression (1), so we can let</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x54.png" xlink:type="simple"/></inline-formula>and</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x55.png" xlink:type="simple"/></inline-formula>is the asymptotic covariance matrix of<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x56.png" xlink:type="simple"/></inline-formula>.</p><p>In fact, it has been shown that it suffices to use a consistent estimate for <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x57.png" xlink:type="simple"/></inline-formula> to obtain asymptotic equivalent estimators. For example, first we obtain a preliminary consistent estimate <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x58.png" xlink:type="simple"/></inline-formula> and if we can construct a consistent estimate</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x59.png" xlink:type="simple"/></inline-formula>for<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x60.png" xlink:type="simple"/></inline-formula>, i.e., <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x61.png" xlink:type="simple"/></inline-formula></p><p>then we can construct a consistent estimate which is given <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x62.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x63.png" xlink:type="simple"/></inline-formula> as in general,</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x64.png" xlink:type="simple"/></inline-formula>.</p><p>In practice, for QD estimation we let <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x65.png" xlink:type="simple"/></inline-formula> to obtain QD estimators and the asymptotic efficiency is identical as QD estimators based on <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x66.png" xlink:type="simple"/></inline-formula> and it is simpler to obtain them numerically.</p><p>For GMM estimation, it is quite straightforward to construct<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x67.png" xlink:type="simple"/></inline-formula>, see expression (4.2) given by Newey and McFadden [<xref ref-type="bibr" rid="scirp.94146-ref11">11</xref>] (p2155). The authors also pointed out that this might not be the case for CMD estimation or QD estimation. This is a point that we shall address when generalizing the quadratic distance methods using a finite number of quantiles to method using quantile function over a continuous range which we shall refer to as continuous quadratic distances (CQD); we shall use an approach based on the influence functions of the sample quantiles to estimate the optimum kernel which is the analogous of the use of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x68.png" xlink:type="simple"/></inline-formula> to estimate <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x69.png" xlink:type="simple"/></inline-formula> for the continuous set-up.</p><p>Continuous GMM theory makes use of Hilbert space linear operator theory and have been developed in details by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] and as mentioned it is closely related to the theory for continuous QD, we shall make use of their results to establish consistency and asymptotic normality of continuous quadratic distance estimators and since the paper aims at providing results for practitioners for their applied works, the presentation will emphasize methodologies with less technicalities so that it might be more suitable for applied researchers for their works. First, we shall briefly outline how to form the quadratic distance to obtain the CQD estimators and postpone the details for later sections of the paper.</p><p>CQD estimators can be viewed as estimators based on minimizing a continuous quadratic form as given by</p><disp-formula id="scirp.94146-formula3"><label>(2)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x70.png"  xlink:type="simple"/></disp-formula><p>with:</p><p>1) <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x71.png" xlink:type="simple"/></inline-formula>is an optimum symmetric positive definite kernel assumed to be fully specified.</p><p>2) a and b are chosen values with a being close to 0 and b close to 1 and<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x72.png" xlink:type="simple"/></inline-formula>.</p><p>In practice, we work with an asymptotic equivalent objective function <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x73.png" xlink:type="simple"/></inline-formula> instead of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x74.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x75.png" xlink:type="simple"/></inline-formula> is estimated by a degenerate kernel<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x76.png" xlink:type="simple"/></inline-formula>, i.e.,</p><disp-formula id="scirp.94146-formula4"><label>. (3)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x77.png"  xlink:type="simple"/></disp-formula><p>Since the kernel <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x78.png" xlink:type="simple"/></inline-formula> is degenerate and in our case, we can find explicitly n eigenvalues <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x79.png" xlink:type="simple"/></inline-formula> with corresponding closed form eigenfunctions<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x80.png" xlink:type="simple"/></inline-formula>. These eigenfunctions can be computed explicitly.</p><p>As in the spectral decomposition of a symmetric positive defined matrix for the Euclidean space, spectral decomposition in Hilbert space allows the kernel</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x81.png" xlink:type="simple"/></inline-formula>to be represented as<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x82.png" xlink:type="simple"/></inline-formula>, and using this</p><p>representation, we can express <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x83.png" xlink:type="simple"/></inline-formula> as a sum of n components, i.e.,</p><disp-formula id="scirp.94146-formula5"><label>(4)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x84.png"  xlink:type="simple"/></disp-formula><p>which is similar to the expression used to obtain continuous GMM estimators as given by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 799).</p><p>Spectral decompositions in functional space have been used in the literature, see Feuerverger and McDunnough [<xref ref-type="bibr" rid="scirp.94146-ref13">13</xref>] (page 312), Durbin [<xref ref-type="bibr" rid="scirp.94146-ref14">14</xref>] (page 292-294). Furthermore, if <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x85.png" xlink:type="simple"/></inline-formula> are not stable, they can be replaced by suitable defined <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x86.png" xlink:type="simple"/></inline-formula> without affecting the asymptotic theory of the CQD estimators. In practice, we work with</p><disp-formula id="scirp.94146-formula6"><label>(5)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x87.png"  xlink:type="simple"/></disp-formula><p>to obtain CQD estimators. Unless otherwise stated, by CQD estimators we mean estimators using the objective function of the form as defined by expression (5).</p><p>Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref6">6</xref>] (page 799) developed perturbation technique, a technique to obtain <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x88.png" xlink:type="simple"/></inline-formula> from the eigenvalues<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x89.png" xlink:type="simple"/></inline-formula>. The perturbation technique will also be used for constructing a degenerate optimum kernel for CQD estimation.</p><p>The objectives of the paper are to develop CQD estimation based on quantiles with the aims to have estimators which are robust in the sense of bounded influence functions and have good efficiencies. For technicalities, we refer to the paper by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] who have introduced continuous GMM estimation.</p><p>The paper is organized as follows. Section 2 gives some preliminary results such as statistical functional and its influence function from which the sample quantiles can be viewed as robust statistics with bounded influence functions. CQD estimation using quantiles will inherit the same robustness property. Some of the standard notions for the study of kernel functions will also be reviewed. By linking a kernel to a linear operator in the Hilbert space of functions which are square integrable over the range <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x90.png" xlink:type="simple"/></inline-formula> with an inner product, it allows a norm <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x91.png" xlink:type="simple"/></inline-formula> to be introduced. Also, the notion of self adjoint linear operator which can be viewed as analogous to a symmetric matrix in Euclidean space is also introduced in Section 2. Section 3 gives asymptotic properties of the CQD estimators based on an estimate optimum kernel. An estimate of the covariance matrix is also given in Section 3.</p><p>Finally, we shall mention that simulation studies are not discussed in this paper as numerical quadrature methods are involved for evaluating the integrals over the range <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x92.png" xlink:type="simple"/></inline-formula> for computing the objective function, we prefer to gather numerical aspects and simulation aspects together for further works and include these type of results in a separate paper leaving this paper focusing only on the methodologies.</p></sec><sec id="s2"><title>2. Some Preliminaries</title><p>In this section we shall review the notion of statistical functional and its influence function and view a sample quantile as a statistical functional. Using its influence function, we can see that the sample quantile is a robust statistic and using the influence functions of two sample quantiles, we can also obtain the asymptotic covariance of the two sample quantiles.</p><sec id="s2_1"><title>2.1. Statistical Functional and Its Influence Function</title><p>Often, a statistic can be represented as a functional of the sample distribution <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x93.png" xlink:type="simple"/></inline-formula> which we can denote by<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x94.png" xlink:type="simple"/></inline-formula>. For example, the sth-sample quantile is defined as<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x95.png" xlink:type="simple"/></inline-formula>. Associated with<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x96.png" xlink:type="simple"/></inline-formula>, there is its influence function which is a weak functional directional derivative at <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x97.png" xlink:type="simple"/></inline-formula> in the direction of<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x98.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x99.png" xlink:type="simple"/></inline-formula>is the degenerate distribution at x. More specifically, the influence function of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x100.png" xlink:type="simple"/></inline-formula> as a function of x is defined as</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x101.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x102.png" xlink:type="simple"/></inline-formula>is a linear function in the functional space. It is not difficult to see that we can also compute <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x103.png" xlink:type="simple"/></inline-formula> using the usual derivative</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x104.png" xlink:type="simple"/></inline-formula>.</p><p>Furthermore, since a Taylor type of approximation in a functional space can be used, we then have the following approximation expressed with a remainder term <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x105.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.94146-formula7"><graphic  xlink:href="//html.scirp.org/file/1-1241235x106.png"  xlink:type="simple"/></disp-formula><p>or equivalently using<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x107.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x108.png" xlink:type="simple"/></inline-formula>and using <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x109.png" xlink:type="simple"/></inline-formula> is linear,</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x110.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x111.png" xlink:type="simple"/></inline-formula>.</p><p>If <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x112.png" xlink:type="simple"/></inline-formula> as a function of x is bounded, the statistics is robust and the remainder is <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x113.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x114.png" xlink:type="simple"/></inline-formula> being a term which converges to 0 in probability faster than <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x115.png" xlink:type="simple"/></inline-formula> as<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x116.png" xlink:type="simple"/></inline-formula>.</p><p>Therefore, if we want to find the asymptotic variance of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x117.png" xlink:type="simple"/></inline-formula>, it is given by the variance of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x118.png" xlink:type="simple"/></inline-formula> as</p><disp-formula id="scirp.94146-formula8"><graphic  xlink:href="//html.scirp.org/file/1-1241235x119.png"  xlink:type="simple"/></disp-formula><p>The influence function of the sth-sample quantile <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x120.png" xlink:type="simple"/></inline-formula> can be obtained and it is given by</p><disp-formula id="scirp.94146-formula9"><label>(6)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x121.png"  xlink:type="simple"/></disp-formula><p>from which we can obtain the asymptotic variance of</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x122.png" xlink:type="simple"/></inline-formula>,</p><p>See Serfing [<xref ref-type="bibr" rid="scirp.94146-ref3">3</xref>] (page236), Hogg et al. [<xref ref-type="bibr" rid="scirp.94146-ref15">15</xref>] (page 593). Also, using the influence function representation for the sth-sample quantile <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x123.png" xlink:type="simple"/></inline-formula> and the corresponding one for the tth-sample quantile<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x124.png" xlink:type="simple"/></inline-formula>, it can be shown that the asymptotic covariance of the following sample quantiles <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x125.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x126.png" xlink:type="simple"/></inline-formula> is given by</p><disp-formula id="scirp.94146-formula10"><graphic  xlink:href="//html.scirp.org/file/1-1241235x127.png"  xlink:type="simple"/></disp-formula><p>see LaRiccia and Wehrly [<xref ref-type="bibr" rid="scirp.94146-ref1">1</xref>] (page 743).</p><p>If we define the covariance kernel as</p><disp-formula id="scirp.94146-formula11"><label>(7)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x128.png"  xlink:type="simple"/></disp-formula><p>then associated to this kernel there is a linear operator <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x129.png" xlink:type="simple"/></inline-formula> in a functional space which can be defined as follows, let a function <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x130.png" xlink:type="simple"/></inline-formula> which belongs to the functional space being considered, K is defined as</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x131.png" xlink:type="simple"/></inline-formula>.</p><p>We can see that for a suitable functional space, it is natural to consider the Hilbert space of functions which are square integrable so that a norm and linear operators can be defined in this space. This will facilitate the studies of kernels which are function of<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x132.png" xlink:type="simple"/></inline-formula>. The necessary notions are introduced in the following section.</p></sec><sec id="s2_2"><title>2.2. Linear Operators Associated with Kernels in a Hilbert Space</title><p>The functional space that we are interested is the space of integrable function with the range <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x133.png" xlink:type="simple"/></inline-formula> and it is natural to introduce an inner product <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x134.png" xlink:type="simple"/></inline-formula> and therefore, a norm <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x135.png" xlink:type="simple"/></inline-formula> can be defined as</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x136.png" xlink:type="simple"/></inline-formula>.</p><p>For a Euclidean space, the composition of two linear operators <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x137.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x138.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x139.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x140.png" xlink:type="simple"/></inline-formula> are matrices produces a matrix <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x141.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x142.png" xlink:type="simple"/></inline-formula>. For linear operators in the Hilbert space the composition of the linear operators <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x143.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x144.png" xlink:type="simple"/></inline-formula> is a linear operator <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x145.png" xlink:type="simple"/></inline-formula> with its kernel <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x146.png" xlink:type="simple"/></inline-formula> and</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x147.png" xlink:type="simple"/></inline-formula>.</p><p>Just as a matrix <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x148.png" xlink:type="simple"/></inline-formula> has its transpose <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x149.png" xlink:type="simple"/></inline-formula> matrix and if <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x150.png" xlink:type="simple"/></inline-formula> is symmetric then<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x151.png" xlink:type="simple"/></inline-formula>, these notions can be extended to a functional space as a linear operator <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x152.png" xlink:type="simple"/></inline-formula> has its adjoint <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x153.png" xlink:type="simple"/></inline-formula> and if the kernel defining <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x154.png" xlink:type="simple"/></inline-formula> is symmetric then<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x155.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x156.png" xlink:type="simple"/></inline-formula>is called self adjoint.</p><p>More precisely, given <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x157.png" xlink:type="simple"/></inline-formula> is found using the following equality, see Definition 6 given by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 823),</p><disp-formula id="scirp.94146-formula12"><graphic  xlink:href="//html.scirp.org/file/1-1241235x158.png"  xlink:type="simple"/></disp-formula><p>Furthermore,</p><p>if <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x159.png" xlink:type="simple"/></inline-formula> then<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x160.png" xlink:type="simple"/></inline-formula>.</p><p>In this paper we focus on positive definite symmetric kernel <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x161.png" xlink:type="simple"/></inline-formula> which can be viewed as the covariance of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x162.png" xlink:type="simple"/></inline-formula> for some stochastic process<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x163.png" xlink:type="simple"/></inline-formula>; therefore, the objective function is of the type <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x164.png" xlink:type="simple"/></inline-formula> is always positive unless <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x165.png" xlink:type="simple"/></inline-formula> then<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x166.png" xlink:type="simple"/></inline-formula>, see Luenberger [<xref ref-type="bibr" rid="scirp.94146-ref16">16</xref>] (page 152) for this notion.</p><p>Unless otherwise stated, we work with linear operators associated with positive definite symmetric kernels. For the Euclidean space if the covariance matrix <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x167.png" xlink:type="simple"/></inline-formula> is invertible with the inverse given by <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x168.png" xlink:type="simple"/></inline-formula> assumed to exist after regularizations then there are symmetric positive definite symmetric matrices denoted by <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x169.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x170.png" xlink:type="simple"/></inline-formula> so that</p><disp-formula id="scirp.94146-formula13"><label>(8)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x171.png"  xlink:type="simple"/></disp-formula><p>see Hogg et al. [<xref ref-type="bibr" rid="scirp.94146-ref15">15</xref>] (pages 179-180) for square root of a symmetric positive definite matrices and they can be computed using the technique of spectral decomposition of matrices.</p><p>If <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x172.png" xlink:type="simple"/></inline-formula> is linear operator with covariance kernel<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x173.png" xlink:type="simple"/></inline-formula>, the analogous properties given by expression (8) continues to hold but unlike matrices where closed forms for the matrices can be found, one might not be able to display the kernel of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x174.png" xlink:type="simple"/></inline-formula> or <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x175.png" xlink:type="simple"/></inline-formula> explicitly as no closed form expressions are available despite that both <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x176.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x177.png" xlink:type="simple"/></inline-formula> exist subject to some technical regularizations as discussed in section 4 by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (pages 506-510).</p><p>For our purpose, we shall focus on a linear operator <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x178.png" xlink:type="simple"/></inline-formula> with its kernel defined by Equation (7) for the rest of the paper. Since <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x179.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x180.png" xlink:type="simple"/></inline-formula> are related and if we can construct an estimator for<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x181.png" xlink:type="simple"/></inline-formula>, we can construct an estimator for <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x182.png" xlink:type="simple"/></inline-formula> and the construction of these estimators will be discussed in the next sub-section.</p></sec><sec id="s2_3"><title>2.3. Estimation of K and K<sup>−1</sup></title><p>The methods used to construct an estimator for <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x183.png" xlink:type="simple"/></inline-formula> follows from the techniques proposed by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] . The steps are given below:</p><p>1) We need a preliminary consistent estimate <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x184.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x185.png" xlink:type="simple"/></inline-formula>, for our case we can minimize the following simple objective function to obtain<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x186.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x187.png" xlink:type="simple"/></inline-formula>.</p><p>2) Use <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x188.png" xlink:type="simple"/></inline-formula> and the sample of observations to construct a degenerate kernel <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x189.png" xlink:type="simple"/></inline-formula> which has the form</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x190.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x191.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x192.png" xlink:type="simple"/></inline-formula> depends on<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x191.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x192.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x193.png" xlink:type="simple"/></inline-formula>.</p><p>For our set-up, i.e., CQD estimation, we should use the influence function of the sample quantiles as given by expression (6) to specify<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x194.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x195.png" xlink:type="simple"/></inline-formula>.</p><p>The notion of influence function was not mentioned in Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] .</p><p>3) Since <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x196.png" xlink:type="simple"/></inline-formula> is a degenerate kernel it only has n eigenvalues <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x196.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x197.png" xlink:type="simple"/></inline-formula> with the corresponding eigenvectors<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x196.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x197.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x198.png" xlink:type="simple"/></inline-formula>, these eigenvectors have closed forms. The procedures to find these eigenvalues and eigenvectors have been given Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 805) and will be summarized in the next paragraphs. Let <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x196.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x197.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x199.png" xlink:type="simple"/></inline-formula> be one of these n eigenvalues with its corresponding eigenvector<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x196.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x197.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x200.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x196.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x197.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x201.png" xlink:type="simple"/></inline-formula>needs to satisfy</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x202.png" xlink:type="simple"/></inline-formula>, i.e.,<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x203.png" xlink:type="simple"/></inline-formula>.</p><p>4) Use the spectral decomposition to express <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x204.png" xlink:type="simple"/></inline-formula> using its eigenvalues and eigenfunctions, i.e.,</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x205.png" xlink:type="simple"/></inline-formula>.</p><p>The above expression is similar to the representation of a positive definite matrix <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x206.png" xlink:type="simple"/></inline-formula> using the spectral decomposition and from which we only need to adjust the eigenvalues if we want to find<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x207.png" xlink:type="simple"/></inline-formula>, the inverse of the matrix <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x208.png" xlink:type="simple"/></inline-formula> or the matrices <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x209.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x209.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x210.png" xlink:type="simple"/></inline-formula>.</p><p>We can proceed as follows in order to find <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x211.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x212.png" xlink:type="simple"/></inline-formula>, following Carraco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 805). First we form a matrix <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x211.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x213.png" xlink:type="simple"/></inline-formula> with</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x214.png" xlink:type="simple"/></inline-formula>.</p><p>It turns out that <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x215.png" xlink:type="simple"/></inline-formula> for each j is also an eigenvalue of the matrix <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x216.png" xlink:type="simple"/></inline-formula> and its eigenvectors is <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x217.png" xlink:type="simple"/></inline-formula>with respect to the matrix <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x216.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x217.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x218.png" xlink:type="simple"/></inline-formula> with</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x219.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x219.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x220.png" xlink:type="simple"/></inline-formula>.</p><p>The eigenfunction can be expressed as <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x221.png" xlink:type="simple"/></inline-formula> and they</p><p>can be computed as statistical packages often offer routines to compute eigenvalues and eigenvectors for a given matrix.</p><p>For numerical evaluations of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x222.png" xlink:type="simple"/></inline-formula> a numerical quadrature procedure is needed to compute the integrals over a range<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x222.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x223.png" xlink:type="simple"/></inline-formula>.</p><p>Now we turn into attention of constructing <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x224.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x225.png" xlink:type="simple"/></inline-formula> to estimate <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x226.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x226.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x227.png" xlink:type="simple"/></inline-formula>.</p><p>It appears then the kernel of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x228.png" xlink:type="simple"/></inline-formula> can be defined as</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x229.png" xlink:type="simple"/></inline-formula>, see Definition 3 given by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 807). Howewer, Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 799) have shown that <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x230.png" xlink:type="simple"/></inline-formula> will create numerical instabilities and need to be regularized and instead of<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x231.png" xlink:type="simple"/></inline-formula>, we need to replace it by<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x231.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x232.png" xlink:type="simple"/></inline-formula>, and since <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x231.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x233.png" xlink:type="simple"/></inline-formula> are positive in probability, we can also let <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x230.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x231.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x233.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x234.png" xlink:type="simple"/></inline-formula> and these expressions might be easier to handle numerically.</p><p>Now we can define define <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x235.png" xlink:type="simple"/></inline-formula> to be the kernel of<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x236.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x236.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x237.png" xlink:type="simple"/></inline-formula>will be a valid estimator for <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x236.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x238.png" xlink:type="simple"/></inline-formula> providing that the sequence <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x236.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x238.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x239.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x236.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x237.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x238.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x239.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x240.png" xlink:type="simple"/></inline-formula> using their Theorem 7 on page 810.</p><p>For example, if we let <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x241.png" xlink:type="simple"/></inline-formula> for some d chosen to be positive then the requirements for the sequence <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x241.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x242.png" xlink:type="simple"/></inline-formula> are met.</p><p>This also means that the kernel for <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x243.png" xlink:type="simple"/></inline-formula> can be defined as</p><disp-formula id="scirp.94146-formula14"><label>(9)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x244.png"  xlink:type="simple"/></disp-formula><p>and again <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x245.png" xlink:type="simple"/></inline-formula> is a valid estimator for<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x245.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x246.png" xlink:type="simple"/></inline-formula>.</p><p>This also means that <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x247.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x247.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x248.png" xlink:type="simple"/></inline-formula> can be replaced by <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x247.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x248.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x249.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x247.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x248.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x249.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x250.png" xlink:type="simple"/></inline-formula> whenever they appear in expressions or equations used to derive asymptotic properties for the CQD estimators based on their Theorem 7.</p><p>In Section 3 we shall turn our attention to asymptotic properties of CQD estimators using the objective function <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x251.png" xlink:type="simple"/></inline-formula> an using the norm<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x251.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x252.png" xlink:type="simple"/></inline-formula>, it can also be expressed neatly as</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x253.png" xlink:type="simple"/></inline-formula>with <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x253.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x254.png" xlink:type="simple"/></inline-formula> and</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x255.png" xlink:type="simple"/></inline-formula>is the linear operator as defined by expression (9).</p><p>For consistency, we shall make use the basic consistency Theorem, i.e., Theorem 2.1 as given by Newey and McFadden [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 2121). For establishing asymptotic normality for the CQD estimators, the procedures are similar to those used for establishing asymptotic normality of continuous GMM estimators as given by Theorem 8 given by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 811, page 825).</p></sec></sec><sec id="s3"><title>3. Asymptotic Properties</title><sec id="s3_1"><title>3.1. Consistency</title><p>Assuming <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x256.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x256.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x257.png" xlink:type="simple"/></inline-formula> is compact and observe that</p><disp-formula id="scirp.94146-formula15"><label>. (10)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x258.png"  xlink:type="simple"/></disp-formula><p>Now if we assume that the integrand can be dominated by a function <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x259.png" xlink:type="simple"/></inline-formula> which does not depend <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x260.png" xlink:type="simple"/></inline-formula> and furthermore <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x260.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x261.png" xlink:type="simple"/></inline-formula> then we have uniform convergence in probability, i.e., <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x259.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x260.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x261.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x262.png" xlink:type="simple"/></inline-formula>uniformly with</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x263.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x264.png" xlink:type="simple"/></inline-formula>is the optimum symmetric positive definite kernel of<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x265.png" xlink:type="simple"/></inline-formula>. Therefore, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x266.png" xlink:type="simple"/></inline-formula>is uniquely minimized at<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x266.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x267.png" xlink:type="simple"/></inline-formula>, this implies consistency of the CQD estimators given by the vector <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x266.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x267.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x268.png" xlink:type="simple"/></inline-formula> using the basic consistency Theorem. Therefore, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x266.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x267.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x268.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x269.png" xlink:type="simple"/></inline-formula>, the symbol <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x266.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x267.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x268.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x269.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x270.png" xlink:type="simple"/></inline-formula> denotes convergence in probability. We implicitly assume that the conditions <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x266.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x267.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x268.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x269.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x270.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x271.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x264.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x265.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x266.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x267.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x268.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x269.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x270.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x271.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x272.png" xlink:type="simple"/></inline-formula> are met.</p></sec><sec id="s3_2"><title>3.2. Asymptotic Normality</title><p>The basic assumption used to establish asymptotic normality for the CQD estimators is the model quantile function is twice differentiable which allows a standard Taylor expansion the estimating equations.</p><p>Assuming the first derivative vector <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x273.png" xlink:type="simple"/></inline-formula> and the second derivative matrix</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x274.png" xlink:type="simple"/></inline-formula>exist.</p><p>Before considering the Taylor expansion, we also need the following notation and the notion of a random element with zero mean and covariance given by the kernel of the associated linear operator K, i.e., <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x275.png" xlink:type="simple"/></inline-formula>, see Remark 2 as given by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 803). Note that if we let<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x275.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x276.png" xlink:type="simple"/></inline-formula>, using the Mean value Theorem, we then have</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x277.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x278.png" xlink:type="simple"/></inline-formula>lies in the segment joining <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x278.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x279.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x278.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x279.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x280.png" xlink:type="simple"/></inline-formula>. Now we have <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x278.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x279.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x280.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x281.png" xlink:type="simple"/></inline-formula> which satisfies <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x278.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x279.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x280.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x281.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x282.png" xlink:type="simple"/></inline-formula> which is also given by</p><disp-formula id="scirp.94146-formula16"><label>(11)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x283.png"  xlink:type="simple"/></disp-formula><p>as <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x284.png" xlink:type="simple"/></inline-formula> is symmetric. Using inner product and Hilbert space as in the proofs of Theorem 2 by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 825), expression (11) can be expressed as</p><disp-formula id="scirp.94146-formula17"><label>. (12)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x285.png"  xlink:type="simple"/></disp-formula><p>Using expression (12), we then have</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x286.png" xlink:type="simple"/></inline-formula>.</p><p>Now using <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x287.png" xlink:type="simple"/></inline-formula> is a linear operator, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x287.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x288.png" xlink:type="simple"/></inline-formula>, rearranging the terms gives the following equality in distribution</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x289.png" xlink:type="simple"/></inline-formula>.</p><p>Note that <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x290.png" xlink:type="simple"/></inline-formula> and the symbol <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x290.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x291.png" xlink:type="simple"/></inline-formula> denotes equality in distribution.</p><p>Let <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x292.png" xlink:type="simple"/></inline-formula></p><p>And <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x293.png" xlink:type="simple"/></inline-formula> then it is easy to see that</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x294.png" xlink:type="simple"/></inline-formula>,</p><p>so that</p><disp-formula id="scirp.94146-formula18"><label>(13)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x295.png"  xlink:type="simple"/></disp-formula><p>with the symbol <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x296.png" xlink:type="simple"/></inline-formula> denotes convergence in law or in distribution.</p><p>The matrix <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x297.png" xlink:type="simple"/></inline-formula> plays the same role as the information matrix for maximum likelihood (ML) estimation. Clearly, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x297.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x298.png" xlink:type="simple"/></inline-formula>needs to be estimated, an estimate is given as</p><disp-formula id="scirp.94146-formula19"><label>, (14)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x299.png"  xlink:type="simple"/></disp-formula><p>using the spectral decomposition technique, the <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x300.png" xlink:type="simple"/></inline-formula> element of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x300.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x301.png" xlink:type="simple"/></inline-formula> can be expressed as</p><disp-formula id="scirp.94146-formula20"><label>(15)</label><graphic position="anchor" xlink:href="//html.scirp.org/file/1-1241235x302.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s4"><title>4. Summary and Conclusion</title><p>The proposed method is similar to the continuous GMM method with the estimators obtained using sample distribution function obtained by minimizing</p><p><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x303.png" xlink:type="simple"/></inline-formula>with <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x303.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x304.png" xlink:type="simple"/></inline-formula></p><p>being an optimum kernel but using a sample distribution function <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x305.png" xlink:type="simple"/></inline-formula> instead of the sample quantile function as studied by Carrasco and Florens [<xref ref-type="bibr" rid="scirp.94146-ref12">12</xref>] (page 816) for nonnegative continuous distributions. The kernel <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x305.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x306.png" xlink:type="simple"/></inline-formula> is constructed with the use of<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x305.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x306.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x307.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x305.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x306.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x307.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x308.png" xlink:type="simple"/></inline-formula>being the usual indicator function.</p><p>The authors also showed that by letting<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x309.png" xlink:type="simple"/></inline-formula>, the continuous GMM estimators are as efficient as ML estimators.</p><p>For robustness sake for continuous GMM estimation we might want to let 𝑇 be finite and the lower bound be <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x310.png" xlink:type="simple"/></inline-formula> so that the optimum kernel <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x310.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x311.png" xlink:type="simple"/></inline-formula> remains bounded for the regions of the double integrals used to define the continuous GMM objective function. This can be viewed as equivalent to choose <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x310.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x311.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x312.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x310.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x311.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x312.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x313.png" xlink:type="simple"/></inline-formula> for the integrals of the objective function for CQD estimation. For robustness sake, it appears simpler to work with the domain (a, b) instead of <inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x310.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x311.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x312.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x313.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x314.png" xlink:type="simple"/></inline-formula> as numerical quadrature methods applied over the range (a, b) might be simpler to implement. We conjecture that CQD estimators can also be fully efficient just as the continuous GMM estimators as defined above despite a proof is still lacking for the time being by letting<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x310.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x311.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x312.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x313.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x314.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x315.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x310.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x311.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x312.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x313.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x314.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x315.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="//html.scirp.org/file/1-1241235x316.png" xlink:type="simple"/></inline-formula>. More numerical and more simulation studies are needed but we hope that based on the presentation of this paper the proposed method is implementable and its asymptotic properties useful so that applied researchers might want to consider to use them for their works especially for fitting models where the model quantile function is simpler to handle than its model distribution or density function and especially when there is a need for robust estimation with the data.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The helpful and constructive comments of a referee which lead to an improvement of the presentation of the paper and support from the editorial staffs of Open Journal of Statistics to process the paper are all gratefully acknowledged.</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Luong, A. (2019) Robust Continuous Quadratic Distance Estimation Using Quantiles for Fitting Continuous Distributions. Open Journal of Statistics, 9, 421-435. https://doi.org/10.4236/ojs.2019.94028</p></sec></body><back><ref-list><title>References</title><ref id="scirp.94146-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">LaRiccia, V.N. and Wehrly, T.E. (1985) Asymptotic Properties of a Family of Minimum Quantile Distance Estimators. Journal of the American Statistical Association, 80, 742-747. https://doi.org/10.1080/01621459.1985.10478178</mixed-citation></ref><ref id="scirp.94146-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Castillo, E., Hadi, A.S., Balakrishnan, N. and Sarabia, J.M. (2005) Extreme Value and Related Models with Applications in Engineering and Science. Wiley, New York.</mixed-citation></ref><ref id="scirp.94146-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Serfling, R.J. (1980) Approximation Theorems of Mathematical Statistics. Wiley, New York. https://doi.org/10.1002/9780470316481</mixed-citation></ref><ref id="scirp.94146-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Hosking, J.R.M. and Wallis, J.R. (1987) Parameter and Quantile Estimation for the Generalized Pareto Distribution. Technometrics, 29, 339-349.  
https://doi.org/10.1080/00401706.1987.10488243</mixed-citation></ref><ref id="scirp.94146-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Kotz, S. and Nadarajah, S. (2000) Extreme Value Distributions. Imperial College Press, London. https://doi.org/10.1142/p191</mixed-citation></ref><ref id="scirp.94146-ref6"><label>6</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Dupuis</surname><given-names> D.J. </given-names></name>,<etal>et al</etal>. (<year>1988</year>)<article-title>Exceedances over High Thresholds: A Guide to Threshold Selection</article-title><source> Extremes</source><volume> 1</volume>,<fpage> 251</fpage>-<lpage>261</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.94146-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Juarez, S.F. and Schucany, W.R. (2004) Robust and Efficient Estimation for the Generalized Pareto Distribution. Extremes, 7, 237-251.  
https://doi.org/10.1007/s10687-005-6475-6</mixed-citation></ref><ref id="scirp.94146-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Klugman, S.A., Panjer, H.H. and Willmot, G.E. (2012) Loss Models: From Data to Decisions. Fourth Edition, Wiley, New York.  
https://doi.org/10.1002/9781118787106</mixed-citation></ref><ref id="scirp.94146-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Castillo, E. and Hadi, A.S. (1997) Fitting the Generalized Pareto Distribution to Data. Journal of the American Statistical Association, 92, 1619-1620.  
https://doi.org/10.1080/01621459.1997.10473683</mixed-citation></ref><ref id="scirp.94146-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Luong, A. and Thompson, M.E. (1987) Minimum Distance Methods Based on Quadratic Distance for Transforms. Canadian Journal of Statistics, 15, 239-251.  
https://doi.org/10.2307/3314914</mixed-citation></ref><ref id="scirp.94146-ref11"><label>11</label><mixed-citation publication-type="book" xlink:type="simple">Newey, W.K. and McFadden, D. (1994) Large Sample Estimation and Hypothesis Testing. In: Engle, R. and McFadden, D., Eds., Handbook of Econometrics, Volume 4, Elsevier, Amsterdam, 419-554.</mixed-citation></ref><ref id="scirp.94146-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Carrasco, M. and Florens, J.-P. (2000) Generalization of GMM to a Continuum of Moment Condition. Econometric Theory, 16, 797-834.  
https://doi.org/10.1017/S0266466600166010</mixed-citation></ref><ref id="scirp.94146-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Feuerverger, A. and McDunnough, P. (1984) On Statistical Transform Methods and Their Efficiency. Canadian Journal of Statistics, 12, 303-317.  
https://doi.org/10.2307/3314814</mixed-citation></ref><ref id="scirp.94146-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Durbin, J. and Knott, M. (1972) Components of the Cramer-von Mises Statistics. Journal of the Royal Statistical Society, Series B, 34, 290-307.  
https://doi.org/10.1111/j.2517-6161.1972.tb00908.x</mixed-citation></ref><ref id="scirp.94146-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Hogg, R.V., McKean, J.W. and Craig, A.T. (2013) Introduction to Mathematical Statistics. Seventh Edition, Pearson, Hoboken.</mixed-citation></ref><ref id="scirp.94146-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Luenberger, D.G. (1968) Optimization by Vector Space Methods. Wiley, New York.</mixed-citation></ref></ref-list></back></article>