<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2016.715143</article-id><article-id pub-id-type="publisher-id">AM-70513</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>
 
 
  On Data-Independent Properties for Density-Based Dissimilarity Measures in Hybrid Clustering
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Kajsa</surname><given-names>Møllersen</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>Subhra</surname><given-names>S. Dhar</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fred</surname><given-names>Godtliebsen</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Norwegian Centre for Integrated Care and Telemedicine, University Hospital of North Norway, Troms&amp;amp;Oslash;, Norway</addr-line></aff><aff id="aff2"><addr-line>Department of Mathematics and Statistics, IIT Kanpur, Uttar Pradesh, India</addr-line></aff><aff id="aff3"><addr-line>Department of Mathematics and Statistics, UiT The Arctic University of Norway, Troms&amp;amp;Oslash;, Norway</addr-line></aff><pub-date pub-type="epub"><day>12</day><month>09</month><year>2016</year></pub-date><volume>07</volume><issue>15</issue><fpage>1674</fpage><lpage>1706</lpage><history><date date-type="received"><day>March</day>	<month>11,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>September</month>	<year>9,</year>	</date><date date-type="accepted"><day>September</day>	<month>12,</month>	<year>2016</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>
 
 
  Hybrid clustering combines partitional and hierarchical clustering for computational effectiveness and versatility in cluster shape. In such clustering, a dissimilarity measure plays a crucial role in the hierarchical merging. The dissimilarity measure has great impact on the final clustering, and data-independent properties are needed to choose the right dissimilarity measure for the problem at hand. Properties for distance-based dissimilarity measures have been studied for decades, but properties for density-based dissimilarity measures have so far received little attention. Here, we propose six data-independent properties to evaluate density-based dissimilarity measures associated with hybrid clustering, regarding equality, orthogonality, symmetry, outlier and noise observations, and light-tailed models for heavy-tailed clusters. The significance of the properties is investigated, and we study some well-known dissimilarity measures based on Shannon entropy, misclassification rate, Bhattacharyya distance and Kullback-Leibler divergence with respect to the proposed properties. As none of them satisfy all the proposed properties, we introduce a new dissimilarity measure based on the Kullback-Leibler information and show that it satisfies all proposed properties. The effect of the proposed properties is also illustrated on several real and simulated data sets.
 
</p></abstract><kwd-group><kwd>Background Noise</kwd><kwd> Gaussian Mixture Distribution</kwd><kwd> Kullback-Leibler</kwd><kwd> Outliers</kwd><kwd> Subcluster Weight</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Clustering or cluster analysis is a well-known unsupervised statistical learning tech- nique, which describes the formation of groups in a data set based on the relation between the observations. The common understanding of a cluster is that the observa- tions within the cluster are more closely related to each other than to the observations in another cluster. The definition of closely related observations depends both on the problem at hand and the user’s understanding of the cluster concept, and hence there exists a wide range of clustering techniques. <xref ref-type="fig" rid="fig1">Figure 1</xref> shows one way of categorising clustering techniques, which will be helpful for the understanding of hybrid clustering and dissimilarity measures. At the top level, clustering techniques are divided into partitional and hierarchical clustering. Partitional clustering provides a single partition of the data, whereas hierarchical clustering provides a nested series of partitions. At each step in a hierarchical clustering, either two subclusters are merged (agglomerative clustering) or one subcluster is divided into two subclusters (divisive clustering). A dissimilarity measure defines which two subclusters will be merged at each step in agglomerative clustering, and might be based on a probability density function or a proper distance function. Several other categorisations of clustering techniques exist; for a comprehensive overview, we refer the readers to [<xref ref-type="bibr" rid="scirp.70513-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.70513-ref3">3</xref>] .</p><p>Hybrid clustering combines partitional and hierarchical clustering to overcome the shortcomings of each separate technique. Model-based partitional clusterings, like Gaussian mixture model (GMM) and k-means [<xref ref-type="bibr" rid="scirp.70513-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref5">5</xref>] , impose shape restrictions on the clusters [<xref ref-type="bibr" rid="scirp.70513-ref6">6</xref>] , which are a drawback if the model does not fit the data well. Model-free partitional clusterings are more versatile, but for high-dimensional data, sparsity makes low- and high-density regions difficult to distinguish. On the other hand, the hier- archical clustering technique does not impose restrictions on the cluster shape, but it has extensive computational complexity. Hybrid clustering takes advantage of the versatility of hierarchical clustering, but avoids the computational costs, and can be described as follows: Initially, a partitional clustering defines K subclusters. These are then merged hierarchically into C final clusters. Hybrid clustering and its related issues have been studied for decades; see e.g. [<xref ref-type="bibr" rid="scirp.70513-ref6">6</xref>] - [<xref ref-type="bibr" rid="scirp.70513-ref15">15</xref>] .</p><p>To illustrate how different clustering techniques give us different outcomes, let us consider the well-known Old Faithful Geyser data, which is available in R. The data set consists of the length of 272 eruptions, and eruption length versus previous eruption length is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(a). The observations are clearly clustered, and the objective</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> A partial taxonomy of clustering techniques</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x2.png"/></fig><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Eruption length versus previous eruption length of the Old Faithful Geyser. (a) The gap-statistic estimates three clusters, whereas ICL estimates four (see Section 2.2); (b) Data labelled according to MAP for a four-component GMM fitted to the data. The number of components was estimated by BIC (see Section 2.1).</title></caption><fig id ="fig2_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x3.png"/></fig></fig-group><p>of a clustering technique is to identify the clusters. The actual number of clusters is unknown, and it has served as an illustrative example for a number of techniques. It illustrates the clustering concept through a set of observations where some are more closely related than others, but also the inherit subjectivity since not all observations have a clear cluster membership, and the number of clusters depends on the user’s subjective understanding. Clustering includes both assigning the observations to a specific cluster and estimating the number of clusters. Depending on the observer’s subjective understanding, there are either three or four clusters in <xref ref-type="fig" rid="fig2">Figure 2</xref>(a), and different cluster number estimation techniques give different results. For a discussion on three versus four clusters for this particular data set, see [<xref ref-type="bibr" rid="scirp.70513-ref16">16</xref>] . <xref ref-type="fig" rid="fig2">Figure 2</xref>(b) shows an example of a clustering result where the Bayesian information criterion (BIC) was used to estimate the number of clusters, and the observations have been clustered using GMM and labelled according to the maximum a posteriori probability (MAP). Alterna- tively, the gap statistic (see Section 2.2) can be used to estimate the number of clusters, which resulted in three clusters. The partitional clustering in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b) can then be regarded as the initial step in a hybrid clustering, where BIC was used to estimate the number of subclusters K. The next and final step will then be to merge two of the subclusters to reach the number of final clusters,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x4.png" xlink:type="simple"/></inline-formula>. It turns out that the choice of dissimilarity measure has significant impact on the final result of hybrid clustering. The well-known distance-based dissimilarity measures, single-link, complete-link and average-link merge blue-green coloured, blue-red coloured and blue-green coloured observations, respectively. On the other hand, the measures SE (see Section 3.3) and Bhat (see Section 3.3), both density-based, merge blue-green coloured and blue-red coloured observations, respectively. There is no definition of “true” clusters, but some results are more agreeable with the cluster concept. The results when using single-link, average-link or SE as dissimilarity measure, have, to our knowledge, not been proposed for this well-known data-set.</p><p>In the above example, the choice of dissimilarity measure can be done based on whether the result agrees with the user’s own perception. However, when the dimen- sion is larger than three, the user cannot check the clustering result by visual inspection. If the user already has a clear opinion on how the data should be clustered, a clustering technique is not needed. For other situations, when clustering is used to explore the data, to discover patterns or as a pre-processing for other tasks, the clustering result must be interpreted in view of the method used. The result can be interpreted in view of how the chosen dissimilarity measure behaves under various circumstances, or vice- versa; the dissimilarity measure can be chosen based on pre-defined requests. Since the same dataset can lead to very different clustering results, as illustrated in the above example, the clustering result itself says very little about the data unless some analysis of the method is included.</p><p>In the present work, we have investigated one crucial aspect of clustering; the choice of dissimilarity measure. The investigation is restricted to density-based measures, and is exemplified on the partitional-hierarchical hybrid clustering technique. At first, we have identified a set of properties that are relevant for density-based dissimilarity measures in the hybrid clustering context (see Section 3.2). The properties have been identified by observing known dissimilarity measures’ behaviour under circumstances that are likely to occur in the hybrid clustering context. Further, we have analysed a set of known dissimilarity measures in view of these properties, and none of them fulfil all. Furthermore, we propose a new density-based dissimilarity measure that fulfils all the proposed properties. The new measure is constructed to be robust to background noise, a property that none of the other dissimilarity measures fulfil.</p><p>The performance of a dissimilarity measure on a specific data set does not imply that it will perform equally good or bad on another data set. Data-independent properties to evaluate dissimilarity measures enable us to choose a dissimilarity measure based on the user’s understanding of the cluster concept for a given problem without extra knowledge about the data set. For instance, whether a small subcluster, such as the red observations in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b), should be considered a proper cluster or the effect of noise observations can be known beforehand, regardless of the actual data. The preferred concepts may differ, and data-independent properties will serve to categorise the dis- similarity measures. Properties for distance-based dissimilarity measures have been discussed for decades [<xref ref-type="bibr" rid="scirp.70513-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref17">17</xref>] - [<xref ref-type="bibr" rid="scirp.70513-ref20">20</xref>] . To our best knowledge, there has been no attempt in investigating data-independent properties for density-based dissimilarity measures, except in the context of image analysis [<xref ref-type="bibr" rid="scirp.70513-ref21">21</xref>] . However, many density-based dissimilarity measures originate from divergence functions, which possess certain pro- perties (see Section 3.1). In this article, we propose additional properties regarding clustering-specific problems related to small outlying subclusters, low-density sub- clusters associated with background noise, and light-tailed models for heavy-tailed data (see Section 3.2). We would like to point out that this is not an attempt to describe the best dissimilarity measure, but rather to provide a tool for evaluation and catego- risation depending upon prior knowledge on the data and the user’s understanding regarding the clustering concept. In addition, several density-based dissimilarity measures have been proposed for hybrid clustering, and since none of them satisfy all the proposed properties, we propose a new one that does.</p><p>The rest of the article is organised as follows. Hybrid clustering is discussed in Section 2. Section 3 introduces the f-divergences and proposes a set of properties for dissimilarity measures. Section 3.3 investigates well-known dissimilarity measures and proposes a new dissimilarity measure. Section 4 illustrates the dissimilarity measures’ impact on the final clustering based on different simulated and real data. Some concluding remarks are mentioned in Section 5. The appendices provide the necessary technical details.</p></sec><sec id="s2"><title>2. Hybrid Clustering Techniques</title><p>As discussed in the Introduction, hybrid clustering seeks to take advantage of the versatility of hierarchical clustering, but at the same time avoid the computational complexity. Hybrid clustering can be summarised in three steps:</p><p>1) Partition the data into K subclusters by partitional clustering.</p><p>2) Hierarchically merge the two subclusters with lowest dissimilarity.</p><p>3) Repeat the merging until some stopping rule applies.</p><p>Let K denote the number of initial partitions, N denote the number of observations, and C denote the number of final clusters. When K is close to N, the shape restrictions of the initial partitioning technique does not have significant impact on the final result. On the other hand, when K is close to C, the computational complexity will be optimised, and hence, there is a trade-off between versatility and computational com- plexity. For a more thorough discussion on the computational complexity of partitional, hierarchical and hybrid clustering, see [<xref ref-type="bibr" rid="scirp.70513-ref15">15</xref>] . The subsequent subsections discuss each of the three steps.</p><sec id="s2_1"><title>2.1. Partitional Clustering</title><p>Various techniques have been used for initial partitioning, among them the well-known k-means [<xref ref-type="bibr" rid="scirp.70513-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref8">8</xref>] - [<xref ref-type="bibr" rid="scirp.70513-ref10">10</xref>] , and GMM [<xref ref-type="bibr" rid="scirp.70513-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref22">22</xref>] . For other examples, see [<xref ref-type="bibr" rid="scirp.70513-ref11">11</xref>] - [<xref ref-type="bibr" rid="scirp.70513-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref23">23</xref>] . A brief description of the GMM is as follows.</p><p>Any continuous distribution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x5.png" xlink:type="simple"/></inline-formula> can be approximated with arbitrary accuracy by a mixture of Gaussian distributions [<xref ref-type="bibr" rid="scirp.70513-ref24">24</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref25">25</xref>] :</p><disp-formula id="scirp.70513-formula393"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x6.png"  xlink:type="simple"/></disp-formula><p>Here, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x7.png" xlink:type="simple"/></inline-formula>is the a priori probability associated with the i-th class, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x8.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x9.png" xlink:type="simple"/></inline-formula> are the location and the scale parameters of the Gaussian distribution of the i-th component. When the underlying distribution is unknown, the GMM is fitted to the observed values, most commonly by the EM algorithm [<xref ref-type="bibr" rid="scirp.70513-ref26">26</xref>] , and the accuracy will depend on how the observations were generated from the parent distribution. The number of components must be estimated separately, with a trade-off between good fit and model complexity. A common procedure is to fit several GMMs, having <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x10.png" xlink:type="simple"/></inline-formula> components, and then use a criterion like BIC [<xref ref-type="bibr" rid="scirp.70513-ref27">27</xref>] or the Akaike infor- mation criterion (AIC) [<xref ref-type="bibr" rid="scirp.70513-ref28">28</xref>] to select the number of components. For other criteria and a discussion, the reader is referred to [<xref ref-type="bibr" rid="scirp.70513-ref29">29</xref>] , p. 175.</p><p>For any choice of dissimilarity measure, the final clustering depends on the par- titional clustering technique through the initial subclusters’ purity. In a totally pure subcluster, all observations belong to the same “true’’ cluster, but frequently one or more subclusters will contain observations from at least two different “true’’ clusters. The final clustering will therefore rely on the purity of the partitional clustering. We illustrate this on the Yeast data from the UCI machine learning repository [<xref ref-type="bibr" rid="scirp.70513-ref30">30</xref>] . Franczak et al. chose three variables (McGeoch’s method for signal sequence re- cognition (mcg), the score of the ALOM membrane spanning region prediction pro- gram (alm), and the score of discriminant analysis of the amino acid content of vacuolar and extracellular proteins (vac)), and two classes (localisation sites CYT (cytosolic or cytoskeletal) and ME3 (membrane protein, no N-terminal signal)) to illustrate Laplace clustering [<xref ref-type="bibr" rid="scirp.70513-ref31">31</xref>] . <xref ref-type="fig" rid="fig3">Figure 3</xref>(a) shows the observations labelled according to class.</p><p>We use GMM and BIC for partitional clustering, and the observations are assigned to a subcluster according to MAP. The result can be seen in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) where the subcluster shown as yellow crosses contains observations from both classes. <xref ref-type="fig" rid="fig3">Figure 3</xref>(c) shows the partitional clustering when using Student’s t mixture distribution instead of GMM, and we see that the subclusters are purer. To be able to separate the impact of the dissimilarity measure from that of the partitional clustering technique (see Section 4) we define minimum misclassification rate as the minimum proportion of observa- tions assigned to the wrong cluster when all possible final clusterings are considered. The minimum misclassification rates in this example are 7.8% for GMM and 3.4% for Student’s t. The superior performance of Student’s t in this example was expected, since Student’s t mixture distributions are more robust to heavy tails than GMMs [<xref ref-type="bibr" rid="scirp.70513-ref32">32</xref>] . In general, the best partitional clustering technique will depend on the problem at hand.</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Yeast data. (a) The true labelling; (b) Five-component GMM fit; and (c) Three-component Student’s t mixture fit.</title></caption><fig id ="fig3_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x11.png"/></fig></fig-group></sec><sec id="s2_2"><title>2.2. Dissimilarity Measure and Stopping Rule</title><p>Dissimilarity measures for hybrid clustering can be based on distance functions (for example, [<xref ref-type="bibr" rid="scirp.70513-ref12">12</xref>] ) or density functions (for example, [<xref ref-type="bibr" rid="scirp.70513-ref8">8</xref>] ). The dissimilarity measure will be involved in each step in the hierarchical merging, and therefore, the choice of dissimilarity measure might have significant impact on the final outcome, as discussed in the Introduction. Density-based dissimilarity measures are functions of the sub- clusters’ density and size (also referred to as weight), estimated from the data. If the partitional clustering is done by mixture distribution fitting, the components’ pro- bability density function (pdf) and a priori probability of the class represent the sub- clusters’ density and weight, and the dissimilarity measure is a function of the observa- tions indirectly through the estimated mixture distribution.</p><p>The number of clusters can be estimated from the data using, for example, the gap statistic [<xref ref-type="bibr" rid="scirp.70513-ref33">33</xref>] or integrated completed likelihood (ICL) [<xref ref-type="bibr" rid="scirp.70513-ref34">34</xref>] . For demonstration, an example is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>(a). The dissimilarity measure can define the stopping rule by setting a threshold value at which the merging process will stop. This threshold can be pre-defined by the user, or defined by analysing the dissimilarity as a function of the number of subclusters, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x12.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.70513-ref33">33</xref>] , see <xref ref-type="fig" rid="fig1">Figure 1</xref>1. The number of clusters can also be chosen by the user based on prior knowledge about the data. To gain insight about different stopping rules, the reader may read [<xref ref-type="bibr" rid="scirp.70513-ref19">19</xref>] .</p></sec></sec><sec id="s3"><title>3. Data-Independent Properties for Density-Based Dissimilarity Measures</title><p>The divergence between two probability distributions essentially measures the distance between them, and hence there is a close relationship between density-based dis- similarity measures and divergences. There have been many attempts to define the distance between two probability distributions, and the concept is context dependent and subjective like clustering. Note that many divergences do not satisfy symmetry or triangular inequality, and are therefore not proper distances. Ali and Silvey [<xref ref-type="bibr" rid="scirp.70513-ref35">35</xref>] defined four properties for divergences, and through them defined the class of f-divergences. The f-divergences are of special interest due to their properties and since they have been used directly or in modified form as dissimilarity measures for hybrid clustering [<xref ref-type="bibr" rid="scirp.70513-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref36">36</xref>] . Many well-known distance functions or information criteria are f-diver- gences, for example, variational distance, Hellinger/Kolmogorov distance, Kullback- Leibler information, Kullback-Leibler/Jeffrey divergence, Chernoff distance, Bhatta- charyya distance, Matusita distance [<xref ref-type="bibr" rid="scirp.70513-ref35">35</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref37">37</xref>] - [<xref ref-type="bibr" rid="scirp.70513-ref39">39</xref>] , and therefore automatically satisfy the properties.</p><p>Dissimilarity measures used as merging criteria attempt to measure the distance between two subclusters with respect to which two subclusters are most appropriate to merge. We therefore introduce properties specifically for dissimilarity measures which offer the user a data-independent tool for choosing, evaluating or modifying dis- similarity measures.</p><sec id="s3_1"><title>3.1. Properties for f-Divergences</title><p>The f-divergences, introduced independently in [<xref ref-type="bibr" rid="scirp.70513-ref38">38</xref>] and in [<xref ref-type="bibr" rid="scirp.70513-ref35">35</xref>] , are defined as follows [<xref ref-type="bibr" rid="scirp.70513-ref39">39</xref>] .</p><p>Definition: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x13.png" xlink:type="simple"/></inline-formula> be a random vector defined on a subset of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x14.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x15.png" xlink:type="simple"/></inline-formula> be the probability density function of the probability distribution function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x16.png" xlink:type="simple"/></inline-formula>. For any convex function f having <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x17.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x18.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.70513-formula394"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x19.png"  xlink:type="simple"/></disp-formula><p>is an f-divergence. Here <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x20.png" xlink:type="simple"/></inline-formula> is the support of the probability distribution function induced by the random vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x21.png" xlink:type="simple"/></inline-formula>.</p><p>The f-divergences satisfy, by construction, the following properties:</p><p>1) An f-divergence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x22.png" xlink:type="simple"/></inline-formula> is defined for all pairs <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x23.png" xlink:type="simple"/></inline-formula> on the same sample space.</p><p>2) For any measurable transformation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x24.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x25.png" xlink:type="simple"/></inline-formula>.</p><p>3) The f-divergence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x26.png" xlink:type="simple"/></inline-formula> takes its minimum when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x27.png" xlink:type="simple"/></inline-formula> and maximum when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x28.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x29.png" xlink:type="simple"/></inline-formula> are orthogonal, denoted by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x30.png" xlink:type="simple"/></inline-formula>.</p><p>4) If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x31.png" xlink:type="simple"/></inline-formula> is a family of densities on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x32.png" xlink:type="simple"/></inline-formula> with monotone likelihood ratio, then for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x33.png" xlink:type="simple"/></inline-formula>, we have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x34.png" xlink:type="simple"/></inline-formula>.</p><p>We will refer to them as f-properties. For more rigorous definitions, details, explana- tions, examples and discussions, see [<xref ref-type="bibr" rid="scirp.70513-ref35">35</xref>] . The first property simply ensures validity of the divergence. The second property, which is extensively studied in [<xref ref-type="bibr" rid="scirp.70513-ref38">38</xref>] , implies that a measurable transformation will not increase the divergence between two probability distributions. At first, this property might seem counterintuitive in a clustering context, since transformations are often used to increase discernability between clusters. How- ever, these transformations are applied on the observations before density estimation, and hence, the increased discernability will be reflected by the new density estimates. The third property stating minimum value at equality and maximum value at ortho- gonality follows immediately from the concept of a divergence being a measure of the distance between two probability distributions. A definition of orthogonality between distributions can be found in [<xref ref-type="bibr" rid="scirp.70513-ref40">40</xref>] (see also Appendix A). The fourth property ensures that when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x35.png" xlink:type="simple"/></inline-formula> is further away from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x36.png" xlink:type="simple"/></inline-formula> than <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x37.png" xlink:type="simple"/></inline-formula> is, the divergence between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x38.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x39.png" xlink:type="simple"/></inline-formula> will be larger than between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x40.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x41.png" xlink:type="simple"/></inline-formula>, which also follows from the diver- gence being a concept of distance. There has been extensive research on f-divergences, and they have other properties not listed here. We have presented these four properties for the reader to gain insight about f-divergences since they are popular as fundaments for dissimilarity measures.</p></sec><sec id="s3_2"><title>3.2. Properties for Dissimilarity Measures for Hybrid Clustering</title><p>An important difference between divergences and dissimilarity measures is that sub- clusters can have different weights (corresponding to the a priori probability), as op- posed to probability distributions. <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) shows an example of a Gaussian mixture</p><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Gaussian mixtures densities (black line) and their components; coloured lines from left to right; blue, red, green, pink. (a) Equal variance, unequal a priori probabilities; (b) Small outlying component; (c) Background noise component; (d) Equal mean and unequal variance; (e) Two equal components (green hidden by pink); (f) A priori probabilities with different relative values.</title></caption><fig id ="fig4_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x42.png"/></fig><fig id ="fig4_2"><label> (c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x43.png"/></fig></fig-group><p>distribution where all three components have equal variance. Since the Gaussian distribution has monotone likelihood ratio, it follows from the fourth f-property that the two components with smallest distance between the means will have the smallest f-divergence. Since the blue and the red components are slightly closer to each other than the red and the green components are, those are the two with the smallest f-divergence. This illustrative example shows that dissimilarity measures should be functions of both the subclusters’ density and weight, and that dissimilarity measures should have other properties than divergences. We will continue this section with motivation for the data-independent properties presented here.</p><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows Gaussian mixture densities and their components, and illustrates different aspects of merging in the following situation: The coloured lines represent the probability densities of the current subclusters, and the next step in the hybrid cluster- ing is to merge the two subclusters with lowest dissimilarity. These examples illustrate the demand for the properties introduced later in this section. The details are found in Appendix B, where also the results of different dissimilarity measures (see Section 3.3) are given.</p><p>Here, we illustrate that the presence of outlier and noise observations can obstruct the clustering. Because of this, we propose properties that involve robustness to outlier and noise observations. Since density-based dissimilarity measures are functions of the observations indirectly through the density and weight estimates of the subclusters, we refer to an outlying component as one having small weight and large distance from the other components (see <xref ref-type="fig" rid="fig4">Figure 4</xref>(b)), and noise component as one having large scatter and low maximum density (see <xref ref-type="fig" rid="fig4">Figure 4</xref>(c)). Robustness, in this context, refers to the concept that the presence or absence of an outlier component or noise component should not influence the final clustering significantly. This can be illustrated by the example in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b). Let the small component to the right be an outlying com- ponent, and let the stopping rule of this particular clustering be to stop at two clusters. If the outlying component were absent, the clustering would not involve merging, and the two components to the left would define the two final clusters. In the presence of the outlying component, any robust dissimilarity measure would merge the outlying component with one of the large components, as this has minimal influence on the final clustering. Similarly, for <xref ref-type="fig" rid="fig4">Figure 4</xref>(c), the noise component should be merged with one of the other components instead of constituting a cluster of its own in the case of a two-cluster solution.</p><p>There are other ways to deal with outliers and noise than by having robust dis- similarity measures. A common approach is to remove outliers and noise observations by pre-processing of the data (for example, trimming or snipping, [<xref ref-type="bibr" rid="scirp.70513-ref41">41</xref>] ), and for hybrid clustering, several algorithms have been proposed [<xref ref-type="bibr" rid="scirp.70513-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref14">14</xref>] . The drawback of this approach is that it usually requires some user-set parameter, which in turn requires knowledge of the data. Huber and Ronchetti ( [<xref ref-type="bibr" rid="scirp.70513-ref42">42</xref>] , p. 4) discussed several other issues regarding robustness versus pre-processing. Another important issue that they ad- dressed ( [<xref ref-type="bibr" rid="scirp.70513-ref42">42</xref>] , p. 8) is the difference between robustness and diagnostics, where the purpose of diagnostics is to detect the outliers. Clearly, if the main objective of a par- ticular clustering procedure is diagnostics then the dissimilarity measure should not be robust to outliers. It is therefore important to know whether the chosen dissimilarity measure satisfies a given outlier property.</p><p>Hybrid clustering assumes that the model used for partitional clustering is different from the final clusters, else, there would be no need for a merging step. An example is the GMM for heavy-tailed clusters, as illustrated in <xref ref-type="fig" rid="fig4">Figure 4</xref>(d) where the red and the green components have the same mean, and unequal variances. Whether the red and the green component actually belong to the same cluster depends on the particular understanding of the cluster concept, and having a data-independent property for this particular situation enables the user to choose the proper dissimilarity measure.</p><p>The third f-property (minimum at equality and maximum at orthogonality) is funda- mental for divergences, but can cause trouble for dissimilarity measures. In <xref ref-type="fig" rid="fig4">Figure 4</xref>(b), the outlying component is nearly orthogonal to the two other components, but if the dissimilarity measure is robust to outliers, it cannot at the same time attain its maxi- mum value. We therefore propose an additional<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x44.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x45.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x46.png" xlink:type="simple"/></inline-formula> are the weights of subcluster k and l, to the third f-property to make it suitable for dissimilarity measures. We use the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x47.png" xlink:type="simple"/></inline-formula> both to denote a priori probabilities for a mixture distribu- tion, and the subclusters’ weight, since one is an estimate of the other. <xref ref-type="fig" rid="fig4">Figure 4</xref>(e) shows a four-component GMM where the two rightmost components are identical, and therefore the green component is hidden behind the pink. The Shannon entropy dis- similarity measure, SE, defined in Section 3.3, does not attain its minimum value at equality, and as a result, the dissimilarity between the blue and the red component is smaller than that between the identical green and pink components.</p><p>First, we propose a symmetry property, which does not require further explanation. The other five properties are motivated by the discussions earlier in this section. Suppose that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x48.png" xlink:type="simple"/></inline-formula> is the pdf associated with the k-th subcluster having weight<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x49.png" xlink:type="simple"/></inline-formula>,</p><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x50.png" xlink:type="simple"/></inline-formula>. The dissimilarity between the subclusters k and l is denoted by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x51.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x52.png" xlink:type="simple"/></inline-formula> when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x53.png" xlink:type="simple"/></inline-formula>, or arbitrarily small when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x54.png" xlink:type="simple"/></inline-formula>, and let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x55.png" xlink:type="simple"/></inline-formula> when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x56.png" xlink:type="simple"/></inline-formula>, or arbitrarily large when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x57.png" xlink:type="simple"/></inline-formula>.</p><p>Symmetry: The dissimilarity measure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x58.png" xlink:type="simple"/></inline-formula> is symmetric, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x59.png" xlink:type="simple"/></inline-formula>for all k and l.</p><p>Equality: If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x60.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x61.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x62.png" xlink:type="simple"/></inline-formula>.</p><p>Orthogonality: If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x63.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x64.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x65.png" xlink:type="simple"/></inline-formula>.</p><p>Outlier: If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x66.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x67.png" xlink:type="simple"/></inline-formula> are not orthogonal, and if one of the weights is close to zero, the dissimilarity measure will be close to its minimum. That is, for every<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x68.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x69.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x70.png" xlink:type="simple"/></inline-formula>.</p><p>Noise: If the maximum density of the large-scatter subcluster, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x71.png" xlink:type="simple"/></inline-formula>, is close to zero, the dissimilarity measure will be close to its minimum. That is, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x72.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x73.png" xlink:type="simple"/></inline-formula> for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x74.png" xlink:type="simple"/></inline-formula>, then for every<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x75.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x76.png" xlink:type="simple"/></inline-formula> such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x77.png" xlink:type="simple"/></inline-formula>.</p><p>Mode: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula> be two Gaussian probability density functions with loca- tion parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula>, respectively, and scatter parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x83.png" xlink:type="simple"/></inline-formula>, respectively. Further, suppose that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x84.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x85.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x86.png" xlink:type="simple"/></inline-formula> is a constant. Under such circumstances, for every<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x87.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x88.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x89.png" xlink:type="simple"/></inline-formula>. And, for every<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x90.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x91.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x92.png" xlink:type="simple"/></inline-formula>.</p><p>The properties do not state whether the outlying component in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b), the noise component in <xref ref-type="fig" rid="fig4">Figure 4</xref>(c), or the two components with equal mean in <xref ref-type="fig" rid="fig4">Figure 4</xref>(d) should be merged. They state that, at some point, for a very small component, for a component with very low maximum density, or for two components with equal mean, the dissimilarity measure should attain its minimum value.</p></sec><sec id="s3_3"><title>3.3. Dissimilarity Measures for Hybrid Clustering</title><p>We here present some density-based dissimilarity measures, illustrating which pro- perties some well-known dissimilarity measures satisfy. Many dissimilarity measures are closely connected, e.g. the Shannon entropy and the Kullback-Leibler information, but they satisfy different properties. The list of dissimilarity measures is not, and cannot be, extensive, but shows a variety and includes dissimilarity measures both based on f-divergences and the Shannon entropy. None of the dissimilarity measures we could find in the literature satisfies all of the properties, and we therefore propose one that does; a Kullback-Leibler information based dissimilarity measure, KLinf. <xref ref-type="table" rid="table1">Table 1</xref> shows which properties each dissimilarity measure satisfies. The technical details are provided in Appendix A. In the following, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x93.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x94.png" xlink:type="simple"/></inline-formula> are the pdf’s of the probability measures <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x95.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x96.png" xlink:type="simple"/></inline-formula>, respectively, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x97.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x98.png" xlink:type="simple"/></inline-formula> are the weights of the k-th and the l-th subcluster, respectively, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x99.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x100.png" xlink:type="simple"/></inline-formula>.</p><p>1) Shannon entropy</p><p>The Shannon entropy for a continuous distribution, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x101.png" xlink:type="simple"/></inline-formula>, is defined as [<xref ref-type="bibr" rid="scirp.70513-ref43">43</xref>]</p><disp-formula id="scirp.70513-formula395"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x102.png"  xlink:type="simple"/></disp-formula><p>We here present three dissimilarity measures for probability measures <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x103.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x104.png" xlink:type="simple"/></inline-formula> that are functions of the Shannon entropy; the Shannon entropy dissimilarity measure (SE), the weighted Shannon entropy dissimilarity measure (wSE), and the Jensen- Shannon dissimilarity measure (JS).</p><disp-formula id="scirp.70513-formula396"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x105.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula397"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x106.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula398"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x107.png"  xlink:type="simple"/></disp-formula><p>SE minimises the Shannon entropy of the resulting merging [<xref ref-type="bibr" rid="scirp.70513-ref22">22</xref>] . wSE measures the divergence between the two components and their merging, multiplied by the subclusters’ weights [<xref ref-type="bibr" rid="scirp.70513-ref36">36</xref>] . Straightforward algebra shows that JS is a weighted version of the Kullback-Leibler divergence [<xref ref-type="bibr" rid="scirp.70513-ref44">44</xref>] .</p><p>As discussed in Section 3.2, the Shannon entropy dissimilarity measure does not satisfy the Equality property, with the result seen in <xref ref-type="fig" rid="fig4">Figure 4</xref>(e). The weighted version, wSE, neither satisfies the Equality nor the Orthogonality property. The Jensen-Shannon dissimilarity measure is a function of relative weights, and an example of its con- sequences is seen in <xref ref-type="fig" rid="fig4">Figure 4</xref>(f), showing a large component to the left (blue) and three equally sized components to the right (red, green, and pink). Since the red component is relatively small compared to the blue one, but has the same size as the green one, the Jensen-Shannon dissimilarity between the blue and the red component is smallest.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Dissimilarity measures and properties. “x” indicates satisfaction and “-” indicates violation</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Dissimilarity measure</th><th align="center" valign="middle"  colspan="6"  >Property</th></tr></thead><tr><td align="center" valign="middle" >Equality</td><td align="center" valign="middle" >Orthogonality</td><td align="center" valign="middle" >Symmetry</td><td align="center" valign="middle" >Outlier</td><td align="center" valign="middle" >Noise</td><td align="center" valign="middle" >Mode</td></tr><tr><td align="center" valign="middle" >SE</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >wSE</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >JS</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >Err</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >x</td></tr><tr><td align="center" valign="middle" >Bhat</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >x</td></tr><tr><td align="center" valign="middle" >KLdiv</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >x</td></tr><tr><td align="center" valign="middle" >KLinf</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td><td align="center" valign="middle" >x</td></tr></tbody></table></table-wrap><p>2) Probability of misclassification</p><p>The error probability of the Bayes classifier for two classes is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x108.png" xlink:type="simple"/></inline-formula>, and subtracting it from one will be an f-divergence [<xref ref-type="bibr" rid="scirp.70513-ref37">37</xref>]</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x109.png" xlink:type="simple"/></inline-formula>.</p><p>Err is an example of a dissimilarity measure that does not satisfy the Outlier property. As a consequence, the small outlying component in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) will not be merged with any of the other components even if its size decreases to a minimum.</p><p>3) Bhattacharyya distance</p><p>The Bhattacharyya coefficient measures how much two distributions overlap, and is defined as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x110.png" xlink:type="simple"/></inline-formula>. The Bhattacharyya distance is one of the most classical distance function used in the literature [<xref ref-type="bibr" rid="scirp.70513-ref45">45</xref>] [<xref ref-type="bibr" rid="scirp.70513-ref46">46</xref>] , and is defined as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x111.png" xlink:type="simple"/></inline-formula>. A weighted version of the distance is defined as [<xref ref-type="bibr" rid="scirp.70513-ref36">36</xref>] .</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x112.png" xlink:type="simple"/></inline-formula>.</p><p>As we will see in Sections 4.1 and 4.2, Bhat performs very well in many situations, but can fail in the presence of a noise component, since it does not satisfy the Noise property. In <xref ref-type="fig" rid="fig4">Figure 4</xref>(c), Bhat would have merged the blue and the red component.</p><p>4) Kullback-Leibler information</p><p>When one distribution is approximated by another, information is lost. The amount of lost information can be measured by the Kullback-Leibler information. For two probability measures <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x113.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x114.png" xlink:type="simple"/></inline-formula>, the Kullback-Leibler information, I, and Kullback- Leibler divergence, J are defined as [<xref ref-type="bibr" rid="scirp.70513-ref47">47</xref>]</p><disp-formula id="scirp.70513-formula399"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x115.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula400"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x116.png"  xlink:type="simple"/></disp-formula><p>Since the Kullback-Leibler information is not symmetric, it is less suited for hybrid clustering. The Kullback-Leibler divergence was evaluated as dissimilarity measure for hybrid clustering by [<xref ref-type="bibr" rid="scirp.70513-ref21">21</xref>] , but in the unweighted version. We therefore define a dis- similarity measure based on the Kullback-Leibler divergence as</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x117.png" xlink:type="simple"/></inline-formula>.</p><p>A new dissimilarity measure:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x118.png" xlink:type="simple"/></inline-formula>does not satisfy the Noise property, and we therefore propose a symmetric dissimilarity measure based on the symmetrisation of the Kullback-Leibler information by the minimum function. The new dissimilarity measure is denoted by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x119.png" xlink:type="simple"/></inline-formula>, and for two probability measures <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x120.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x121.png" xlink:type="simple"/></inline-formula>, it is defined as</p><disp-formula id="scirp.70513-formula401"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x122.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x123.png" xlink:type="simple"/></inline-formula>satisfies all our proposed properties in Section 3.2 and we therefore expect it to perform well in situations where these properties are desirable.</p></sec></sec><sec id="s4"><title>4. Illustration of the Dissimilarity Measure’s Impact on the Final Clustering</title><p>We here illustrate how the choice of dissimilarity measure impacts the final clustering in view of the proposed properties. GMM is used to estimate the density, and BIC and AIC are used to estimate the number of components, corresponding to the number of subclusters. It does not suggest that this is the best partitional clustering technique, but for illustrational purposes it is appropriate, since it is well-known, relatively fast, and easily available. A pre-defined number of clusters is used as stopping rule since the focus of this article is the dissimilarity measure and not the stopping rule. The results for wSE are not displayed since its shortcomings are illustrated by SE and JS.</p><p>We compare the performances of the dissimilarity measures by the difference between the misclassification rate, which is dependent on the dissimilarity measure, and the minimum misclassification rate, which is defined by the partitional clustering (see Section 2.1). The misclassification rate is defined as the proportion of the observations wrongly clustered by the final clustering. To compare the dissimilarity measures, we define true cluster membership according to the samples’ origin, as illustrated in <xref ref-type="fig" rid="fig5">Figure 5</xref>, which deviates from the usual concept of cluster. However, defining cluster membership by the relation between observations will favour some</p><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Examples of random samples of 500 observations drawn from different types of two-dimensional distributions. The colours indicate which cluster each sample is drawn from. (a) Student’s t,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x126.png" xlink:type="simple"/></inline-formula>; (b) Cauchy (Student’s t,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x127.png" xlink:type="simple"/></inline-formula>; (c) Uniform; (d) Gamma; (e) Gaussian with uniform noise; (f) Gaussian-Laplace mixture.</title></caption><fig id ="fig5_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x124.png"/></fig><fig id ="fig5_2"><label> (c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x125.png"/></fig></fig-group><p>dissimilarity measures over others by construction, according to how relation is defined.</p><sec id="s4_1"><title>4.1. Simulation Study</title><p>We here present a simulation study for six types of distributions (for details, see Appendix C), shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>. The wide variety in distributions and their deviance from the model for partitional clustering illustrate the relevance of the proposed properties. For each random sampling, a partitional clustering is performed by GMM, where the number of components is estimated by BIC and AIC. The hierarchical clustering is then performed according to each dissimilarity measure, until three clusters is reached. <xref ref-type="fig" rid="fig6">Figure 6</xref> shows the entire merging process. The mean values of 100 repetitions and their 95% confidence intervals are shown in <xref ref-type="fig" rid="fig7">Figure 7</xref>. There are eight varieties for each distribution: BIC (blue) or AIC (red) for the number of components, small (open) or large (filled) data sets, and dimension 2 (circles) or 3 (triangles). The noise observations in <xref ref-type="fig" rid="fig5">Figure 5</xref>(e) are not counted as misclassified, regardless of which cluster they are assigned to. As discussed in Section 2, both partitional clustering and the stopping criterion impact the final clustering, and it is possible that the results would have been different with another partitional clustering technique on the same data set.</p><p>From the above study we see that no dissimilarity measure performs uniformly best. We have observed some phenomena for different dissimilarity measures. The three dissimilarity measures that satisfy the Equality, Orthogonality and Outlier properties (Bhat, KLdiv, and KLinf) have overall lower misclassification than those that do not satisfy the aforementioned properties (JS, SE, and Err). When the observations are generated from a Student’s t distribution with 2 degrees of freedom, the clusters are well separated, symmetric and dense (see <xref ref-type="fig" rid="fig5">Figure 5</xref>(a)), but still, JS, SE, and Err fail to perform well. The poor performance of SE is shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>. The misclassification rates for JS, SE, and Err are higher using AIC than using BIC because the number of components is higher with AIC, and consequently, the subcluster weights are smaller. For most distributions, there are no clear distinctions among Bhat, KLdiv, and KLinf, with some exceptions. For the Gaussian-Laplace mixture distribution, an example of a heavy-tailed distribution, KLinf performs better than KLdiv. This can be explained by investigating at which rate the dissimilarity measure changes according to changes in the constant a described in the Mode property; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x128.png" xlink:type="simple"/></inline-formula>faster than <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x129.png" xlink:type="simple"/></inline-formula> as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x130.png" xlink:type="simple"/></inline-formula> (see Appendix A for details). For the Gaussian with uniform noise distribution, Bhat and KLdiv, which do not satisfy the noise property, perform worse than KLinf. Bhat also does not perform well for the Cauchy distribution due to the noise-like observations from the heavy tails; The sparsely scattered observations with different origins result in one component with large scatter and low density. The AIC and the Kullback-Leibler information measure the fit of the model to the true dis- tribution in a similar manner [<xref ref-type="bibr" rid="scirp.70513-ref28">28</xref>] . However, this will not favour the Kullback-Leibler based dissimilarity measures because they measure the fit between components.</p><fig-group id="fig6"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> A random sample from Student’s t distribution with 2 degrees of freedom. (a) True cluster membership (dots, circles, crosses); (b) MAP-component membership for a six-component GMM fitted to the observations; (c) The best merging in terms of minimum misclassification rate; (d)-(f) and (g)-(i) Hierarchical merging using KLinf and SE, respectively. (d) First merging step; KLinf; (e) Second step; KLinf; (f) Final merging; KLinf; (g) First merging step; SE; (h) Second step; SE; (i) Final merging; SE.</title></caption><fig id ="fig6_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x131.png"/></fig><fig id ="fig6_2"><label> (c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x132.png"/></fig><fig id ="fig6_3"><label>(d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x133.png"/></fig></fig-group><p>Several other studies have investigated hybrid clustering by simulated data. We illustrate the performance of the dissimilarity measures for the simulated data described in [<xref ref-type="bibr" rid="scirp.70513-ref22">22</xref>] , where GMM/BIC was used for partitioning in hybrid clustering, in [<xref ref-type="bibr" rid="scirp.70513-ref32">32</xref>] and [<xref ref-type="bibr" rid="scirp.70513-ref34">34</xref>] , where GMM/BIC was used as reference for ICL and Student’s t mixture fitting, respectively. <xref ref-type="fig" rid="fig8">Figure 8</xref> shows the results for the data from [<xref ref-type="bibr" rid="scirp.70513-ref34">34</xref>] (blue), [<xref ref-type="bibr" rid="scirp.70513-ref32">32</xref>] (red), and [<xref ref-type="bibr" rid="scirp.70513-ref22">22</xref>] (cyan). The data are generated by random sampling from the distributions described in the respective papers, with 100 repetitions. The trends that appeared in</p><fig-group id="fig7"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Difference between misclassification rate and minimum misclassification rate, and the 95% confidence intervals, for BIC and AIC, small and large data sets, dimension 2 and 3, for random samples from the distributions in <xref ref-type="fig" rid="fig5">Figure 5</xref>, obtained by GMM fitting and three final clusters. The number of components estimated by BIC and AIC varies for each sample. (a) Student’s t,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x136.png" xlink:type="simple"/></inline-formula>; (b) Cauchy (Student’s t,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x137.png" xlink:type="simple"/></inline-formula>; (c) Uniform; (d) Gamma; (e) Gaussian with uniform noise; (f) Gaussian-Laplace mixture.</title></caption><fig id ="fig7_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x134.png"/></fig><fig id ="fig7_2"><label> (c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x135.png"/></fig></fig-group><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Difference between misclassification rate and minimum misclassification rate, and the 95% confidence intervals for simulated data, using GMM/BIC as partitional clustering</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x138.png"/></fig><p><xref ref-type="fig" rid="fig7">Figure 7</xref> are also seen in <xref ref-type="fig" rid="fig8">Figure 8</xref> where no dissimilarity measure is uniformly best, but that Bhat, KLdiv, and KLinf perform better. For the Gaussian mixture distribution (cyan) described in [<xref ref-type="bibr" rid="scirp.70513-ref22">22</xref>] , the choice of dissimilarity measure has very little impact on the final clustering. Interestingly, their proposed dissimilarity measure, SE, does not perform better than the others. KLinf fails more often than Bhat and KLdiv for the Uniform and Gaussian distribution.</p></sec><sec id="s4_2"><title>4.2. Application to Real Data</title><p>Wisconsin diagnostic breast cancer data: The Wisconsin diagnostic breast cancer data, available from the UCI machine learning repository [<xref ref-type="bibr" rid="scirp.70513-ref30">30</xref>] , consists of 569 observa- tions in 30 dimensions and is labelled according to diagnosis, which defines the classes. Fraley and Raftery [<xref ref-type="bibr" rid="scirp.70513-ref48">48</xref>] used the three features selected by Mangasarian et al. [<xref ref-type="bibr" rid="scirp.70513-ref49">49</xref>] and achieved a misclassification rate of 5%. We have here used sequential forward feature selection. At each step, the feature that improves a quadratic discriminant classifier the most in terms of correctly classified observations is added. The process is stopped when adding a new feature results in an improvement of less than 10<sup>−6</sup>. The training and testing of the classifier is performed on separate sets, using cross-validation. The di- mension of the resulting data sets varied from three to nine, and all features were selected at least once in 100 repetitions. <xref ref-type="fig" rid="fig9">Figure 9</xref>(a) shows an example with three di- mensions chosen by the feature selection. The mean misclassification rate for KLinf and Bhat was 5%. The result is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>0. As we have observed the phenomena in the simulated data, here also, Bhat, KLdiv and KLinf perform better than JS, SE, and Err. The Wisconsin breast cancer data is an example of data with higher dimensions, in this example, up to nine dimensions. The dissimilarity measures themselves are not limited by the number of dimensions and data sparsity, but indirectly they will suffer from bad density estimation.</p><p>Yeast data: A Student’s t mixture distribution was used for partitional clustering of the Yeast data described in Section 1 (see <xref ref-type="fig" rid="fig3">Figure 3</xref>). The result for 10 repetitions is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>0. We used Student’s t mixture on the Yeast data to illustrate the use of another partitional clustering technique. The variation is due to slightly different estimated parameters for each repetition.</p><fig-group id="fig9"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> The Wisconsin diagnostic breast cancer data. (a) The initial partitioning, labelled according to MAP. Final clustering using (b) Bhat and (c) SE.</title></caption><fig id ="fig9_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x139.png"/></fig></fig-group><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> Difference between misclassification rate and minimum misclassification rate, and the 95% confidence intervals for Breast Cancer data using GMM as partitional clustering (red), and Yeast data using Student’s t as partitional clustering (blue)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x140.png"/></fig></sec></sec><sec id="s5"><title>5. Discussion</title><p>In the literature, the choice of density-based dissimilarity measure for hybrid clustering has been given little attention, despite its heavy influence on the final clustering. We have proposed data-independent properties. The Equality and Orthogonality properties are presented as axiomatic for divergences [<xref ref-type="bibr" rid="scirp.70513-ref35">35</xref>] , and although we will not claim that they are axiomatic for dissimilarity measures, it is indeed hard to imagine how they would be a drawback in hybrid clustering. The Outlier and the Noise properties ensure that the dissimilarity measure is robust to certain types of outlier and noise observa- tions, meaning that whether outlier or noise observations are present or absent has little effect on the clustering. One can choose a partitional clustering that is less likely to produce small outlying subclusters (for example Student’s t instead of GMM), but the possibility cannot be ruled out. Detection of outliers in pre-processing can reduce the necessity for robust dissimilarity measures, but requires extra knowledge about the data. The Mode property is valid only for the case of two Gaussian components with equally shaped covariance matrices, which is a special case. However, light-tailed models for heavy-tailed clusters are an important issue in hybrid clustering, since the need for hybrid clustering arises from a situation where the partitional clustering model does not fit the cluster distribution, and the Mode property can contribute in explaining a dissimilarity measure’s behaviour under these circumstances.</p><p>The illustration of clustering results for different dissimilarity measures shows that the choice of dissimilarity measure can have significant impact on the final clustering. It also shows that the behaviour of a dissimilarity measure can be anticipated based on which properties it satisfies. However, the properties will not give a full description of a dissimilarity measure’s behaviour, and analysis can give further insight. The different behaviour of KLdiv and KLinf for the Gaussian-Laplace mixture required further ana- lysis, since both dissimilarity measures satisfied the Mode property. Data-independent properties can be used to choose the right dissimilarity measure, evaluate new dis- similarity measures, and modify existing ones. As an example of modification, the factor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x141.png" xlink:type="simple"/></inline-formula> in the dissimilarity measures Bhat, KLdiv, and KLinf can be changed to, for example,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x142.png" xlink:type="simple"/></inline-formula>. The dissimilarity measures will satisfy the Outlier property, but the behaviour with respect to how small the outlying component in <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) must be before it is merged despite its near orthogonality, will change.</p><p>The final number of clusters is another legitimate issue in hybrid clustering. A pro- perty for dissimilarity measures when used for cluster number estimation, for instance by setting a threshold or searching for an “elbow” should be a topic for future studies. <xref ref-type="fig" rid="fig1">Figure 1</xref>1 shows the values for KLinf and SE as the number of clusters goes from six to one for the sample in <xref ref-type="fig" rid="fig6">Figure 6</xref>. Both show an elbow at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x143.png" xlink:type="simple"/></inline-formula>. The three-cluster solution is more appropriate for the KLinf-based merging than for the SE-based merging.</p><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> The normalised values of KLinf (red) and SE (blue). They both show an elbow at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x145.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403126x144.png"/></fig><sec id="s5_1"><title>5.1. Main Contribution of the Article</title><p>We have proposed data-independent properties for density-based dissimilarity mea- sures for hybrid clustering. Data-independent properties provide a tool for evaluating and comparing dissimilarity measures on a more general level than for particular data sets with known or user defined clusters.</p><p>The significance of the properties has been illustrated through studies on simulated and real data. We have evaluated several well-known dissimilarity measures in terms of the proposed properties. Besides, we have proposed a new dissimilarity measure, KLinf, that satisfies all the proposed properties. It shows good performance in both simulated and real data. However, we do not claim that KLinf is the best density-based dis- similarity measure for hybrid clustering; the concept of clustering is far too complex and diverse.</p></sec><sec id="s5_2"><title>5.2. Concluding Remarks</title><p>Clustering is an exploratory tool for use in situations where the data have no ground truth. The diversity of clustering problems and the inherit subjectivity demands dif- ferent dissimilarity measures for different problems. In this article, we have proposed specific properties, and those properties offer a tool to choose the most appropriate dissimilarity measure and to interpret the clustering result. In particular, a measure that does not fulfil the Equality or Orthogonality properties can give peculiar results, since it violates the most common concepts of “distance”. Similarly, a dissimilarity measure that does not fulfil the Outlier property can lead to extreme results in many situations (see e.g. <xref ref-type="fig" rid="fig9">Figure 9</xref>(c)). The data presented in this article are in two or three dimensions, for illustration purposes, but for higher dimensions, the user cannot visually inspect the clustering result, and analytical knowledge is then crucial.</p></sec></sec><sec id="s6"><title>Cite this paper</title><p>M&#248;llersen, K., Dhar, S.S. and Godtliebsen, F. (2016) On Data-In- dependent Properties for Density-Based Dis- similarity Measures in Hybrid Clustering. Applied Mathematics, 7, 1674-1706. http://dx.doi.org/10.4236/am.2016.715143</p></sec><sec id="s7"><title>Appendix</title>Appendix A<p>Some preliminaries:</p><p>1) It is straightforward to see that the dissimilarity measures in Section 3.3 are symmetric.</p><p>2) The integral is taken over <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x146.png" xlink:type="simple"/></inline-formula> unless otherwise noted. Here <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x147.png" xlink:type="simple"/></inline-formula> denotes the support of the distribution function associated with the random variable X. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x148.png" xlink:type="simple"/></inline-formula> be the pdf of subcluster k, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x149.png" xlink:type="simple"/></inline-formula> denote the weight,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x150.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x151.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x152.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x153.png" xlink:type="simple"/></inline-formula>denotes the dissimilarity measure between the two subclusters k and l.</p><p>3) Orthogonality is defined as [<xref ref-type="bibr" rid="scirp.70513-ref40">40</xref>] : <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x154.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x155.png" xlink:type="simple"/></inline-formula> are orthogonal if for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x156.png" xlink:type="simple"/></inline-formula>, there exist <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x157.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x158.png" xlink:type="simple"/></inline-formula> such that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x159.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x160.png" xlink:type="simple"/></inline-formula>,</p><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x161.png" xlink:type="simple"/></inline-formula>.</p><p>4) Note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula> for any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula> implies that for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x164.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x165.png" xlink:type="simple"/></inline-formula>almost everywhere (a.e.) on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x166.png" xlink:type="simple"/></inline-formula>, since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x167.png" xlink:type="simple"/></inline-formula>, and similarly <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x168.png" xlink:type="simple"/></inline-formula> for any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x169.png" xlink:type="simple"/></inline-formula> implies that for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x170.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x171.png" xlink:type="simple"/></inline-formula>a.e. on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x172.png" xlink:type="simple"/></inline-formula>, since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x173.png" xlink:type="simple"/></inline-formula>.</p><p>5) The logarithmic function is monotonic increasing, and consequently, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x174.png" xlink:type="simple"/></inline-formula>, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x175.png" xlink:type="simple"/></inline-formula>. Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x176.png" xlink:type="simple"/></inline-formula> is a pdf,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x177.png" xlink:type="simple"/></inline-formula>.</p><p>6) If a dissimilarity measure does not satisfy either the Equality or the Orthogonality property, the Mode property will not be satisfied, since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x178.png" xlink:type="simple"/></inline-formula> gives<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x179.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x180.png" xlink:type="simple"/></inline-formula> gives<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x181.png" xlink:type="simple"/></inline-formula>. If a dissimilarity measure is an f-divergence, the Mode property is automatically satisfied. This is not necessarily true for modified f- divergences.</p><p>Next, we investigate whether the dissimilarity measures in Section 3.3 satisfy the properties proposed in Section 3.2.</p><p>Shannon entropy based measures</p><p>1) Unweighted version, SE: Recall that</p><disp-formula id="scirp.70513-formula402"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x182.png"  xlink:type="simple"/></disp-formula><p>and note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x183.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x184.png" xlink:type="simple"/></inline-formula>. We have the following results:</p><p>Equality: Set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x185.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x185.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x186.png" xlink:type="simple"/></inline-formula>. We now have</p><disp-formula id="scirp.70513-formula403"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x187.png"  xlink:type="simple"/></disp-formula><p>This implies that SE does not satisfy the Equality property, since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x188.png" xlink:type="simple"/></inline-formula>.</p><p>Orthogonality: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x189.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x190.png" xlink:type="simple"/></inline-formula>. Then we can write</p><disp-formula id="scirp.70513-formula404"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x191.png"  xlink:type="simple"/></disp-formula><p>Let</p><disp-formula id="scirp.70513-formula405"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x192.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula406"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x193.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula407"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x194.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula408"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x195.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula409"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x196.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula410"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x197.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x198.png" xlink:type="simple"/></inline-formula> a.e. on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x199.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x200.png" xlink:type="simple"/></inline-formula> a.e. on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x201.png" xlink:type="simple"/></inline-formula> for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x202.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x203.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x204.png" xlink:type="simple"/></inline-formula>. Consequently,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x205.png" xlink:type="simple"/></inline-formula>. Since this is true for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x206.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x198.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x199.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x200.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x202.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x203.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x207.png" xlink:type="simple"/></inline-formula>, it follows that SE satisfies the Orthogonality property.</p><p>Outlier: Without loss of generality, let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x208.png" xlink:type="simple"/></inline-formula>. Let</p><disp-formula id="scirp.70513-formula411"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x209.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula412"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x210.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula413"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x211.png"  xlink:type="simple"/></disp-formula><p>For any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x212.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x213.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x214.png" xlink:type="simple"/></inline-formula>. Consequently, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x215.png" xlink:type="simple"/></inline-formula>, and since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x212.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x213.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x216.png" xlink:type="simple"/></inline-formula>, it follows that SE does not satisfy the Outlier property.</p><p>Noise: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x217.png" xlink:type="simple"/></inline-formula>, and let</p><disp-formula id="scirp.70513-formula414"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x218.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula415"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x219.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula416"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x220.png"  xlink:type="simple"/></disp-formula><p>For any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x221.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x222.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x222.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x223.png" xlink:type="simple"/></inline-formula>. Consequently, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x222.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x223.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x224.png" xlink:type="simple"/></inline-formula>, and since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x222.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x223.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x224.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x225.png" xlink:type="simple"/></inline-formula>, it follows that SE does not satisfy the Noise property.</p><p>Mode: Since SE does not satisfy the Equality property, it will not satisfy the Mode property. ,</p><p>2) Weighted version, wSE: Recall that</p><disp-formula id="scirp.70513-formula417"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x226.png"  xlink:type="simple"/></disp-formula><p>and note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x227.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x227.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x228.png" xlink:type="simple"/></inline-formula>. We have the following results:</p><p>Equality: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x229.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x229.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x230.png" xlink:type="simple"/></inline-formula>. We then have</p><disp-formula id="scirp.70513-formula418"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x231.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x232.png" xlink:type="simple"/></inline-formula> attains its minimum only if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x232.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x233.png" xlink:type="simple"/></inline-formula> has infinite entropy, the Equality property is not satisfied.</p><p>Orthogonality: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x234.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x234.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x235.png" xlink:type="simple"/></inline-formula>. Then we can write</p><disp-formula id="scirp.70513-formula419"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x236.png"  xlink:type="simple"/></disp-formula><p>Let</p><disp-formula id="scirp.70513-formula420"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x237.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula421"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x238.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula422"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x239.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula423"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x240.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula424"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x241.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula425"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x242.png"  xlink:type="simple"/></disp-formula><p>Consequently,</p><disp-formula id="scirp.70513-formula426"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x243.png"  xlink:type="simple"/></disp-formula><p>and attains its maximum only if the two latter terms are equal to zero. It follows that wSE does not satisfy the Orthogonality property.</p><p>Outlier: Without loss of generality, let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x244.png" xlink:type="simple"/></inline-formula>. Let</p><disp-formula id="scirp.70513-formula427"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x245.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula428"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x246.png"  xlink:type="simple"/></disp-formula><p>Consequently,</p><disp-formula id="scirp.70513-formula429"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x247.png"  xlink:type="simple"/></disp-formula><p>and attains its minimum only if the two latter terms are infinite. It follows that wSE does not satisfy the Outlier property.</p><p>Noise: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x248.png" xlink:type="simple"/></inline-formula>, and let</p><disp-formula id="scirp.70513-formula430"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x249.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula431"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x250.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula432"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x251.png"  xlink:type="simple"/></disp-formula><p>Consequently, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x252.png" xlink:type="simple"/></inline-formula>, and attains its minimum only if the entropy of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x252.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x253.png" xlink:type="simple"/></inline-formula> is infinite. It follows that wSE does not satisfy the Noise property.</p><p>Mode: Since wSE does not satisfy the Equality and the Orthogonality properties, it will not satisfy the Mode property. ,</p><p>3) Jensen-Shannon dissimilarity measure, JS: Recall that</p><disp-formula id="scirp.70513-formula433"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x254.png"  xlink:type="simple"/></disp-formula><p>and note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x255.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x255.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x256.png" xlink:type="simple"/></inline-formula>.</p><p>Equality: Set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x257.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x257.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x258.png" xlink:type="simple"/></inline-formula>, and hence,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x257.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x258.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x259.png" xlink:type="simple"/></inline-formula>. We then have</p><disp-formula id="scirp.70513-formula434"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x260.png"  xlink:type="simple"/></disp-formula><p>Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x261.png" xlink:type="simple"/></inline-formula>, the Equality property is satisfied.</p><p>Orthogonality: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x262.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x262.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x263.png" xlink:type="simple"/></inline-formula>. Then we can write</p><disp-formula id="scirp.70513-formula435"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x264.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.70513-formula436"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x265.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula437"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x266.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula438"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x267.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula439"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x268.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula440"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x269.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula441"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x270.png"  xlink:type="simple"/></disp-formula><p>Consequently,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x271.png" xlink:type="simple"/></inline-formula>. Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x271.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x272.png" xlink:type="simple"/></inline-formula> will attain its maximum value only if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x271.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x272.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x273.png" xlink:type="simple"/></inline-formula>, the Orthogonality property is not satisfied.</p><p>Outlier: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x274.png" xlink:type="simple"/></inline-formula>. Then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x274.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x275.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x274.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x275.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x276.png" xlink:type="simple"/></inline-formula> are constant regardless of the value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x274.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x275.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x276.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x277.png" xlink:type="simple"/></inline-formula>, and</p><disp-formula id="scirp.70513-formula442"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x278.png"  xlink:type="simple"/></disp-formula><p>does not satisfy the Outlier property.</p><p>Noise: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x279.png" xlink:type="simple"/></inline-formula>, and let</p><disp-formula id="scirp.70513-formula443"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x280.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula444"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x281.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula445"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x282.png"  xlink:type="simple"/></disp-formula><p>Consequently,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x283.png" xlink:type="simple"/></inline-formula>. Since the latter term attains zero only if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x283.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x284.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x283.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x284.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x285.png" xlink:type="simple"/></inline-formula>, the Noise property is not satisfied.</p><p>Mode: Since JS does not satisfy the Orthogonality property, it will not satisfy the Mode property. ,</p><p>Probability of misclassification</p><p>1) Probability of misclassification, Err: Recall that</p><disp-formula id="scirp.70513-formula446"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x286.png"  xlink:type="simple"/></disp-formula><p>and note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x287.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x287.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x288.png" xlink:type="simple"/></inline-formula>. Note also that Err is an f-diver- gence, and hence satisfies the Equality, Orthogonality and Mode properties.</p><p>Outlier: Without loss of generality, let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x289.png" xlink:type="simple"/></inline-formula>. For any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x289.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x290.png" xlink:type="simple"/></inline-formula> there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x289.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x290.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x291.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.70513-formula447"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x292.png"  xlink:type="simple"/></disp-formula><p>and hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x293.png" xlink:type="simple"/></inline-formula> does not satisfy the Outlier property, since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x293.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x294.png" xlink:type="simple"/></inline-formula>.</p><p>Noise: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x295.png" xlink:type="simple"/></inline-formula>. For any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x295.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x296.png" xlink:type="simple"/></inline-formula> there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x295.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x296.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x297.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.70513-formula448"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x298.png"  xlink:type="simple"/></disp-formula><p>and hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x299.png" xlink:type="simple"/></inline-formula> does not satisfy the Noise property, since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x299.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x300.png" xlink:type="simple"/></inline-formula>. ,</p><p>Bhattacharyya distance</p><p>1) Weighted Bhattacharyya distance, Bhat: Recall that</p><disp-formula id="scirp.70513-formula449"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x301.png"  xlink:type="simple"/></disp-formula><p>and note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x302.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x302.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x303.png" xlink:type="simple"/></inline-formula>. Note also that the Bhattacharyya distance, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x302.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x303.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x304.png" xlink:type="simple"/></inline-formula>, is an f-divergence, and hence it is straightforward to show that Bhat satisfies the Equality and Orthogonality properties.</p><p>Outlier: Without loss of generality, let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x305.png" xlink:type="simple"/></inline-formula>. Then, for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x305.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x306.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x305.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x306.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x307.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.70513-formula450"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x308.png"  xlink:type="simple"/></disp-formula><p>for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x309.png" xlink:type="simple"/></inline-formula>, and hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x309.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x310.png" xlink:type="simple"/></inline-formula>satisfies the Outlier property.</p><p>Noise: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x311.png" xlink:type="simple"/></inline-formula>. Then, for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x311.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x312.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x311.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x312.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x313.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.70513-formula451"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x314.png"  xlink:type="simple"/></disp-formula><p>and hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x315.png" xlink:type="simple"/></inline-formula>does not satisfy the Noise property.</p><p>Mode: Since the Bhattacharyya distance is an f-divergence, it is straightforward to show that Bhat satisfies the Mode property. However, it is of interest to know how Bhat behaves as a function of a. The Bhattacharrya distance between two normal distribu- tions is</p><disp-formula id="scirp.70513-formula452"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x316.png"  xlink:type="simple"/></disp-formula><p>and hence in the special case of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x317.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x317.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x318.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.70513-formula453"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x319.png"  xlink:type="simple"/></disp-formula><p>,</p><p>Kullback-Leibler information</p><p>Kullback-Leibler divergence and Kullback-Leibler information: Recall that</p><disp-formula id="scirp.70513-formula454"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x320.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula455"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x321.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula456"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x322.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula457"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x323.png"  xlink:type="simple"/></disp-formula><p>and note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x324.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x324.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x325.png" xlink:type="simple"/></inline-formula>, and hence<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x324.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x325.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x326.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x324.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x325.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x326.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x327.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x324.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x325.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x326.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x327.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x328.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x324.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x325.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x326.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x327.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x328.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x329.png" xlink:type="simple"/></inline-formula>. Note also that I and J are f- divergences, and hence it is straightforward to show that KLinf and KLdiv satisfy the Equality and Orthogonality properties.</p><p>Outlier: Without loss of generality, let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x330.png" xlink:type="simple"/></inline-formula>. Then, for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x330.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x331.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x330.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x331.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x332.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.70513-formula458"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x333.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula459"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x334.png"  xlink:type="simple"/></disp-formula><p>for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x335.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x335.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x336.png" xlink:type="simple"/></inline-formula>, and hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x335.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x336.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x337.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x335.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x336.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x337.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x338.png" xlink:type="simple"/></inline-formula> satisfy the Outlier property.</p><p>Noise: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x339.png" xlink:type="simple"/></inline-formula>. Then, for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x339.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x340.png" xlink:type="simple"/></inline-formula>, there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x339.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x340.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x341.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.70513-formula460"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x342.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70513-formula461"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x343.png"  xlink:type="simple"/></disp-formula><p>and hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x344.png" xlink:type="simple"/></inline-formula>does not satisfy the Noise property. However, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x344.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x345.png" xlink:type="simple"/></inline-formula>satisfies the Noise property.</p><p>Mode: Since both <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x346.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x346.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x347.png" xlink:type="simple"/></inline-formula> are f-divergences, it is straightforward to show that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x346.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x347.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x348.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x346.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x347.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x348.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x349.png" xlink:type="simple"/></inline-formula> satisfy the Mode property. However, it is of interest to know how the dissimilarity measures behave as a function of a. The Kullback-Leibler information between two normal distributions is</p><disp-formula id="scirp.70513-formula462"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x350.png"  xlink:type="simple"/></disp-formula><p>and hence in the special case of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x351.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x351.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x352.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.70513-formula463"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x353.png"  xlink:type="simple"/></disp-formula><p>which result in</p><disp-formula id="scirp.70513-formula464"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x354.png"  xlink:type="simple"/></disp-formula><p>,</p>Appendix B<p>The probability density functions displayed in <xref ref-type="fig" rid="fig4">Figure 4</xref> are Gaussian mixtures,</p><disp-formula id="scirp.70513-formula465"><graphic  xlink:href="http://html.scirp.org/file/3-7403126x355.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x356.png" xlink:type="simple"/></inline-formula> is a Gaussian distribution with mean <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x356.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x357.png" xlink:type="simple"/></inline-formula> and variance<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x356.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x357.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x358.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x356.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x357.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x358.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x359.png" xlink:type="simple"/></inline-formula>. In the hybrid clustering context we have the following scenario: The coloured lines represent the current subclusters and the next step is to merge the two subclusters with lowest dissimilarity. The figures illustrate the relevance of the pro- posed properties.</p><p>(a) The distribution consists of three components with equal variance, but different component weights. We have that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x360.png" xlink:type="simple"/></inline-formula>, and therefore <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x360.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x361.png" xlink:type="simple"/></inline-formula> for any f-divergence independent of component weights, e.g. the (original) Bhattach- aryya distance and the (original) Kullback-Leibler information. This is due to the fourth f-property, and also applies for other dissimilarity measures that fulfil this property. From left to right:</p><p>Blue: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x362.png" xlink:type="simple"/></inline-formula></p><p>Red: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x363.png" xlink:type="simple"/></inline-formula></p><p>Green: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x364.png" xlink:type="simple"/></inline-formula></p><p>(b) The distribution consists of three components, where one of the components is small and near orthogonal to the others. Orthogonality can be achieved by increasing the distance between the means, by reducing the variance, or by decreasing the size of the smallest component. In this example, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x365.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x365.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x366.png" xlink:type="simple"/></inline-formula>, which is consistent with their violation of the Outlier property (see Section 3.2 and <xref ref-type="table" rid="table1">Table 1</xref>). This is true for any dissimilarity measure that fulfils the Orthogonality property but violates the Outlier property, as the size of the smallest component approaches zero. From left to right:</p><p>Blue: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x367.png" xlink:type="simple"/></inline-formula></p><p>Red: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x368.png" xlink:type="simple"/></inline-formula></p><p>Green: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x369.png" xlink:type="simple"/></inline-formula></p><p>(c) The distribution consists of four components, where the background noise consists of two components. In this example, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x370.png" xlink:type="simple"/></inline-formula>, which is consistent with the violation of the Noise property (see Section 3.2 and <xref ref-type="table" rid="table1">Table 1</xref>). This is true for any dissimilarity measure that violates the Noise property, as the maximum of the noise density approaches zero, in this example, e.g., by increasing the variances of the two noise components.</p><p>Blue: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x371.png" xlink:type="simple"/></inline-formula></p><p>Red: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x372.png" xlink:type="simple"/></inline-formula></p><p>Green: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x373.png" xlink:type="simple"/></inline-formula></p><p>(d) The distribution consists of three components, where two of them have equal mean but unequal variance. In this example, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x374.png" xlink:type="simple"/></inline-formula>but<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x374.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x375.png" xlink:type="simple"/></inline-formula>. Both fulfil the Mode property, but they behave different as a function of a, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x374.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x375.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x376.png" xlink:type="simple"/></inline-formula> (see Appendix A).</p><p>Blue: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x377.png" xlink:type="simple"/></inline-formula></p><p>Red: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x378.png" xlink:type="simple"/></inline-formula></p><p>Green: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x379.png" xlink:type="simple"/></inline-formula></p><p>(e) The distribution consists of four components, where the green and the pink component are identical, and therefore only the pink line is visible. In this example, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x380.png" xlink:type="simple"/></inline-formula>, which is consistent with SE violating the Equality property (see Section 3.2 and <xref ref-type="table" rid="table1">Table 1</xref>).</p><p>Blue: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x381.png" xlink:type="simple"/></inline-formula></p><p>Red: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x382.png" xlink:type="simple"/></inline-formula></p><p>Green: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x383.png" xlink:type="simple"/></inline-formula></p><p>Pink: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x384.png" xlink:type="simple"/></inline-formula></p><p>(f) This distribution consists of four components, where three of the components have the same weights, and are small relative to the first component. In this example<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x385.png" xlink:type="simple"/></inline-formula>, and illustrates that a dissimilarity measure should be a function of the absolute values of the component weights, not only the pairwise relative weights.</p><p>Blue: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x386.png" xlink:type="simple"/></inline-formula></p><p>Red: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x387.png" xlink:type="simple"/></inline-formula></p><p>Green: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x388.png" xlink:type="simple"/></inline-formula></p><p>Pink: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x389.png" xlink:type="simple"/></inline-formula></p>Appendix C<p>The following six distributions with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x390.png" xlink:type="simple"/></inline-formula> clusters in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x390.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x391.png" xlink:type="simple"/></inline-formula> or <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x390.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x391.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x392.png" xlink:type="simple"/></inline-formula> dimensions are used. In the following, we list the parameters with a brief description along with different distributions.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x393.png" xlink:type="simple"/></inline-formula>: The location vector.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x394.png" xlink:type="simple"/></inline-formula>: The scatter matrix.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x395.png" xlink:type="simple"/></inline-formula>: The degrees of freedom.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x396.png" xlink:type="simple"/></inline-formula>: The scale parameter.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x397.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x397.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x398.png" xlink:type="simple"/></inline-formula>: The parameters of a uniform distribution.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x399.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x399.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x400.png" xlink:type="simple"/></inline-formula>: The parameters of multivariate Gamma distribution parameters (see [<xref ref-type="bibr" rid="scirp.70513-ref50">50</xref>] for details).</p><p>When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x401.png" xlink:type="simple"/></inline-formula>, only the values corresponding to the first two dimensions are used. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x401.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x402.png" xlink:type="simple"/></inline-formula>is the identity matrix of d dimensions.</p><p>1) Student’s t (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x403.png" xlink:type="simple"/></inline-formula>):<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x403.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x404.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x403.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x404.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x405.png" xlink:type="simple"/></inline-formula>.</p><p>2) Cauchy:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x406.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x406.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x407.png" xlink:type="simple"/></inline-formula>.</p><p>3) Uniform:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x408.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x408.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x409.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x408.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x409.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x410.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x408.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x409.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x410.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x411.png" xlink:type="simple"/></inline-formula>.</p><p>4) Gamma:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x412.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x412.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x413.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x412.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x413.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x414.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x412.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x413.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x414.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x415.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x412.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x413.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x414.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x415.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x416.png" xlink:type="simple"/></inline-formula>.</p><p>5) Gaussian with uniform noise:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x417.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x417.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x418.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x417.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x418.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x419.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x417.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x418.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x419.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x420.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x417.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x418.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x419.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x420.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x421.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x417.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x418.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x419.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x420.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x421.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x422.png" xlink:type="simple"/></inline-formula>.</p><p>6) Gaussian-Laplace mixture: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x424.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x424.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x423.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x424.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x423.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x425.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x424.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x423.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x425.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x426.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x424.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x423.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x425.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x426.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x427.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x424.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x423.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x425.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x426.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x427.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x428.png" xlink:type="simple"/></inline-formula>.</p><p>The three clusters have sample size <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x429.png" xlink:type="simple"/></inline-formula> (small) and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x429.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x430.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x429.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x430.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x431.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x429.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x430.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x431.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x432.png" xlink:type="simple"/></inline-formula> (large). Because the integrals cannot be solved analytically, we used importance sampling from the fitted GMM with 100,000 samples. For the GMM fitting, we used the following parameters: number of repetitions = 10; maximum number of iterations = 1000; number of components =<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x429.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x430.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x431.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x432.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403126x433.png" xlink:type="simple"/></inline-formula>; starting points: randomly selected observations. 10<sup>−6</sup> was added to the dia- gonal of the covariance matrices to ensure that they are positive-definite.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.70513-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Hastie, T., Tibshirani, R. and Friedman, J. 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