<?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.2022.122018</article-id><article-id pub-id-type="publisher-id">OJS-116726</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  A Comparison of the Estimators of the Scale Parameter of the Errors Distribution in the L&lt;sub&gt;1&lt;/sub&gt; Regression
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Carmen</surname><given-names>D. Saldiva de André</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Silvia</surname><given-names>Nagib Elian</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Institute of Mathematics and Statistics, University of S&amp;amp;atilde;o Paulo, S&amp;amp;atilde;o Paulo, Brazil</addr-line></aff><pub-date pub-type="epub"><day>14</day><month>03</month><year>2022</year></pub-date><volume>12</volume><issue>02</issue><fpage>261</fpage><lpage>276</lpage><history><date date-type="received"><day>18,</day>	<month>March</month>	<year>2022</year></date><date date-type="rev-recd"><day>21,</day>	<month>April</month>	<year>2022</year>	</date><date date-type="accepted"><day>24,</day>	<month>April</month>	<year>2022</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The L<sub>1</sub> regression is a robust alternative to the least squares regression whenever there are outliers in the values of the response variable, or the errors follow a long-tailed distribution.
   
  To calculate the standard errors of the L<sub>1</sub> estimators, construct confidence intervals and test hypotheses about the parameters of the model, or to calculate a robust coefficient of determination, it is necessary to have an estimate of a scale parameter
  τ
  .
   This parameter is such that 
  τ<sup>2</sup>/
  n
   
  is the variance of the median of a sample of size n from the errors distribution. 
  [1] 
  proposed the use of , a consistent, and so, an asymptotically unbiased estimator of τ. However, this estimator is not stable in small samples, in the sense that it can increase with the introduction of new independent variables in the model. When the errors follow the Laplace distribution, the maximum likelihood estimator of τ, say <inline-formula><inline-graphic xlink:href="dit_e07c570d-f1ab-4578-99fd-81b324bac5a3.png" xlink:type="simple"/></inline-formula>, is the mean absolute error, that is, the mean of the absolute residuals. This estimator always decreases when new independent variables are added to the model. Our objective is to develop asymptotic properties of <inline-formula><inline-graphic xlink:href="dit_fd8cb634-cf1c-4110-9f89-ec820f657cfd.png" xlink:type="simple"/></inline-formula> under several errors distributions analytically. We also performed a simulation study to compare the distributions of both estimators in small samples with the objective to establish conditions in which <inline-formula><inline-graphic xlink:href="dit_6df3abe6-cbfd-4408-a4a5-6ca9bc091e7c.png" xlink:type="simple"/></inline-formula>is a good alternative to <inline-formula><inline-graphic xlink:href="dit_bcf0b458-2802-40aa-83ff-1cd0f91aa0b9.png" xlink:type="simple"/></inline-formula> for such situations.
  
 
</p></abstract><kwd-group><kwd>Minimum Sum of Absolute Errors Regression</kwd><kwd> Multiple Linear Regression</kwd><kwd> Variable Selection</kwd><kwd> Heavy Tail Distributions</kwd><kwd> Asymptotic Theory</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Consider the multiple linear regression model</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x7.png" xlink:type="simple"/></inline-formula>,</p><p>where</p><p>y is an n &#215; 1 vector of values of the response variable corresponding to X, an n &#215; k matrix of predictor variables that may include a column of ones for the intercept term;</p><p>β is a k &#215; 1 vector of unknown parameters and;</p><p>ε is an n &#215; 1 vector of unobservable random errors.</p><p>The components of ε are independent and identically distributed random variables with cumulative distribution function F. Suppose that F has a unique median equal to zero and a continuous derivative f in the neighborhood of zero such that f(0) &gt; 0. The scale parameter of f is defined as</p><disp-formula id="scirp.116726-formula3"><label>. (1.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-1241601x8.png"  xlink:type="simple"/></disp-formula><p>So τ<sup>2</sup>/n is the variance of the median in a sample of size n from the error distribution.</p><p>The L<sub>1</sub> estimator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x9.png" xlink:type="simple"/></inline-formula> of β, minimizes <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x10.png" xlink:type="simple"/></inline-formula> for all values of β, where y<sub>i</sub> is the i-th element of the vector y and x<sub>i</sub> is the i-th row of the matrix X.</p><p>The L<sub>1</sub> criterion is a robust alternative to the least squares regression whenever the data contains outliers or the errors follow a long tailed distribution such as Laplace or Cauchy.</p><p>It is well known that when the errors follow Laplace distribution, the L<sub>1</sub> estimators of β are maximum likelihood estimators and so, they are asymptotically unbiased and efficient. [<xref ref-type="bibr" rid="scirp.116726-ref2">2</xref>] proved that the L<sub>1</sub> estimator is asymptotically unbiased, consistent and follows a multinormal distribution with covariance matrix τ<sup>2</sup>(X'X)<sup>−1</sup>. An important implication of this result is that the L<sub>1</sub> estimator of β has a smaller confidence ellipsoid than the least squares estimator for any error distribution for which the sample median is a more efficient estimator than the sample mean.</p><p>Based on the asymptotic distribution results, formulae for constructing confidence intervals and testing hypotheses on the parameters of the model have been developed [<xref ref-type="bibr" rid="scirp.116726-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.116726-ref4">4</xref>]. To apply these formulae and also to compute the standard errors of the estimators of β, it is necessary to have an estimate of the parameter τ. Several estimators of τ were proposed [<xref ref-type="bibr" rid="scirp.116726-ref1">1</xref>]. They recommend the consistent estimator</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x12.png" xlink:type="simple"/></inline-formula>,</p><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x13.png" xlink:type="simple"/></inline-formula>,</p><p>n<sup>*</sup> is the number of non-zero residuals and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x14.png" xlink:type="simple"/></inline-formula> are the non-zero residuals arranged in ascending order.</p><p>It is important to observe that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x15.png" xlink:type="simple"/></inline-formula> is a measure of the variability of the residuals and, although is influenced by all of them, it is determined by only two of them.</p><p>A consistent estimator of τ is also needed to calculate the robust coefficient of determination R proposed by [<xref ref-type="bibr" rid="scirp.116726-ref5">5</xref>]. This coefficient is an informal measure of goodness of fit of a model and it is given by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x16.png" xlink:type="simple"/></inline-formula>,</p><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x17.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x18.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x19.png" xlink:type="simple"/></inline-formula>is the predicted value of the response variable in the i-th observation, that is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x20.png" xlink:type="simple"/></inline-formula>;</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x21.png" xlink:type="simple"/></inline-formula>is the L<sub>1</sub> estimator of the regression coefficients of the model.</p><p>A desirable property for a coefficient of determination is that it increases when passing from a reduced to a full model, that is, when new predictor variables are included in the model [<xref ref-type="bibr" rid="scirp.116726-ref6">6</xref>]. For R<sub>2</sub> this property is true only if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x22.png" xlink:type="simple"/></inline-formula> decreases as new variables are included in the model and this might not happen, as shown in Example 1.</p><p>Example 1—In this example, we use the real state data from [<xref ref-type="bibr" rid="scirp.116726-ref7">7</xref>]. The predictor variables are taxes, in hundred dollars (X<sub>1</sub>), lot area, in thousand squares feet (X<sub>2</sub>), living space, in thousand squares feet (X<sub>3</sub>), age of the home, in years (X<sub>4</sub>). The response variable (Y) is the selling price of the home, in thousands of dollars.</p><p>In <xref ref-type="table" rid="table1"><xref ref-type="table" rid="table">Table </xref>1</xref>, we present all possible linear models obtained with the four predicted variables, the number of parameters (k), the estimates <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x23.png" xlink:type="simple"/></inline-formula> and the values of R<sub>2</sub> for each model. In this table, we see that the value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x24.png" xlink:type="simple"/></inline-formula> for the model with variable X<sub>1</sub> only (4.0079) is smaller than the observed value of this statistic in the model with X<sub>1</sub> and X<sub>3</sub> (5.4301), and then the value of R<sub>2</sub> in the model containing only X<sub>1</sub> as predictor is larger than in the model with X<sub>1</sub> and X<sub>3</sub>. However, the contribution of X<sub>3</sub> given that X<sub>1</sub> is already in the model is significant (p-value less than 0.01).</p><p>So, it may happen that the value of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x25.png" xlink:type="simple"/></inline-formula> increases even with the introduction of a variable with significant contribution in the model. This fact will decrease the value of R<sub>2</sub> and the new model might not be selected if the coefficient of determination is the criterion to select a model.</p><p>This instable behavior of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x26.png" xlink:type="simple"/></inline-formula> may be explained by the fact that it is determined by only two residuals and so we can expect that it happens more frequently in small samples.</p><p>When errors follow the Laplace distribution, the maximum likelihood estimator of τ is the mean absolute error [<xref ref-type="bibr" rid="scirp.116726-ref8">8</xref>], given by</p><disp-formula id="scirp.116726-formula4"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x27.png"  xlink:type="simple"/></disp-formula><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x28.png" xlink:type="simple"/></inline-formula>.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1"><xref ref-type="table" rid="table">Table </xref>1</xref></label><caption><title> Number of parameters (k), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x29.png" xlink:type="simple"/></inline-formula>and R<sub>2</sub> observed values for all possible regression models for the state data</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Variables in the model</th><th align="center" valign="middle" >k</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x30.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >R<sub>2</sub></th></tr></thead><tr><td align="center" valign="middle" >nothing</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >10.9629</td><td align="center" valign="middle" >0.0000</td></tr><tr><td align="center" valign="middle" >x<sub>1</sub></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >4.0079</td><td align="center" valign="middle" >0.7105</td></tr><tr><td align="center" valign="middle" >x<sub>2</sub></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >8.0285</td><td align="center" valign="middle" >0.3830</td></tr><tr><td align="center" valign="middle" >x<sub>3</sub></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >9.8973</td><td align="center" valign="middle" >0.4681</td></tr><tr><td align="center" valign="middle" >x<sub>4</sub></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >11.8750</td><td align="center" valign="middle" >0.1164</td></tr><tr><td align="center" valign="middle" >x<sub>1</sub>&#183;x<sub>2</sub></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3.9590</td><td align="center" valign="middle" >0.7215</td></tr><tr><td align="center" valign="middle" >x<sub>1</sub>&#183;x<sub>3</sub></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >5.4301</td><td align="center" valign="middle" >0.6860</td></tr><tr><td align="center" valign="middle" >x<sub>1</sub>&#183;x<sub>4</sub></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3.9636</td><td align="center" valign="middle" >0.7212</td></tr><tr><td align="center" valign="middle" >x<sub>2</sub>&#183;x<sub>3</sub></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >8.0913</td><td align="center" valign="middle" >0.5470</td></tr><tr><td align="center" valign="middle" >x<sub>2</sub>&#183;x<sub>4</sub></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >6.5918</td><td align="center" valign="middle" >0.4576</td></tr><tr><td align="center" valign="middle" >x<sub>3</sub>&#183;x<sub>4</sub></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >6.6577</td><td align="center" valign="middle" >0.6098</td></tr><tr><td align="center" valign="middle" >x<sub>1</sub>&#183;x<sub>2</sub>&#183;x<sub>3</sub></td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >6.1331</td><td align="center" valign="middle" >0.6701</td></tr><tr><td align="center" valign="middle" >x<sub>1</sub>&#183;x<sub>2</sub>&#183;x<sub>4</sub></td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >7.3275</td><td align="center" valign="middle" >0.5937</td></tr><tr><td align="center" valign="middle" >x<sub>1</sub>&#183;x<sub>3</sub>&#183;x<sub>4</sub></td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >5.4875</td><td align="center" valign="middle" >0.7011</td></tr><tr><td align="center" valign="middle" >x<sub>2</sub>&#183;x<sub>3</sub>&#183;x<sub>4</sub></td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >4.0022</td><td align="center" valign="middle" >0.7410</td></tr><tr><td align="center" valign="middle" >x<sub>1</sub>&#183;x<sub>2</sub>&#183;x<sub>3</sub>&#183;x<sub>4</sub></td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >4.0246</td><td align="center" valign="middle" >0.7704</td></tr></tbody></table></table-wrap><p>Although the usual regularity conditions do not hold for Laplace distribution, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x31.png" xlink:type="simple"/></inline-formula>is a consistent estimator of τ [<xref ref-type="bibr" rid="scirp.116726-ref9">9</xref>]. This estimator is a measure of variability of the residuals, and it has the property of decreasing when new predictor variables are included in the model. Using this estimator, it is possible to construct a robust coefficient of determination that satisfies the desirable conditions in [<xref ref-type="bibr" rid="scirp.116726-ref6">6</xref>]. It is possible also to calculate the coefficient of determination adjusted by the number of predictor variables proposed in [<xref ref-type="bibr" rid="scirp.116726-ref10">10</xref>].</p><p>Our objective is to study the possibility of using <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x32.png" xlink:type="simple"/></inline-formula> as an alternative to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x33.png" xlink:type="simple"/></inline-formula> when the errors follow a distribution other than Laplace. We have special interest in small sample sizes because of the instable behavior of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x34.png" xlink:type="simple"/></inline-formula> in such cases.</p><p>[<xref ref-type="bibr" rid="scirp.116726-ref11">11</xref>] pointed out the importance of the L<sub>1</sub> method of estimation, presenting many practical situations in which its application is recommended. So, the search of procedures that make its use more efficient gives important contribution to the statistical theory.</p><p>The paper is organized as follows. Initially, the asymptotic distributions of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x35.png" xlink:type="simple"/></inline-formula> were derived analytically assuming errors with Normal, Mixture of Normals, Laplace and Logistic distributions. These results allowed to compute the asymptotic bias and mean squared error of this estimator. Then, we performed a simulation study and generated empirical distributions of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x36.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x37.png" xlink:type="simple"/></inline-formula> in small samples, after the fitting of models with one predictor variable and errors with the same distributions considered previously and Cauchy distribution also. The distributions considered in this study were characterized according to the weight of their tails [<xref ref-type="bibr" rid="scirp.116726-ref12">12</xref>]. The results obtained in this study allowed indicating situations in which <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x38.png" xlink:type="simple"/></inline-formula> can be used as an alternative to estimate τ.</p></sec><sec id="s2"><title>2. Asymptotic Distribution of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x39.png" xlink:type="simple"/></inline-formula></title><p>In this section, we derive analytically the asymptotic distribution of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x40.png" xlink:type="simple"/></inline-formula>, considering four different distributions for the errors. We assume errors with normal (0, σ<sup>2</sup>) distribution, mixture of Normals when random variables are selected from a normal (0, 1) with probability p and of a normal (0, σ<sup>2</sup>) with probability 1 − p, Logistic distribution with mean zero and variance γ<sup>2</sup>π<sup>2</sup>/3 and Laplace distribution with mean zero and variance 2σ<sup>2</sup>.</p><p>First, we note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x41.png" xlink:type="simple"/></inline-formula> may be written as</p><disp-formula id="scirp.116726-formula5"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x42.png"  xlink:type="simple"/></disp-formula><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x43.png" xlink:type="simple"/></inline-formula>is the L<sub>1</sub> estimator of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x44.png" xlink:type="simple"/></inline-formula>.</p><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x45.png" xlink:type="simple"/></inline-formula> is a consistent estimator of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x46.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.116726-ref2">2</xref>], the asymptotic distribution of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x47.png" xlink:type="simple"/></inline-formula> is the same of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x48.png" xlink:type="simple"/></inline-formula>, and this quantity is equal to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x49.png" xlink:type="simple"/></inline-formula>, where ε<sub>i</sub> is the i-th element of the vector of errors of the model. Next, we study the asymptotic distribution of this random variable for different errors distributions.</p></sec><sec id="s3"><title>3. Errors with Normal (0, σ<sup>2</sup>) Distribution</title><p>Using the fact that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x50.png" xlink:type="simple"/></inline-formula> we observe (see Appendix A) that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x51.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x52.png" xlink:type="simple"/></inline-formula>.</p><p>Further, the random variables<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x53.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x54.png" xlink:type="simple"/></inline-formula>, are independent and identically distributed and, by the Central-limit theorem</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x55.png" xlink:type="simple"/></inline-formula>.</p><p>So, it follows that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x56.png" xlink:type="simple"/></inline-formula>.</p><p>Finally, since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x57.png" xlink:type="simple"/></inline-formula> then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x58.png" xlink:type="simple"/></inline-formula>, which implies that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x59.png" xlink:type="simple"/></inline-formula>,</p><p>or that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x60.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. Errors with Mixture of Normal Distributions</title><p>In this case, we assume that the errors distribution is a mixture of two normal distributions: a Normal (0, 1) selected with probability p and a Normal (0, σ<sup>2</sup>) selected with probability (1 − p). Hence, the probability density function of ε<sub>i</sub> is</p><disp-formula id="scirp.116726-formula6"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x61.png"  xlink:type="simple"/></disp-formula><p>It is not very difficult to see that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x62.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x63.png" xlink:type="simple"/></inline-formula>and that the parameter τ is</p><disp-formula id="scirp.116726-formula7"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x64.png"  xlink:type="simple"/></disp-formula><p>Furthermore, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x65.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x66.png" xlink:type="simple"/></inline-formula>are independent and identically distributed random variables with mean and variance (see Appendix A) given by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x67.png" xlink:type="simple"/></inline-formula>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x68.png" xlink:type="simple"/></inline-formula>.</p><p>So, as the same way that in the Normal errors distribution case</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x69.png" xlink:type="simple"/></inline-formula>,</p><p>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x70.png" xlink:type="simple"/></inline-formula>,</p><p>that is,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x71.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s5"><title>5. Errors with Logistic Distribution</title><p>Let us suppose that the errors follow a Logistic distribution with probability density function</p><disp-formula id="scirp.116726-formula8"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x72.png"  xlink:type="simple"/></disp-formula><p>such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x73.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x74.png" xlink:type="simple"/></inline-formula>, and, therefore, τ = 2γ.</p><p>Also, because<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x75.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x76.png" xlink:type="simple"/></inline-formula>, are independent and identically distributed random variables, it is proved in the Appendix A that the mean and the variance of these variables are 1.386γ and 1.37γ<sup>2</sup>.</p><p>So, by the Central-limit theorem</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x77.png" xlink:type="simple"/></inline-formula>.</p><p>Using the same arguments of the previous demonstrations, it follows that</p><disp-formula id="scirp.116726-formula9"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x78.png"  xlink:type="simple"/></disp-formula><p>Since in this case τ = 2γ, we have</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x79.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s6"><title>6. Errors with Laplace Distribution</title><p>When the errors follow a Laplace distribution with mean zero and variance 2σ<sup>2</sup> then</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x80.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x81.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x82.png" xlink:type="simple"/></inline-formula>.</p><p>Therefore, because of the Central-limit theorem</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x83.png" xlink:type="simple"/></inline-formula>,</p><p>and hence</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x84.png" xlink:type="simple"/></inline-formula>.</p><p>Remark: Based on the asymptotic distribution of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x85.png" xlink:type="simple"/></inline-formula>, confidence intervals for τcan be developed. In the Normal errors case, an asymptotic confidence interval for τ is</p><disp-formula id="scirp.116726-formula10"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x86.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x87.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x88.png" xlink:type="simple"/></inline-formula>and z is the percentile of order (1 + γ)/2 of the standard Normal distribution and γ is the confidence coefficient of the interval.</p><p>This confidence interval enables us to test hypothesis like H: τ = τ<sub>0</sub> at a significance level α = (1 − γ).</p></sec><sec id="s7"><title>7. Asymptotic Bias of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x89.png" xlink:type="simple"/></inline-formula></title><p>Because the sample mean of the values of the absolute residuals is a continuous and limited function, by the Helly-Bray Lemma [<xref ref-type="bibr" rid="scirp.116726-ref13">13</xref>], the expectation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x90.png" xlink:type="simple"/></inline-formula> converges to the mean of its asymptotic distribution. Therefore, it is possible to calculate the asymptotic bias of this estimator.</p><p>The analysis of the results presented in the previous section shows that the bias of this estimator is different of zero for every errors distribution considered, except the Laplace distribution.</p><p>When the errors follow the Normal (0, σ<sup>2</sup>) distribution, the asymptotic bias is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x91.png" xlink:type="simple"/></inline-formula>,</p><p>that is negative, and so, in average, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x92.png" xlink:type="simple"/></inline-formula>sub-estimates τ.</p><p>For the mixture of Normal distribution errors, the asymptotic bias is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x93.png" xlink:type="simple"/></inline-formula>,</p><p>that is negative if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x94.png" xlink:type="simple"/></inline-formula>, and is positive otherwise.</p><p>In the Logistic distribution, the asymptotic bias is given by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x95.png" xlink:type="simple"/></inline-formula>,</p><p>and so, it is always negative.</p></sec><sec id="s8"><title>8. Simulation Study</title><p>In this section, we perform a simulation study with the objective of generate empirical distributions of the estimators <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x96.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x97.png" xlink:type="simple"/></inline-formula> considering small sample sizes, under the following distributions of the errors ε<sub>i</sub>:</p><p>- Normal (0, 1) (τ = 1.253);</p><p>- Logistic with mean zero and variance π<sup>2</sup>/3 (τ = 2.00);</p><p>- Laplace with mean zero and variance 2 (τ = 1.00);</p><p>- Mixture of Normals (NM 85-15) when random variables are selected from a Normal (0, 1) with probability 0.85 and a N (0, 49) with probability 0.15 (τ = 1.439);</p><p>- Mixture of Normals (NM80-20) when random variables are selected from a Normal (0, 1) with probability 0.80 and a N (0, 49) with probability 0.20 (τ = 1.513) and</p><p>- Cauchy with median zero and scale parameter 1 (τ = 1.571).</p><p>Our objective is to find situations determined by errors distributions and sample sizes, under which <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x98.png" xlink:type="simple"/></inline-formula> has empirically a better behavior than <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x99.png" xlink:type="simple"/></inline-formula> in terms of bias and mean squared error.</p><p>The simulation study was designed as follows.</p><p>➢ We considered regression models with one independent variable generated from a Normal (0, 1) distribution, independently of the errors. Without loss of generality, the true parameters β<sub>0</sub> and β<sub>1</sub> were fixed equal to 1;</p><p>➢ The sample sizes (n) were set as 10, 20, 30, 50, 100 and 200;</p><p>➢ For each combination of sample size and errors distribution, 1000 sets of data were generated;</p><p>➢ Using the L<sub>1</sub> method, a regression model was fitted for each set of data and the values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x100.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x101.png" xlink:type="simple"/></inline-formula> were calculated. So, this procedure generated 1000 values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x102.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x103.png" xlink:type="simple"/></inline-formula>.</p><p>The computations were performed using a special routine constructed in S-Plus 4.5.</p><p>The results obtained in this study are summarized in Tables B1-B6 in Appendix B. They suggest that</p><p>➢ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x104.png" xlink:type="simple"/></inline-formula>is a good alternative to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x105.png" xlink:type="simple"/></inline-formula> when the errors follow Laplace, NM 85-15 or NM 80-20 distributions. In these cases, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x106.png" xlink:type="simple"/></inline-formula>has bias and mean squared error smaller or of the same order than<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x107.png" xlink:type="simple"/></inline-formula>;</p><p>➢ When the errors follow Normal or Logistic distribution, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x108.png" xlink:type="simple"/></inline-formula>tends to sub-estimate τ. The means of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x109.png" xlink:type="simple"/></inline-formula> distributions generated in the study are closer to the parameter value and its mean squared errors are in general uniformly smaller than that of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x110.png" xlink:type="simple"/></inline-formula>, for all considered sample sizes.</p><p>➢ For the Cauchy distribution errors, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x111.png" xlink:type="simple"/></inline-formula>tends to super-estimate τ. This result may be a consequence of the fact that all the residuals are considered in the computation of this estimator. Although <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x112.png" xlink:type="simple"/></inline-formula> has smaller bias and mean squared error than<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x113.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x114.png" xlink:type="simple"/></inline-formula>does not seem to be a good estimator of τ for sample sizes smaller or equal to 30.</p></sec><sec id="s9"><title>9. Some Characteristics of the Distributions in the Study</title><p>The distributions considered in the previous sections are symmetrical about zero and can be ordered by the weight of their tails [<xref ref-type="bibr" rid="scirp.116726-ref12">12</xref>]. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x115.png" xlink:type="simple"/></inline-formula>, an appropriate coefficient that can be used with this objective is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x116.png" xlink:type="simple"/></inline-formula>,</p><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x117.png" xlink:type="simple"/></inline-formula>,</p><p>F (x) is the distribution function of the errors and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x118.png" xlink:type="simple"/></inline-formula>is the median of the density function associated to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x119.png" xlink:type="simple"/></inline-formula>.</p><p>This coefficient has the following properties</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2"><xref ref-type="table" rid="table">Table </xref>2</xref></label><caption><title> Values of b<sub>2</sub>(α) for the distributions in the study</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Distribution</th><th align="center" valign="middle" >b<sub>2</sub>(0.10)</th><th align="center" valign="middle" >b<sub>2</sub>(0.05)</th></tr></thead><tr><td align="center" valign="middle" >Normal</td><td align="center" valign="middle" >0.2775</td><td align="center" valign="middle" >0.3551</td></tr><tr><td align="center" valign="middle" >Logistic</td><td align="center" valign="middle" >0.3455</td><td align="center" valign="middle" >0.4396</td></tr><tr><td align="center" valign="middle" >Laplace</td><td align="center" valign="middle" >0.4650</td><td align="center" valign="middle" >0.5641</td></tr><tr><td align="center" valign="middle" >NM 85-15</td><td align="center" valign="middle" >0.5618</td><td align="center" valign="middle" >0.7848</td></tr><tr><td align="center" valign="middle" >NM 80-20</td><td align="center" valign="middle" >0.6972</td><td align="center" valign="middle" >0.8076</td></tr><tr><td align="center" valign="middle" >Cauchy</td><td align="center" valign="middle" >0.7265</td><td align="center" valign="middle" >0.8541</td></tr></tbody></table></table-wrap><p>➢ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x120.png" xlink:type="simple"/></inline-formula>;</p><p>➢ Its computation does not require that the errors distribution have any finite moment;</p><p>➢ Its value is independent of the parameters of location and scale.</p><p>Large values of b<sub>2</sub>(α) indicate that the distribution has heavy tails.</p><p>In <xref ref-type="table" rid="table2"><xref ref-type="table" rid="table">Table </xref>2</xref> we present the values of b<sub>2</sub>(α) for the distributions considered in this study, taking α = 0.10 and α = 0.05. For these values of α, it is clear that the ordering of the distribution according to its tails weights is: Normal, Logistic, Laplace, NM 85-15, NM 80-20 and Cauchy.</p></sec><sec id="s10"><title>10. Concluding Remarks</title><p>In this paper, we studied the behavior of the estimator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x121.png" xlink:type="simple"/></inline-formula> with the objective of using it as an alternative to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x122.png" xlink:type="simple"/></inline-formula>. We also determined analytically its asymptotic distribution under different distributions of the errors of the model. It was observed that, in general, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x123.png" xlink:type="simple"/></inline-formula>is asymptotically biased, with asymptotic bias equal to zero when the errors follow the Laplace distribution. In this case, the absence of asymptotic bias was already expected, since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x124.png" xlink:type="simple"/></inline-formula> is the maximum likelihood estimator of τ when the errors follow the Laplace distribution.</p><p>Performing a simulation study, the two estimators were compared empirically by their bias and mean squared error, under distributions with different tails weights and considering sample sizes varying from 10 to 200. The results suggest that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x125.png" xlink:type="simple"/></inline-formula> is a good alternative to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x126.png" xlink:type="simple"/></inline-formula> when the errors in the model follow Laplace or Mixture of Normal distributions with the values of the parameters fixed in the study; when the errors have Normal or Logistic distributions (lighter tails) or Cauchy distribution (heavy tails), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x127.png" xlink:type="simple"/></inline-formula>presented the best performance for every considered sample sizes. However, in the Cauchy distribution case, although <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x128.png" xlink:type="simple"/></inline-formula> seemed to be better than<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x129.png" xlink:type="simple"/></inline-formula>, its use is not recommended in samples of size smaller or equal to 30 because of the bias of this estimator.</p><p>The results of the study indicate that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x130.png" xlink:type="simple"/></inline-formula> should be used when the distribution of the errors is close to the Laplace distribution, whatever the sample size. By the properties of this estimator mentioned in Section 1, we suggest that the fit of the data to the Laplace distribution be analyzed by the construction of a Q-Q plot of the residuals of the model. If there are not serious deviations, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x131.png" xlink:type="simple"/></inline-formula>should be used. Otherwise, Box-Cox transformations can be applied following [<xref ref-type="bibr" rid="scirp.116726-ref14">14</xref>]. After this, in the analysis of the transformed data, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x132.png" xlink:type="simple"/></inline-formula>can be used to construct confidence intervals and hypotheses tests about the parameters of the model and in the computation of robust coefficients of determination with and without a correction by the number of independent variables in the model.</p></sec><sec id="s11"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s12"><title>Cite this paper</title><p>de Andr&#233;, C.D.S. and Elian, S.N. (2022) A Comparison of the Estimators of the Scale Parameter of the Errors Distribution in the L<sub>1</sub> Regression. Open Journal of Statistics, 12, 261-276. https://doi.org/10.4236/ojs.2022.122018</p></sec><sec id="s13"><title>Appendix A. Results Used in Section 2</title><p>In Section 2, when we obtained the asymptotic distributions of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x133.png" xlink:type="simple"/></inline-formula>, the distributions of the errors were symmetrical about zero. It is easy to see that if X is a random variable with values in the interval ]−∞, ∞[, symmetric about zero and with density f(x), then the density of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x134.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.116726-formula11"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x135.png"  xlink:type="simple"/></disp-formula><p>Using this fact, we got E(|ε<sub>i</sub>|) for ε<sub>i</sub> with Normal, Mixture of Normals, Logistic or Laplace distribution.</p><p>If the errors follow a Normal distribution, that is, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x136.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x137.png" xlink:type="simple"/></inline-formula> has the density</p><disp-formula id="scirp.116726-formula12"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x138.png"  xlink:type="simple"/></disp-formula><p>and thus</p><disp-formula id="scirp.116726-formula13"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x139.png"  xlink:type="simple"/></disp-formula><p>Also, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x140.png" xlink:type="simple"/></inline-formula>, and so <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x141.png" xlink:type="simple"/></inline-formula>.</p><p>When the errors follow a mixture of Normal distribution, the probability density function of U<sub>i</sub> = |ε<sub>i</sub>| is given by</p><disp-formula id="scirp.116726-formula14"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x142.png"  xlink:type="simple"/></disp-formula><p>Therefore</p><disp-formula id="scirp.116726-formula15"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x143.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.116726-formula16"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x144.png"  xlink:type="simple"/></disp-formula><p>that is the variance of a random variable with mixture of Normal distributions with parameters p, (1 − p), means equal to zero and variances 1 and σ<sup>2</sup> respectively.</p><p>Consequently,</p><disp-formula id="scirp.116726-formula17"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x145.png"  xlink:type="simple"/></disp-formula><p>When ε<sub>i</sub> has Logistic distribution with mean zero and variance γ<sup>2</sup>π<sup>2</sup>/3.</p><disp-formula id="scirp.116726-formula18"><graphic  xlink:href="http://html.scirp.org/file/9-1241601x146.png"  xlink:type="simple"/></disp-formula><p>because<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x147.png" xlink:type="simple"/></inline-formula>.</p><p>Also<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x148.png" xlink:type="simple"/></inline-formula>, and so <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x149.png" xlink:type="simple"/></inline-formula>.</p><p>For ε<sub>i</sub> with Laplace distribution with zero mean and variance 2σ<sup>2</sup>, |ε<sub>i</sub>| has exponential distribution with mean equal to σ and variance equal to σ<sup>2</sup>. Thus, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x150.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x151.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s14"><title>Appendix B. Tables</title><table-wrap id="table3" ><label><xref ref-type="table" rid="table">Table </xref>B1</label><caption><title> Values of descriptive statistics observed in the distributions of the estimators <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x152.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x153.png" xlink:type="simple"/></inline-formula> generated in the simulation study for models with Normal (0, 1) errors (τ = 1.253) and different sample sizes</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sample size (n)</th><th align="center" valign="middle"  colspan="2"  >mean</th><th align="center" valign="middle"  colspan="2"  >median</th><th align="center" valign="middle"  colspan="2"  >mean squared error</th><th align="center" valign="middle"  colspan="2"  >minimum</th><th align="center" valign="middle"  colspan="2"  >maximum</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x154.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x155.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x156.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x157.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x158.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x159.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x160.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x161.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x162.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x163.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >1.233</td><td align="center" valign="middle" >0.675</td><td align="center" valign="middle" >1.193</td><td align="center" valign="middle" >0.661</td><td align="center" valign="middle" >0.198</td><td align="center" valign="middle" >0.366</td><td align="center" valign="middle" >0.276</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >2.893</td><td align="center" valign="middle" >1.073</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >1.316</td><td align="center" valign="middle" >0.735</td><td align="center" valign="middle" >1.289</td><td align="center" valign="middle" >0.730</td><td align="center" valign="middle" >0.149</td><td align="center" valign="middle" >0.286</td><td align="center" valign="middle" >0.175</td><td align="center" valign="middle" >0.351</td><td align="center" valign="middle" >2.681</td><td align="center" valign="middle" >1.210</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >1.252</td><td align="center" valign="middle" >0.758</td><td align="center" valign="middle" >1.216</td><td align="center" valign="middle" >0.753</td><td align="center" valign="middle" >0.109</td><td align="center" valign="middle" >0.257</td><td align="center" valign="middle" >0.368</td><td align="center" valign="middle" >0.477</td><td align="center" valign="middle" >2.404</td><td align="center" valign="middle" >1.117</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >1.138</td><td align="center" valign="middle" >0.776</td><td align="center" valign="middle" >1.123</td><td align="center" valign="middle" >0.773</td><td align="center" valign="middle" >0.097</td><td align="center" valign="middle" >0.051</td><td align="center" valign="middle" >0.447</td><td align="center" valign="middle" >0.501</td><td align="center" valign="middle" >2.250</td><td align="center" valign="middle" >1.030</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >1.164</td><td align="center" valign="middle" >0.785</td><td align="center" valign="middle" >1.158</td><td align="center" valign="middle" >0.783</td><td align="center" valign="middle" >0.069</td><td align="center" valign="middle" >0.223</td><td align="center" valign="middle" >0.415</td><td align="center" valign="middle" >0.611</td><td align="center" valign="middle" >2.014</td><td align="center" valign="middle" >0.978</td></tr><tr><td align="center" valign="middle" >150</td><td align="center" valign="middle" >1.244</td><td align="center" valign="middle" >0.790</td><td align="center" valign="middle" >1.229</td><td align="center" valign="middle" >0.790</td><td align="center" valign="middle" >0.058</td><td align="center" valign="middle" >0.217</td><td align="center" valign="middle" >0.626</td><td align="center" valign="middle" >0.646</td><td align="center" valign="middle" >2.071</td><td align="center" valign="middle" >0.951</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >1.246</td><td align="center" valign="middle" >0.788</td><td align="center" valign="middle" >1.221</td><td align="center" valign="middle" >0.786</td><td align="center" valign="middle" >0.052</td><td align="center" valign="middle" >0.218</td><td align="center" valign="middle" >0.680</td><td align="center" valign="middle" >0.635</td><td align="center" valign="middle" >2.425</td><td align="center" valign="middle" >0.933</td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table">Table </xref>B2</label><caption><title> Values of descriptive statistics observed in the distributions of the estimators <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x164.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x165.png" xlink:type="simple"/></inline-formula> generated in the simulation study for models with Logistic errors (τ = 2.00) and different sample sizes</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sample size (n)</th><th align="center" valign="middle"  colspan="2"  >mean</th><th align="center" valign="middle"  colspan="2"  >median</th><th align="center" valign="middle"  colspan="2"  >mean squared error</th><th align="center" valign="middle"  colspan="2"  >minimum</th><th align="center" valign="middle"  colspan="2"  >maximum</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x166.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x167.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x168.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x169.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x170.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x171.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x172.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x173.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x174.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x175.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2.120</td><td align="center" valign="middle" >1.189</td><td align="center" valign="middle" >2.019</td><td align="center" valign="middle" >1.165</td><td align="center" valign="middle" >0.722</td><td align="center" valign="middle" >0.784</td><td align="center" valign="middle" >0.253</td><td align="center" valign="middle" >0.386</td><td align="center" valign="middle" >5.459</td><td align="center" valign="middle" >2.675</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >2.206</td><td align="center" valign="middle" >1.281</td><td align="center" valign="middle" >2.146</td><td align="center" valign="middle" >1.263</td><td align="center" valign="middle" >0.500</td><td align="center" valign="middle" >0.580</td><td align="center" valign="middle" >0.624</td><td align="center" valign="middle" >0.597</td><td align="center" valign="middle" >4.950</td><td align="center" valign="middle" >2.146</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >2.039</td><td align="center" valign="middle" >1.311</td><td align="center" valign="middle" >1.990</td><td align="center" valign="middle" >1.297</td><td align="center" valign="middle" >0.290</td><td align="center" valign="middle" >0.519</td><td align="center" valign="middle" >0.256</td><td align="center" valign="middle" >0.746</td><td align="center" valign="middle" >4.144</td><td align="center" valign="middle" >2.195</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >1.814</td><td align="center" valign="middle" >1.352</td><td align="center" valign="middle" >1.797</td><td align="center" valign="middle" >1.340</td><td align="center" valign="middle" >0.270</td><td align="center" valign="middle" >0.446</td><td align="center" valign="middle" >0.619</td><td align="center" valign="middle" >0.900</td><td align="center" valign="middle" >3.462</td><td align="center" valign="middle" >1.910</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >1.866</td><td align="center" valign="middle" >1.363</td><td align="center" valign="middle" >1.831</td><td align="center" valign="middle" >1.357</td><td align="center" valign="middle" >0.183</td><td align="center" valign="middle" >0.420</td><td align="center" valign="middle" >0.779</td><td align="center" valign="middle" >0.986</td><td align="center" valign="middle" >3.383</td><td align="center" valign="middle" >1.742</td></tr><tr><td align="center" valign="middle" >150</td><td align="center" valign="middle" >2.004</td><td align="center" valign="middle" >1.372</td><td align="center" valign="middle" >1.987</td><td align="center" valign="middle" >1.379</td><td align="center" valign="middle" >0.141</td><td align="center" valign="middle" >0.403</td><td align="center" valign="middle" >1.030</td><td align="center" valign="middle" >1.078</td><td align="center" valign="middle" >3.190</td><td align="center" valign="middle" >1.654</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >2.035</td><td align="center" valign="middle" >1.380</td><td align="center" valign="middle" >2.017</td><td align="center" valign="middle" >1.376</td><td align="center" valign="middle" >0.128</td><td align="center" valign="middle" >0.391</td><td align="center" valign="middle" >1.070</td><td align="center" valign="middle" >1.155</td><td align="center" valign="middle" >3.264</td><td align="center" valign="middle" >1.668</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table">Table </xref>B3</label><caption><title> Values of descriptive statistics observed in the distributions of the estimators <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x176.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x177.png" xlink:type="simple"/></inline-formula> generated in the simulation study for models with Laplace errors (τ = 1.00) and different sample sizes</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sample size (n)</th><th align="center" valign="middle"  colspan="2"  >mean</th><th align="center" valign="middle"  colspan="2"  >median</th><th align="center" valign="middle"  colspan="2"  >mean squared error</th><th align="center" valign="middle"  colspan="2"  >minimum</th><th align="center" valign="middle"  colspan="2"  >Maximum</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x178.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x179.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x180.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x181.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x182.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x183.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x184.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x185.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x186.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x187.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >1.461</td><td align="center" valign="middle" >0.872</td><td align="center" valign="middle" >1.368</td><td align="center" valign="middle" >0.843</td><td align="center" valign="middle" >0.705</td><td align="center" valign="middle" >0.112</td><td align="center" valign="middle" >0.162</td><td align="center" valign="middle" >0.238</td><td align="center" valign="middle" >4.413</td><td align="center" valign="middle" >2.207</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >1.442</td><td align="center" valign="middle" >0.936</td><td align="center" valign="middle" >1.401</td><td align="center" valign="middle" >0.917</td><td align="center" valign="middle" >0.443</td><td align="center" valign="middle" >0.052</td><td align="center" valign="middle" >0.373</td><td align="center" valign="middle" >0.482</td><td align="center" valign="middle" >3.479</td><td align="center" valign="middle" >1.942</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >1.314</td><td align="center" valign="middle" >0.975</td><td align="center" valign="middle" >1.263</td><td align="center" valign="middle" >0.960</td><td align="center" valign="middle" >0.261</td><td align="center" valign="middle" >0.034</td><td align="center" valign="middle" >0.462</td><td align="center" valign="middle" >0.481</td><td align="center" valign="middle" >3.105</td><td align="center" valign="middle" >1.621</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >1.072</td><td align="center" valign="middle" >0.979</td><td align="center" valign="middle" >1.042</td><td align="center" valign="middle" >0.974</td><td align="center" valign="middle" >0.100</td><td align="center" valign="middle" >0.021</td><td align="center" valign="middle" >0.382</td><td align="center" valign="middle" >0.616</td><td align="center" valign="middle" >2.351</td><td align="center" valign="middle" >1.453</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >1.076</td><td align="center" valign="middle" >0.996</td><td align="center" valign="middle" >1.058</td><td align="center" valign="middle" >0.992</td><td align="center" valign="middle" >0.068</td><td align="center" valign="middle" >0.009</td><td align="center" valign="middle" >0.403</td><td align="center" valign="middle" >0.711</td><td align="center" valign="middle" >2.025</td><td align="center" valign="middle" >1.393</td></tr><tr><td align="center" valign="middle" >150</td><td align="center" valign="middle" >1.118</td><td align="center" valign="middle" >0.991</td><td align="center" valign="middle" >1.106</td><td align="center" valign="middle" >0.989</td><td align="center" valign="middle" >0.065</td><td align="center" valign="middle" >0.007</td><td align="center" valign="middle" >0.555</td><td align="center" valign="middle" >0.767</td><td align="center" valign="middle" >1.993</td><td align="center" valign="middle" >1.263</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >1.099</td><td align="center" valign="middle" >0.993</td><td align="center" valign="middle" >1.093</td><td align="center" valign="middle" >0.992</td><td align="center" valign="middle" >0.053</td><td align="center" valign="middle" >0.005</td><td align="center" valign="middle" >0.557</td><td align="center" valign="middle" >0.788</td><td align="center" valign="middle" >1.942</td><td align="center" valign="middle" >1.223</td></tr></tbody></table></table-wrap><table-wrap id="table6" ><label><xref ref-type="table" rid="table">Table </xref>B4</label><caption><title> Values of descriptive statistics observed in the distributions of the estimators <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x188.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x188.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x189.png" xlink:type="simple"/></inline-formula> generated in the simulation study for models with 0.85 Normal (0, 1) + 0.15 Normal (0, 49) errors (τ = 1.439) and different sample sizes</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sample size (n)</th><th align="center" valign="middle"  colspan="2"  >mean</th><th align="center" valign="middle"  colspan="2"  >median</th><th align="center" valign="middle"  colspan="2"  >mean squared error</th><th align="center" valign="middle"  colspan="2"  >minimum</th><th align="center" valign="middle"  colspan="2"  >Maximum</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x190.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x191.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x192.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x193.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x194.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x195.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x196.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x197.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x198.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x199.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >1.871</td><td align="center" valign="middle" >1.340</td><td align="center" valign="middle" >1.550</td><td align="center" valign="middle" >1.152</td><td align="center" valign="middle" >1.884</td><td align="center" valign="middle" >0.568</td><td align="center" valign="middle" >0.232</td><td align="center" valign="middle" >0.293</td><td align="center" valign="middle" >9.958</td><td align="center" valign="middle" >6.001</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >1.640</td><td align="center" valign="middle" >1.468</td><td align="center" valign="middle" >1.560</td><td align="center" valign="middle" >1.387</td><td align="center" valign="middle" >0.393</td><td align="center" valign="middle" >0.293</td><td align="center" valign="middle" >0.425</td><td align="center" valign="middle" >0.351</td><td align="center" valign="middle" >8.533</td><td align="center" valign="middle" >3.838</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >1.518</td><td align="center" valign="middle" >1.498</td><td align="center" valign="middle" >1.501</td><td align="center" valign="middle" >1.443</td><td align="center" valign="middle" >0.192</td><td align="center" valign="middle" >0.206</td><td align="center" valign="middle" >0.530</td><td align="center" valign="middle" >0.475</td><td align="center" valign="middle" >3.465</td><td align="center" valign="middle" >3.394</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >1.325</td><td align="center" valign="middle" >1.484</td><td align="center" valign="middle" >1.282</td><td align="center" valign="middle" >1.455</td><td align="center" valign="middle" >0.144</td><td align="center" valign="middle" >0.121</td><td align="center" valign="middle" >0.314</td><td align="center" valign="middle" >0.636</td><td align="center" valign="middle" >2.696</td><td align="center" valign="middle" >2.935</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >1.338</td><td align="center" valign="middle" >1.490</td><td align="center" valign="middle" >1.313</td><td align="center" valign="middle" >1.479</td><td align="center" valign="middle" >0.104</td><td align="center" valign="middle" >0.058</td><td align="center" valign="middle" >0.561</td><td align="center" valign="middle" >0.883</td><td align="center" valign="middle" >2.501</td><td align="center" valign="middle" >2.334</td></tr><tr><td align="center" valign="middle" >150</td><td align="center" valign="middle" >1.450</td><td align="center" valign="middle" >1.500</td><td align="center" valign="middle" >1.435</td><td align="center" valign="middle" >1.493</td><td align="center" valign="middle" >0.072</td><td align="center" valign="middle" >0.043</td><td align="center" valign="middle" >0.721</td><td align="center" valign="middle" >0.942</td><td align="center" valign="middle" >2.558</td><td align="center" valign="middle" >2.120</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >1.451</td><td align="center" valign="middle" >1.502</td><td align="center" valign="middle" >1.441</td><td align="center" valign="middle" >1.500</td><td align="center" valign="middle" >0.067</td><td align="center" valign="middle" >0.031</td><td align="center" valign="middle" >0.706</td><td align="center" valign="middle" >0.975</td><td align="center" valign="middle" >2.432</td><td align="center" valign="middle" >2.053</td></tr></tbody></table></table-wrap><table-wrap id="table7" ><label><xref ref-type="table" rid="table">Table </xref>B5</label><caption><title> Values of descriptive statistics observed in the distributions of the estimators <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x200.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x201.png" xlink:type="simple"/></inline-formula> generated in the simulation study for models with 0.80 Normal (0, 1) + 0.20 Normal (0, 49) errors (τ = 1.513) and different sample sizes</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sample size (n)</th><th align="center" valign="middle"  colspan="2"  >mean</th><th align="center" valign="middle"  colspan="2"  >median</th><th align="center" valign="middle"  colspan="2"  >mean squared error</th><th align="center" valign="middle"  colspan="2"  >minimum</th><th align="center" valign="middle"  colspan="2"  >Maximum</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x202.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x203.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x204.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x205.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x206.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x207.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x208.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x209.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x210.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x211.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2.182</td><td align="center" valign="middle" >1.624</td><td align="center" valign="middle" >1.716</td><td align="center" valign="middle" >1.414</td><td align="center" valign="middle" >2.933</td><td align="center" valign="middle" >0.638</td><td align="center" valign="middle" >0.259</td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >12.500</td><td align="center" valign="middle" >5.204</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >1.808</td><td align="center" valign="middle" >1.690</td><td align="center" valign="middle" >1.677</td><td align="center" valign="middle" >1.626</td><td align="center" valign="middle" >0.684</td><td align="center" valign="middle" >0.427</td><td align="center" valign="middle" >0.393</td><td align="center" valign="middle" >0.541</td><td align="center" valign="middle" >9.292</td><td align="center" valign="middle" >4.419</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >1.610</td><td align="center" valign="middle" >1.498</td><td align="center" valign="middle" >1.558</td><td align="center" valign="middle" >1.498</td><td align="center" valign="middle" >0.221</td><td align="center" valign="middle" >0.270</td><td align="center" valign="middle" >0.606</td><td align="center" valign="middle" >0.475</td><td align="center" valign="middle" >4.200</td><td align="center" valign="middle" >3.394</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >1.410</td><td align="center" valign="middle" >1.727</td><td align="center" valign="middle" >1.399</td><td align="center" valign="middle" >1.697</td><td align="center" valign="middle" >0.153</td><td align="center" valign="middle" >0.193</td><td align="center" valign="middle" >0.480</td><td align="center" valign="middle" >0.803</td><td align="center" valign="middle" >2.883</td><td align="center" valign="middle" >3.244</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >1.405</td><td align="center" valign="middle" >1.739</td><td align="center" valign="middle" >1.367</td><td align="center" valign="middle" >1.719</td><td align="center" valign="middle" >0.111</td><td align="center" valign="middle" >0.126</td><td align="center" valign="middle" >0.671</td><td align="center" valign="middle" >1.069</td><td align="center" valign="middle" >2.738</td><td align="center" valign="middle" >2.830</td></tr><tr><td align="center" valign="middle" >150</td><td align="center" valign="middle" >1.519</td><td align="center" valign="middle" >1.737</td><td align="center" valign="middle" >1.499</td><td align="center" valign="middle" >1.729</td><td align="center" valign="middle" >0.083</td><td align="center" valign="middle" >0.098</td><td align="center" valign="middle" >0.759</td><td align="center" valign="middle" >1.146</td><td align="center" valign="middle" >2.488</td><td align="center" valign="middle" >2.617</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >1.523</td><td align="center" valign="middle" >1.745</td><td align="center" valign="middle" >1.511</td><td align="center" valign="middle" >1.740</td><td align="center" valign="middle" >0.075</td><td align="center" valign="middle" >0.092</td><td align="center" valign="middle" >0.784</td><td align="center" valign="middle" >1.212</td><td align="center" valign="middle" >2.383</td><td align="center" valign="middle" >2.480</td></tr></tbody></table></table-wrap><table-wrap id="table8" ><label><xref ref-type="table" rid="table">Table </xref>B6</label><caption><title> Values of descriptive statistics observed in the distributions of the estimators <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x212.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x213.png" xlink:type="simple"/></inline-formula> generated in the simulation study for models with Cauchy errors (τ = 1.571) and different sample sizes</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Sample size (n)</th><th align="center" valign="middle"  colspan="2"  >mean</th><th align="center" valign="middle"  colspan="2"  >median</th><th align="center" valign="middle"  colspan="2"  >mean squared error</th><th align="center" valign="middle"  colspan="2"  >minimum</th><th align="center" valign="middle"  colspan="2"  >maximum</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x214.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x215.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x216.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x217.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x218.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x219.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x220.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x221.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x222.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-1241601x223.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >3.480</td><td align="center" valign="middle" >7.390</td><td align="center" valign="middle" >2.458</td><td align="center" valign="middle" >2.070</td><td align="center" valign="middle" >20.150</td><td align="center" valign="middle" >2594.0</td><td align="center" valign="middle" >0.294</td><td align="center" valign="middle" >0.340</td><td align="center" valign="middle" >48.505</td><td align="center" valign="middle" >1203.7</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >2.375</td><td align="center" valign="middle" >22.800</td><td align="center" valign="middle" >2.147</td><td align="center" valign="middle" >2.800</td><td align="center" valign="middle" >1.794</td><td align="center" valign="middle" >182089.0</td><td align="center" valign="middle" >0.483</td><td align="center" valign="middle" >0.400</td><td align="center" valign="middle" >8.343</td><td align="center" valign="middle" >13019.1</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >1.931</td><td align="center" valign="middle" >14.740</td><td align="center" valign="middle" >1.863</td><td align="center" valign="middle" >3.010</td><td align="center" valign="middle" >0.587</td><td align="center" valign="middle" >51611.0</td><td align="center" valign="middle" >0.533</td><td align="center" valign="middle" >0.740</td><td align="center" valign="middle" >5.191</td><td align="center" valign="middle" >7064.1</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >1.578</td><td align="center" valign="middle" >6.902</td><td align="center" valign="middle" >1.543</td><td align="center" valign="middle" >3.608</td><td align="center" valign="middle" >0.168</td><td align="center" valign="middle" >348.0</td><td align="center" valign="middle" >0.533</td><td align="center" valign="middle" >0.941</td><td align="center" valign="middle" >3.920</td><td align="center" valign="middle" >285.1</td></tr><tr><td align="center" valign="middle" >100</td><td align="center" valign="middle" >1.530</td><td align="center" valign="middle" >41.700</td><td align="center" valign="middle" >1.509</td><td align="center" valign="middle" >3.700</td><td align="center" valign="middle" >0.117</td><td align="center" valign="middle" >1281096.0</td><td align="center" valign="middle" >0.684</td><td align="center" valign="middle" >1.500</td><td align="center" valign="middle" >2.790</td><td align="center" valign="middle" >35792.4</td></tr><tr><td align="center" valign="middle" >150</td><td align="center" valign="middle" >1.629</td><td align="center" valign="middle" >7.866</td><td align="center" valign="middle" >1.620</td><td align="center" valign="middle" >3.955</td><td align="center" valign="middle" >0.097</td><td align="center" valign="middle" >581.0</td><td align="center" valign="middle" >0.816</td><td align="center" valign="middle" >1.689</td><td align="center" valign="middle" >2.782</td><td align="center" valign="middle" >488.8</td></tr><tr><td align="center" valign="middle" >200</td><td align="center" valign="middle" >1.615</td><td align="center" valign="middle" >7.747</td><td align="center" valign="middle" >1.603</td><td align="center" valign="middle" >4.205</td><td align="center" valign="middle" >0.086</td><td align="center" valign="middle" >375.0</td><td align="center" valign="middle" >0.819</td><td align="center" 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