<?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.2014.518275</article-id><article-id pub-id-type="publisher-id">AM-51052</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Soft Image Segmentation Based on the Mixture of Gaussians and the Phase-Transition Theory
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>elia</surname><given-names>A. Z. Barcelos</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yunmei</surname><given-names>Chen</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fuhua</surname><given-names>Chen</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff3"><addr-line>Department of Natural Science &amp;amp; Mathematics, West Liberty University, West Liberty, WV, USA</addr-line></aff><aff id="aff1"><addr-line>Faculty of Mathematics, Federal University of Uberlandia, Uberlandia, MG, Brazil</addr-line></aff><aff id="aff2"><addr-line>Department of Mathematics, University of Florida, Gainesville, FL, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>celiazb@ufu.br(EAZB)</email>;<email>yun@math.ufl.edu(YC)</email>;<email>fuhua.chen@westliberty.edu(FC)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>30</day><month>10</month><year>2014</year></pub-date><volume>05</volume><issue>18</issue><fpage>2888</fpage><lpage>2898</lpage><history><date date-type="received"><day>24</day>	<month>July</month>	<year>2014</year></date><date date-type="rev-recd"><day>28</day>	<month>August</month>	<year>2014</year>	</date><date date-type="accepted"><day>15</day>	<month>September</month>	<year>2014</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>
 
 
  In this paper, we propose a new soft multi-phase segmentation model where it is assumed that the pixel intensities are distributed as a Gaussian mixture. The model is formulated as a minimization problem through the use of the maximum likelihood estimator and phase-transition theory. The mixture coefficients, which are estimated using a spatially varying mean and variance procedure, are used for image segmentation. The experimental results indicate the effectiveness of the method.
 
</p></abstract><kwd-group><kwd>Image Segmentation</kwd><kwd> Variational Model</kwd><kwd> Gaussian Mixture</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Image segmentation is one of the most extensively studied problems in image processing and computer vision. Many different approaches have been proposed for the partitioning of images based on a variety of criteria including brightness (intensity), color, or texture. In general the partitioning of an image or detection of edges is under the assumption that an image consists of several patterns, and each point on the image domain belongs exclusively to only one pattern. Finding boundaries separating the different patterns in this sense is called a hard segmentation. Different to hard segmentation, soft segmentation assumes that each point may belong to more than one pattern. The goal of soft segmentation is to find all the probabilities that each pixel can belong to each pattern. This probability is also called membership (or ownership) in the literature.</p><p>One of the most extensively studied approaches for hard segmentation is the variational method. Many effective variational models have been developed, for instance, the Mumford-Shah model [<xref ref-type="bibr" rid="scirp.51052-ref1">1</xref>] , geodesic active contour [<xref ref-type="bibr" rid="scirp.51052-ref2">2</xref>] , geodesic active region [<xref ref-type="bibr" rid="scirp.51052-ref3">3</xref>] , and region competition [<xref ref-type="bibr" rid="scirp.51052-ref4">4</xref>] . Level set technique [<xref ref-type="bibr" rid="scirp.51052-ref5">5</xref>] has been proven to be powerful in the implementation of variational models. In two-phase segmentation the composition of the Heaviside function with the level set function is used to represent the regions of the object and background. In [<xref ref-type="bibr" rid="scirp.51052-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.51052-ref7">7</xref>] , the authors extended the level set method to multiphase segmentation by using multiple level set functions, while in [<xref ref-type="bibr" rid="scirp.51052-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.51052-ref9">9</xref>] , the authors proposed another means to extend the level set method by using multiple layers for each level set function. Through the act of carefully choosing the initial values, these methods can work very well. However, the non-convexity of the energy functional in the level set formulation is an inherent drawback of the level set method. As a result, many level set based variational segmentation models are sensitive to initial values and may converge to an undesirable local minimum. This problem is more difficult to deal with for multiphase segmentation.</p><p>To overcome the non-convexity problem mentioned above, one approach is to replace the composition of the heaviside function with the level set function in level set formulation by use of a weight/membership function. Through the implementation of this modification the energy is convex with respect to the membership function. For example, Chan et al. [<xref ref-type="bibr" rid="scirp.51052-ref10">10</xref>] and Bresson et al. [<xref ref-type="bibr" rid="scirp.51052-ref11">11</xref>] stated certain non-convex minimization problems for image segmentation and denosing as equivalent convex minimization problems by using membership functions to replace characteristic functions. These new models allow for the finding of global minimizers via standard convex minimization schemes. In particular in [<xref ref-type="bibr" rid="scirp.51052-ref11">11</xref>] efficient and fast numerical schemes to globally minimize the variational segmentation models were proposed. These algorithms are based on a dual formulation of the TV norm proposed and developed in [<xref ref-type="bibr" rid="scirp.51052-ref12">12</xref>] -[<xref ref-type="bibr" rid="scirp.51052-ref16">16</xref>] .</p><p>Soft segmentation is also motivated by its applications to real world problems. In medical imaging, due to limited spacial resolution of the equipment, not all the voxels in a segmented region contain the same tissue type, especially near the boundary of two subregions. A typical example is the partial volume effect in MRI brain image segmentation. Instead of labeling each image voxel with a unique tissue type [<xref ref-type="bibr" rid="scirp.51052-ref17">17</xref>] , partial volume segmentation aims at estimating the percentage of each voxel belonging to each tissue, which can be viewed as the probability of the voxel belonging to the tissue. Since soft segmentation allows each pixel to belong to several patterns with certain probabilities, it provides a more flexible mechanism, and thereby keeps more options available for post-processing steps.</p><p>There have been many soft segmentation methods. Mory and Ardon extended the original region competition model [<xref ref-type="bibr" rid="scirp.51052-ref4">4</xref>] to a fuzzy region competition method [<xref ref-type="bibr" rid="scirp.51052-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.51052-ref19">19</xref>] . The technique generalizes some existing supervised and unsupervised region-based model. The proposed functional is convex, which guarantees the global solution in the supervised case. Unfortunately, this method only applies to two-phase segmentation and is difficult to extend to multiphase segmentation. The fuzzy C-mean (FCM) [<xref ref-type="bibr" rid="scirp.51052-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.51052-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.51052-ref21">21</xref>] is a method developed for pattern classification and recognition. Hence it is also applicable to image segmentation. The standard FCM model</p><p>partitions a data set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x6.png" xlink:type="simple"/></inline-formula> into <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x7.png" xlink:type="simple"/></inline-formula> clusters by the following objective function [<xref ref-type="bibr" rid="scirp.51052-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.51052-ref23">23</xref>]</p><disp-formula id="scirp.51052-formula1961"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x8.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x9.png" xlink:type="simple"/></inline-formula> is the membership value of datum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x10.png" xlink:type="simple"/></inline-formula> for class <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x11.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x12.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x13.png" xlink:type="simple"/></inline-formula> stands for the</p><p>cluster centers. The original FCM method is very sensitive to noise. An adaptive fuzzy c-means (AFCM) was proposed by Pham et al. [<xref ref-type="bibr" rid="scirp.51052-ref21">21</xref>] , where the constant cluster centers used in the FCM model are substituted by spatially varying functions. The energy functional can be written as</p><disp-formula id="scirp.51052-formula1962"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x14.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x15.png" xlink:type="simple"/></inline-formula> is the bias field and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x16.png" xlink:type="simple"/></inline-formula> is the regularization term for the bias field<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x17.png" xlink:type="simple"/></inline-formula>. AFCM is more robust to noise than the standard FCM. The soft segmentation model developed in [<xref ref-type="bibr" rid="scirp.51052-ref17">17</xref>] used a different similarity measure to that in [<xref ref-type="bibr" rid="scirp.51052-ref21">21</xref>] . Their objective functional reads as</p><disp-formula id="scirp.51052-formula1963"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x18.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.51052-formula1964"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x19.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x20.png" xlink:type="simple"/></inline-formula>stands for the set of neighbors falling into a window around<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x21.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x22.png" xlink:type="simple"/></inline-formula> is its cardinality. The parame-</p><p>ter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x23.png" xlink:type="simple"/></inline-formula> in the second term controls the effect of the penalty.</p><p>Another class of soft segmentation is based on stochastic approaches. It considers that pixel intensities are independent samples from one or several distributions. The likelihood functions have been widely used in soft segmentation. In [<xref ref-type="bibr" rid="scirp.51052-ref24">24</xref>] the maximum-likelihood (ML) is used to find the optimal parameters in the joint pdf such that the likelihood function is maximized. An expectation-maximization (EM) algorithm is used to solve the problem when we are dealing with incomplete data. However, simply using likelihood to model an image is not enough since it ignored the prior knowledge of an image. In [<xref ref-type="bibr" rid="scirp.51052-ref25">25</xref>] the authors proposed an adaptive segmentation method that uses the knowledge of tissue properties and intensity inhomogeneities to correct and segment MR images. The EM algorithm was used to iteratively estimate the posterior tissue class probabilities when the bias field is known, and having a maximum a posteriori principle (MAP) estimator of the bias field, when tissue class probabilities are known.</p><p>In [<xref ref-type="bibr" rid="scirp.51052-ref20">20</xref>] , a segmentation framework based on the MAP principle was proposed for partial volume (PV) segmentation of magnetic resonance brain images. A mixture of the probability density functions is considered to address the PV effect. A Markov Random Field (MRF) model is used to define the prior distribution of the mixture coefficient field imposing a smoothness on the mixture coefficients (ownerships). The fuzzy c-means model is extended to define the likelihood function of the observed image.</p><p>The phase transition theory in material sciences and fluid mechanics have inspired people to borrow ideas from contemporary material sciences, e.g., the diffuse interface model of Cahn-Hilliard [<xref ref-type="bibr" rid="scirp.51052-ref26">26</xref>] , and its rigorous mathematical analysis in the framework of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x24.png" xlink:type="simple"/></inline-formula>-convergence approximation by Modica and Mortola [<xref ref-type="bibr" rid="scirp.51052-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.51052-ref28">28</xref>] into image segmentation. The phase field relaxation consists of approximating the perimeter of the interface using a Cahn-Hilliard type penalization functional [<xref ref-type="bibr" rid="scirp.51052-ref26">26</xref>] , with the form</p><disp-formula id="scirp.51052-formula1965"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x25.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x26.png" xlink:type="simple"/></inline-formula> is a scalar function with exactly two minimizers at 0 and 1 satisfying</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x27.png" xlink:type="simple"/></inline-formula>. The second term of the penalty functional ensures that the values of the material density <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x28.png" xlink:type="simple"/></inline-formula></p><p>converges to 0 or 1 as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x29.png" xlink:type="simple"/></inline-formula>, while the first term controls the perimeter. The parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x30.png" xlink:type="simple"/></inline-formula> can be interpreted as the width of the diffused edge representation in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x31.png" xlink:type="simple"/></inline-formula>. The phase field approach has been used in topological optimization problems [<xref ref-type="bibr" rid="scirp.51052-ref29">29</xref>] -[<xref ref-type="bibr" rid="scirp.51052-ref31">31</xref>] . In [<xref ref-type="bibr" rid="scirp.51052-ref32">32</xref>] , the authors used the phase field to approximate sharp edges and a variational phase field model is derived to compute a shape average of a given number of shapes. In [<xref ref-type="bibr" rid="scirp.51052-ref30">30</xref>] , the authors used the phase transition theory in a Cahn-Hilliard impainting model. The authors in [<xref ref-type="bibr" rid="scirp.51052-ref33">33</xref>] and [<xref ref-type="bibr" rid="scirp.51052-ref34">34</xref>] presented a models for image segmentation based upon the phase transition theory of Modica and Mortola and discussed theirs connections to the Mumford-Shah segmentation model and some related works.</p><p>In paper [<xref ref-type="bibr" rid="scirp.51052-ref35">35</xref>] , J. Shen proposed a general multiphase stochastic variational fuzzy segmentation model combining the stochastic principle and the Modica-Mortola’s phase-transition theory. The image <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x32.png" xlink:type="simple"/></inline-formula> is defined on an open bounded domain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x33.png" xlink:type="simple"/></inline-formula> and is assumed that it can be composed of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x34.png" xlink:type="simple"/></inline-formula> unknown patterns. Let</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x35.png" xlink:type="simple"/></inline-formula>be the pattern label variable,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x36.png" xlink:type="simple"/></inline-formula>. At each voxel<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x37.png" xlink:type="simple"/></inline-formula>, both <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x38.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x39.png" xlink:type="simple"/></inline-formula> are</p><p>viewed as independent random variables indexed by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x40.png" xlink:type="simple"/></inline-formula>. The probability that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x41.png" xlink:type="simple"/></inline-formula> belongs to the i-th pattern, i.e.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x42.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x43.png" xlink:type="simple"/></inline-formula>is represented by the ownership functions<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x44.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x45.png" xlink:type="simple"/></inline-formula>.</p><p>Denote by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x46.png" xlink:type="simple"/></inline-formula> the probability density function (pdf) of the random variable <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x47.png" xlink:type="simple"/></inline-formula></p><p>belonging to the i-th pattern. Then the pdf of the image <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x48.png" xlink:type="simple"/></inline-formula> at each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x49.png" xlink:type="simple"/></inline-formula> is a mixed distribution given by</p><disp-formula id="scirp.51052-formula1966"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x50.png"  xlink:type="simple"/></disp-formula><p>Under the assumption that all random variables are independent, we have the following joint pdf</p><disp-formula id="scirp.51052-formula1967"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x51.png"  xlink:type="simple"/></disp-formula><p>The regularization is made using a double well potential borrowed from the phase-transition theory. By assuming that all patterns are Gaussian distributions with mean fields <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x52.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x53.png" xlink:type="simple"/></inline-formula>, and a fixed variance<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x54.png" xlink:type="simple"/></inline-formula>, the pdf of the mixed Gaussian is given by</p><disp-formula id="scirp.51052-formula1968"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x55.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.51052-formula1969"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x56.png"  xlink:type="simple"/></disp-formula><p>defines the Gaussian probability density function, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x57.png" xlink:type="simple"/></inline-formula>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x58.png" xlink:type="simple"/></inline-formula>The model is to solve the following minimization problem:</p><disp-formula id="scirp.51052-formula1970"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x59.png"  xlink:type="simple"/></disp-formula><p>with constraints</p><disp-formula id="scirp.51052-formula1971"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x60.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x61.png" xlink:type="simple"/></inline-formula> are the ownerships and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x62.png" xlink:type="simple"/></inline-formula> are called patterns. Unlike the original Mumford Shah model, the energy of each channel is defined on the entire domain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x63.png" xlink:type="simple"/></inline-formula> instead of on a specific subregion<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x64.png" xlink:type="simple"/></inline-formula>. In [<xref ref-type="bibr" rid="scirp.51052-ref36">36</xref>] the authors introduced a functional with a variable exponent into the Shen's model which provides a more accurate model for image segmentation and denoising.</p><p>In this paper, we propose a new multiphase soft segmentation model that integrates phase-transition theory into a mixture of Gaussian model for image intensities. The proposed model is an extension of the paper [<xref ref-type="bibr" rid="scirp.51052-ref35">35</xref>] .</p><p>The difference between this work and [<xref ref-type="bibr" rid="scirp.51052-ref35">35</xref>] lies in the facts: i) the data fidelity term in the proposed model is a Gaussian mixture model, while the model in [<xref ref-type="bibr" rid="scirp.51052-ref35">35</xref>] is only an approximation of Gaussian mixture model due to simplification. Although this simplification facilitates the numerical computation it does not reflect upon the real behavior of the data; ii) paper [<xref ref-type="bibr" rid="scirp.51052-ref35">35</xref>] assumed that all the variances of different phases are the same and fixed, while in the proposed model each phase could have a different variance which will also be optimized, making the model more flexible and more robust.</p><p>This paper is organized as follows: Section 2 addresses the proposed model development. Section 3 presents the implementation details and experimental results. Finally, the conclusion is given in section 4.</p></sec><sec id="s2"><title>2. Proposed Model</title><p>In this section, we develop a soft multiphase segmentation model under the assumption that the intensity of the image is distributed as a mixture of Gaussians.</p><p>We assume the intensity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x65.png" xlink:type="simple"/></inline-formula> at each point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x66.png" xlink:type="simple"/></inline-formula> is an independent sample from a mixed Gaussian distribution with probability<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x67.png" xlink:type="simple"/></inline-formula>. Considering the Equations (6, 7, 8 and 9) the goal of the soft segmentation</p><p>is to estimate the optimal vectorial pair of ownerships <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x68.png" xlink:type="simple"/></inline-formula> and patterns<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x69.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.51052-formula1972"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x70.png"  xlink:type="simple"/></disp-formula><p>Through the Bayesian formula, the posterior given <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x71.png" xlink:type="simple"/></inline-formula> is obtained by</p><disp-formula id="scirp.51052-formula1973"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x72.png"  xlink:type="simple"/></disp-formula><p>assuming that the mixture patterns <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x73.png" xlink:type="simple"/></inline-formula> and the mixture rules <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x74.png" xlink:type="simple"/></inline-formula> are independent. Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x75.png" xlink:type="simple"/></inline-formula> is given, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x76.png" xlink:type="simple"/></inline-formula>is constant. So, the Bayesian based optimal problem becomes</p><disp-formula id="scirp.51052-formula1974"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x77.png"  xlink:type="simple"/></disp-formula><p>By taking the logarithmic likelihood<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x78.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.51052-formula1975"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x79.png"  xlink:type="simple"/></disp-formula><p>As assumed, all the samples <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x80.png" xlink:type="simple"/></inline-formula> are independently Gaussian distributed. So, we have</p><disp-formula id="scirp.51052-formula1976"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x81.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.51052-formula1977"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x82.png"  xlink:type="simple"/></disp-formula><p>For energies<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x83.png" xlink:type="simple"/></inline-formula>, we use the general variational form, and assume that all pattern channels are inde- pendent to each other. For functions whose gradients are square integrable, we may consider:</p><disp-formula id="scirp.51052-formula1978"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x84.png"  xlink:type="simple"/></disp-formula><p>Finally, for energy<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x85.png" xlink:type="simple"/></inline-formula>, we borrow the expression from paper [<xref ref-type="bibr" rid="scirp.51052-ref35">35</xref>] based on material science and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x86.png" xlink:type="simple"/></inline-formula>-</p><p>convergence theory.</p><disp-formula id="scirp.51052-formula1979"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x87.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x88.png" xlink:type="simple"/></inline-formula>. Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x89.png" xlink:type="simple"/></inline-formula>, the second term will force <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x90.png" xlink:type="simple"/></inline-formula> approximate either 1 or 0. The first term is the regularity condition on each<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x91.png" xlink:type="simple"/></inline-formula>. The advantage of this expression is that it contains the boundary information. By <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x92.png" xlink:type="simple"/></inline-formula>-convergence theory, the term converges to the length of the boundary in the sense of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x93.png" xlink:type="simple"/></inline-formula>-convergence [<xref ref-type="bibr" rid="scirp.51052-ref37">37</xref>] [<xref ref-type="bibr" rid="scirp.51052-ref38">38</xref>] as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x94.png" xlink:type="simple"/></inline-formula> goes to zero.</p><p>Now, in combination of (15), (16), (18) and (19), the final proposed segmentation model is the minimization of:</p><disp-formula id="scirp.51052-formula1980"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x95.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x96.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x97.png" xlink:type="simple"/></inline-formula> are weights balancing the effects of the three terms.</p></sec><sec id="s3"><title>3. Implementation and Experimental Results</title><p>Since the energy functional contains three group parameters, in order to minimize the energy, we use the alternating iteration scheme:</p><disp-formula id="scirp.51052-formula1981"><graphic  xlink:href="http://html.scirp.org/file/5-7402210x98.png"  xlink:type="simple"/></disp-formula><p>Each group parameter can be iterated with its Euler-Lagrange equation. The Euler-Lagrange equation for patterns<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x99.png" xlink:type="simple"/></inline-formula>, ownerships <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x100.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x101.png" xlink:type="simple"/></inline-formula> are as follows:</p><disp-formula id="scirp.51052-formula1982"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x102.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51052-formula1983"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x103.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51052-formula1984"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x104.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x105.png" xlink:type="simple"/></inline-formula> is defined as</p><disp-formula id="scirp.51052-formula1985"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x106.png"  xlink:type="simple"/></disp-formula><p>Considering that</p><disp-formula id="scirp.51052-formula1986"><graphic  xlink:href="http://html.scirp.org/file/5-7402210x107.png"  xlink:type="simple"/></disp-formula><p>and since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x108.png" xlink:type="simple"/></inline-formula> and so<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x109.png" xlink:type="simple"/></inline-formula>.</p><p>We can solve the equations (21)-(23) using the flow from their associated Euler-Lagrange equations. The flow equation for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x110.png" xlink:type="simple"/></inline-formula> is given by:</p><disp-formula id="scirp.51052-formula1987"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x111.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51052-formula1988"><graphic  xlink:href="http://html.scirp.org/file/5-7402210x112.png"  xlink:type="simple"/></disp-formula><p>The flow equations for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x113.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x114.png" xlink:type="simple"/></inline-formula> are obtained similarly.</p><p>The numerical solution was obtained using finite differences to discretize the flow equations. For the numerical implementation it is supposed that the images are represented by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x115.png" xlink:type="simple"/></inline-formula> matrices of intensity values. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x116.png" xlink:type="simple"/></inline-formula> denote the value of the image <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x117.png" xlink:type="simple"/></inline-formula> at pixel <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x118.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x119.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x120.png" xlink:type="simple"/></inline-formula>. The flow equations obtain images at scales, or times, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x121.png" xlink:type="simple"/></inline-formula>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x122.png" xlink:type="simple"/></inline-formula> is the step size for equation (25).</p><p>We denote <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x123.png" xlink:type="simple"/></inline-formula> by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x124.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.51052-formula1989"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x125.png"  xlink:type="simple"/></disp-formula><p>Following the same procedure for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x126.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x127.png" xlink:type="simple"/></inline-formula>, we have:</p><disp-formula id="scirp.51052-formula1990"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x128.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51052-formula1991"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x129.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x130.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x131.png" xlink:type="simple"/></inline-formula> are the step sizes for Equations (27) and (28), respectively,</p><p>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x132.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x133.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x134.png" xlink:type="simple"/></inline-formula> are given by:</p><disp-formula id="scirp.51052-formula1992"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x135.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51052-formula1993"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x136.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51052-formula1994"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-7402210x137.png"  xlink:type="simple"/></disp-formula><p>To start the iteration process, we need to choose the initial values for the ownership functions<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x138.png" xlink:type="simple"/></inline-formula>, the patterns <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x139.png" xlink:type="simple"/></inline-formula> and the standard deviations<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x140.png" xlink:type="simple"/></inline-formula>. We also need to choose suitable parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x141.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x142.png" xlink:type="simple"/></inline-formula>. The</p><p>adopted procedures is: given<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x143.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x144.png" xlink:type="simple"/></inline-formula>, we take <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x145.png" xlink:type="simple"/></inline-formula> if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x145.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x146.png" xlink:type="simple"/></inline-formula> and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-7402210x147.png" xlink:type="simple"/></inline-formula>if,.</p><p>In <xref ref-type="fig" rid="fig1">Figure 1</xref>, a comparison was made between Shen’s model and the proposed model using synthetic images. <xref ref-type="fig" rid="fig1">Figure 1</xref>(a) is the original image, which is a piecewise constant image added with constant Gaussian noise. <xref ref-type="fig" rid="fig1">Figure 1</xref>(b) and <xref ref-type="fig" rid="fig1">Figure 1</xref>(c) are the reconstructed images using the proposed model after 10 iterations and 50 iterations resp., while <xref ref-type="fig" rid="fig1">Figure 1</xref>(d) to <xref ref-type="fig" rid="fig1">Figure 1</xref>(f) are the images reconstructed using Shen’s model after 50 iterations, 100 iterations and 500 iterations, respectively. We see that the result was improved using the pro- posed model with few iterations. However, when Shen’s model is used very little differences is perceived even when the number of iterations are increased.</p><p>In <xref ref-type="fig" rid="fig2">Figure 2</xref>, we present a comparison between variances updated and not updated. The original image <xref ref-type="fig" rid="fig2">Figure 2</xref>(a) is a piecewise constant image added with different Gaussian noise for different phases. <xref ref-type="fig" rid="fig2">Figure 2</xref>(b) is the reconstructed image when variances are not updated, and <xref ref-type="fig" rid="fig2">Figure 2</xref>(c) is the reconstructed image when variances are updated. <xref ref-type="fig" rid="fig2">Figure 2</xref>(d), <xref ref-type="fig" rid="fig2">Figure 2</xref>(f) are three membership functions obtained with variances not updated, while Figures 2(g)-(i) are three membership functions obtained with variances updated.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> shows the bias correction in the proposed model when bias is evident prior to correction in an image. <xref ref-type="fig" rid="fig3">Figure 3</xref>(a) is the original image. This image was firstly used by X. Bresson and T.F. Chan in their non-local Chan-Vese model [<xref ref-type="bibr" rid="scirp.51052-ref6">6</xref>] . It is clear that the object (disk) in <xref ref-type="fig" rid="fig3">Figure 3</xref>(a) is biased. <xref ref-type="fig" rid="fig3">Figure 3</xref>(b) and <xref ref-type="fig" rid="fig3">Figure 3</xref>(c) are the membership functions obtained using Shen’s model, while <xref ref-type="fig" rid="fig3">Figure 3</xref>(d) and <xref ref-type="fig" rid="fig3">Figure 3</xref>(e) are the corre- sponding membership functions obtained using the proposed model by setting different variances in the implementation.</p><p>In the following experiments, we tested our model on real images. In <xref ref-type="fig" rid="fig4">Figure 4</xref>, we carried out the experiment on the MRI brain image. <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) presents the original brain image; Figures 4(b)-(d) are ownerships of white matter, gray matter and CSF, respectively. <xref ref-type="fig" rid="fig4">Figure 4</xref>(e) is the reconstructed image; Figures 4(f)-(h) are patterns of the three matters. <xref ref-type="fig" rid="fig5">Figure 5</xref> shows a similar result but with natural scene image.</p><p>Finally, we take the experiment on a color image, as shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>, where <xref ref-type="fig" rid="fig6">Figure 6</xref>(a) is the original image; Figures 6(b)-(d) are three phases.</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Comparison between Shen’s model and proposed model using synthetic image.</title></caption><fig id ="fig1_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-7402210x151.png"/></fig><fig id ="fig1_2"><label> (c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-7402210x150.png"/></fig></fig-group><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Comparison between variances updated and not updated</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-7402210x152.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Comparison between Shen’s model and proposed model using biased image</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-7402210x153.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> (a) Original brain image; (b)-(d) Ownerships of white matter, gray matter and CSF; (e) Reconstructed image; (f)-(h) Patterns of white matter, gray matter and CSF</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-7402210x154.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> (a) Original natural image; (b)-(d) Ownerships of different phases; (e) Recon-structed image; (f)-(h) Patterns of different phases</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-7402210x155.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Experimental result on color image after 300 iterations</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-7402210x156.png"/></fig></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper, we extended the idea in paper [<xref ref-type="bibr" rid="scirp.51052-ref35">35</xref>] and developed a soft multiphase segmentation model. The model is a pure Gaussian mixture model. It allows for the choosing of different means and different variances, which leads to a more flexible model. The experiments show that the model is more robust to noise compared with the previous model. Moreover, with the experiment on MRI brain image, we see the advantage of soft segmentation where we can find and calculate partial volume which is very important for brain image segmen- tation.</p></sec><sec id="s5"><title>Acknowledgements</title><p>C.A.Z. Barcelos is partially supported by CNPq-Conselho Nacional de Desenvolvimento Científico e Tec- nológico; Y. Chen is partially supported by NSF grants IIP-1237814 and DMS-1319050.</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.51052-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Mumford, D. and Shah, J. (1989) Optimal Approximations by Piecewise Smooth Functions and Associated Variational Problems. Communications on Pure and Applied Mathematics, 42, 577-685. http://dx.doi.org/10.1002/cpa.3160420503</mixed-citation></ref><ref id="scirp.51052-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Caselles, V., Kimmel, R. and Sapiro, G. (1997) Geodesic Active Contours. International Journal of Computer Vision, 1, 61-79. http://dx.doi.org/10.1023/A:1007979827043</mixed-citation></ref><ref id="scirp.51052-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Paragios, N. and Deriche, R. 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