<?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">ASM</journal-id><journal-title-group><journal-title>Advances in Sexual Medicine</journal-title></journal-title-group><issn pub-type="epub">2164-5191</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/asm.2014.43008</article-id><article-id pub-id-type="publisher-id">ASM-48206</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>MEDICINE &amp; HEALTHCARE</subject></subj-group></article-categories><title-group><article-title>Occlusion Robust Low-Contrast Sperm Tracking Using Switchable Weight Particle Filtering</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mohammadreza</surname><given-names>Ravanfar</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>Leila</surname><given-names>Azinfar</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>Mohammad</surname><given-names>Hassan Moradi</given-names></name></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Reza</surname><given-names>Fazel-Rezai</given-names></name></contrib></contrib-group><aff id="aff1"><addr-line>Amirkabir University of Technology, Tehran, Iran</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>rravanfar@yahoo.com(MR)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>07</day><month>07</month><year>2014</year></pub-date><volume>04</volume><issue>03</issue><fpage>42</fpage><lpage>54</lpage><history><date date-type="received"><day>9</day>	<month>May</month>	<year>2014</year></date><date date-type="rev-recd"><day>9</day>	<month>June</month>	<year>2014</year>	</date><date date-type="accepted"><day>10</day>	<month>July</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>
	Sperm motility analysis has a particular place in male fertility diagnosis. Computerized sperm tracking has an important role in extracting sperm trajectory and measuring sperm’s dynamic features. Due to free movements of sperms in three dimensions, occlusion has remained a challenging problem in this area. This paper aims to present a robust single sperm tracking method being able to handle misdetections in sperm occlusion scenes. In this paper, a robust method of segmentation was utilized to provide the required measurements for a switchable weight particle filtering which was designed for single sperm tracking. In each frame, the target sperm was categorized in one of these three stages: before occlusion, occlusion, and after occlusion where the occlusion had been detected based on sperm’s physical characteristics. Depending on the target sperm stage, particles were weighted differently. In order to evaluate the algorithm, two groups of samples were studied where an expert had selected a single sperm of each sample to track manually and automatically. In the first group, the sperms with no occlusion along their trajectories were tracked to depict the general compatibility of the algorithm with sperm tracking. In the second group, the algorithm was applied on the sperms which had at least one occlusion during their path. The algorithm showed an accuracy of 95% on the first group and 86.66% on the second group which illustrate the robustness of the algorithm against occlusion.<b></b>
</p></abstract><kwd-group><kwd>Sperm Tracking</kwd><kwd> Particle Filtering</kwd><kwd> Object Occlusion</kwd><kwd> Watershed Algorithm</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Human semen analysis is an important experiment in male fertility diagnosis in which morphology and dynamic characteristics of sperms are examined. The semen analysis can be performed manually or automatically. The manual semen analysis depends on the operator’s experiences and skills, and the results can be affected by human errors as well. These imperfections and the brilliant abilities of computerized methods in fast and accurate distinguishing of sperm movement have motivated researchers to develop the computerized tracking algorithms. Usually sperms are divided into four groups in terms of motility [<xref ref-type="bibr" rid="scirp.48206-ref1">1</xref>] :</p><p>1) Rapid progressive motility;</p><p>2) Slow progressive motility;</p><p>3) Non-progressive motility;</p><p>4) Immobility.</p><p>Because of free movements of sperm in semen, mathematical models cannot explain all the above categories. Moreover this diversity in sperm movements compounds the tracking problems.</p><p>From the decade of the 1980 designing sperm imaging systems, tracking algorithms, and computerized analysis became center of attention broadly and valuable works were published in this area as well [<xref ref-type="bibr" rid="scirp.48206-ref2">2</xref>] -[<xref ref-type="bibr" rid="scirp.48206-ref4">4</xref>] . Some of them dealt with supplementary tools like acoustic device [<xref ref-type="bibr" rid="scirp.48206-ref3">3</xref>] , piezo-electric device [<xref ref-type="bibr" rid="scirp.48206-ref5">5</xref>] and lens-free on-chip imaging technique [<xref ref-type="bibr" rid="scirp.48206-ref6">6</xref>] to provide 3D trajectory of sperm. Some others utilized optical tweezers to measure both sperm motility and energy [<xref ref-type="bibr" rid="scirp.48206-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.48206-ref8">8</xref>] . In [<xref ref-type="bibr" rid="scirp.48206-ref9">9</xref>] , a lens-less charge-coupled device (CCD) and a microfluidic system were used to improve field of view (FOV) of microscope and provide automatic recording of sperm.</p><p>In another aspect, it has been tried to develop algorithms in order to achieve more accurate and robust sperm trackers. Using visual evaluation of microscopic field [<xref ref-type="bibr" rid="scirp.48206-ref10">10</xref>] , template matching [<xref ref-type="bibr" rid="scirp.48206-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.48206-ref12">12</xref>] , particle and Kalman filters [<xref ref-type="bibr" rid="scirp.48206-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.48206-ref14">14</xref>] , nearest neighbor technique [<xref ref-type="bibr" rid="scirp.48206-ref15">15</xref>] , time differential method [<xref ref-type="bibr" rid="scirp.48206-ref16">16</xref>] , optimal matching [<xref ref-type="bibr" rid="scirp.48206-ref17">17</xref>] co-regis- tration process based on block matching [<xref ref-type="bibr" rid="scirp.48206-ref18">18</xref>] , high-speed visual feedback [<xref ref-type="bibr" rid="scirp.48206-ref19">19</xref>] , and optical flow [<xref ref-type="bibr" rid="scirp.48206-ref20">20</xref>] are some tracking algorithms for sperm cells employed so far.</p><p>In computer assisted sperm analysis (CASA) system, multi-object tracking algorithm with specific standards is utilized [<xref ref-type="bibr" rid="scirp.48206-ref21">21</xref>] . These systems have board applications for human and animal sperm analysis and in-vitro fertilization (IVF) as well [<xref ref-type="bibr" rid="scirp.48206-ref22">22</xref>] [<xref ref-type="bibr" rid="scirp.48206-ref23">23</xref>] . CASA systems are dealt with from a variety of angles like their capability [<xref ref-type="bibr" rid="scirp.48206-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.48206-ref24">24</xref>] , comparison of existed methods [<xref ref-type="bibr" rid="scirp.48206-ref25">25</xref>] [<xref ref-type="bibr" rid="scirp.48206-ref26">26</xref>] , accuracy and precision [<xref ref-type="bibr" rid="scirp.48206-ref27">27</xref>] [<xref ref-type="bibr" rid="scirp.48206-ref28">28</xref>] , and quantitative analysis [<xref ref-type="bibr" rid="scirp.48206-ref29">29</xref>] [<xref ref-type="bibr" rid="scirp.48206-ref30">30</xref>] . This paper attempts to improve the algorithmic approach by providing occlusion robust single sperm tracking algorithm.</p></sec><sec id="s2"><title>2. Methods and Materials</title><sec id="s2_1"><title>2.1. Object Restrictions</title><p>In this paper, the following object restrictions were assumed:</p><p>• Imaging system is source of some noises and disturbances such as the errors caused by slides, mirrors, microscope lenses, camera lenses, and ambient. It is assumed that these factors remain constant in all frames and are not affected by the sample’s or the sperm’s movements.</p><p>• The sperm can swim out of the plane of focus [<xref ref-type="bibr" rid="scirp.48206-ref31">31</xref>] . Consequently, average intensity for each sperm head changes over time.</p><p>• The sperm may occlude along its path especially, when the semen has a high concentration. In this case, the algorithm should be able to make a distinction between target sperm and the other ones.</p><p>• Directions of sperm head and movement are not necessarily the same, specially, when the sperm belongs to the first or second movement category.</p><p>• There are some local changes in background, hence it couldn’t be considered static.</p></sec><sec id="s2_2"><title>2.2. Preprocessing</title><p>In order to reduce the undesirable effects caused by imaging system, freely movement of sperm, the following preprocessing algorithms were used.</p><p>• Smoothing</p><p>Based on report of WHO [<xref ref-type="bibr" rid="scirp.48206-ref1">1</xref>] , a progressive sperm can move more than 100 μm per second. In [<xref ref-type="bibr" rid="scirp.48206-ref32">32</xref>] it is discussed that based on selected sampling rate sperm’s motility characteristics are partly different. In this paper, image acquisition was performed with 30 fps. Thus, rapid progressive sperm’s movements were unconnected to some extent. To obviate the problem, a sampled spatiotemporal Gaussian filter was utilized [<xref ref-type="bibr" rid="scirp.48206-ref33">33</xref>] :</p><disp-formula id="scirp.48206-formula1734"><label>(1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\d6cbb16b-dc93-4fbc-aced-c082cca12c1d.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\970be9f3-ab2a-48c6-bd32-749f7f4c6983.png" xlink:type="simple"/></inline-formula> is a 3 &#215; 3 covariance matrix and p = (x, y, t) denotes a pixel position (x, y) at time t. In practice, a separable kernel was used in which the standard deviation for every dimension was 1.5 and its length was 5 pixels.</p><p>• Morphological filtering</p><p>Proper use of morphological filters, gives this opportunity to employ the appearance-based information for the objects and also partly expunges undesirable cells. In addition to sperm cells, human semen includes blood cells and cytoplasmic parts. According to WHO, size of sperm head is 3 - 5 μm which is a useful constraint to seclude sperms from other types of cells [<xref ref-type="bibr" rid="scirp.48206-ref1">1</xref>] . Nonetheless, in some samples, non-sperm cells move slowly and locally which misleads motion-based segmentation methods into misdetection. In this paper, a sperm-shaped top hat filter was employed to address this problem. Size of the structure element was designed considering sperm head size.</p></sec><sec id="s2_3"><title>2.3. Background Removing</title><p>Although the morphological filtering reduces the background to some extent, some debris still appear in the images. Furthermore, the images are labeled by the camera. Therefore, a proper background removing algorithm was utilized. Because of some unwanted local slow movements, the statistical methods did not have enough proficiency. Therefore, an adaptive temporal median filter was employed to detect the background. In this method, original image was defined as sum of background and foreground as follows:</p><disp-formula id="scirp.48206-formula1735"><label>(2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\868b8a15-9c4d-40b6-a068-ded4d8d5ac83.png"/></disp-formula><disp-formula id="scirp.48206-formula1736"><label>(3)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\af84e9fa-1775-4d61-a1f9-2ab6dc4818c2.png"/></disp-formula><p>where α denotes the update constant changing in each step. I and B depict foreground (sperm objects) and background intensity respectively [<xref ref-type="bibr" rid="scirp.48206-ref34">34</xref>] . The median changes in accordance to standard deviation and length of time series in each point. Moreover, if a local ramp arises in the median, it will be modified. Finally, median measures are limited by Chebyshev constrain whose magnitude is 0.777 time of standard deviation of the data.</p></sec><sec id="s2_4"><title>2.4. Particle Filter</title><p>Generally, particle filtering is a method for estimating probability distribution. In the other words, particle filtering is a sequential Monte Carlo estimation using importance sampling method. In this method, particles are utilized for point representation of probability distribution and are allotted weights to determine the probability in each point. This is the important sampling technique which determines particle weights. To use particle filtering, it is only needed to express the problem in state space. If <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\9cfaa341-6038-402d-93bd-47437849942e.png" xlink:type="simple"/></inline-formula> is a state variable at time t, then the particles and their weights are shown as <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\276643f8-ff53-4f92-b818-d3345535d75d.png" xlink:type="simple"/></inline-formula> and posterior probability is approximated by:</p><disp-formula id="scirp.48206-formula1737"><label>(4)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\e1a286ee-d828-4765-9426-072ea8ee79a0.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\ab4c78e1-d709-40f5-a0d0-8fd5915f94fc.png" xlink:type="simple"/></inline-formula> denotes measurements. Based on the Bayesian network principal, posterior probability can be approximated by computing<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\47fbff33-cce2-47cf-a09f-700d94e700c0.png" xlink:type="simple"/></inline-formula>. Nonetheless, computing <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\59f4d591-f2d1-4979-9c8e-7fce05dde8f6.png" xlink:type="simple"/></inline-formula> is in need of solving complex integrals [<xref ref-type="bibr" rid="scirp.48206-ref35">35</xref>] . Therefore, reaching optimum solution based on approximate integrations is impracticable. Instead, importance sampling is a competent candidate to solve this problem in which a specific distribution q is used to generate random samples. Assuming chain rule and Markovian condition on the state variable <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\ba651e2f-f272-4220-94ec-62fb0b5013a2.png" xlink:type="simple"/></inline-formula> and conditional independency of<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\d77c1e8f-7995-455e-a31d-b35aa93d4479.png" xlink:type="simple"/></inline-formula>, the weights can be obtained using importance sampling as follows [<xref ref-type="bibr" rid="scirp.48206-ref35">35</xref>] :</p><disp-formula id="scirp.48206-formula1738"><label>(5)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\2469ba01-78b2-4235-a1fb-163748106cc2.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\ae360b21-7ef7-40d0-ade6-7de4d4ed7bc7.png" xlink:type="simple"/></inline-formula>. By rewriting the equation as recursive form, we have:</p><disp-formula id="scirp.48206-formula1739"><label>(6)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\43d6bd62-5628-4627-8f4d-6868eb4ed270.png"/></disp-formula><p>The likelihood or the transition probability is mostly chosen as the proposal distribution. Using the prior distribution instead of the proposal distribution makes the sampling easier and accelerates the weighting process. Replacing q with <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\b1c74263-3fe5-490a-aa07-c7ae30c48f6e.png" xlink:type="simple"/></inline-formula> in Equation (4), final normalized weights will be obtained as follows:</p><disp-formula id="scirp.48206-formula1740"><label>(7)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\1d5cd5f4-f0df-43a0-a3a1-7fe24cd425e3.png"/></disp-formula><p>This process is repeated in each step to approximate the state variable [<xref ref-type="bibr" rid="scirp.48206-ref35">35</xref>] .</p></sec><sec id="s2_5"><title>2.5. Object Representation</title><p>The first step of each tracking algorithm, is selecting a proper type of representation [<xref ref-type="bibr" rid="scirp.48206-ref36">36</xref>] . Based on a specific application and object characteristics, different types of representations are utilized. Of all object representation types, point representation is the simplest and most popular one causing decrease in computational costs. This is often employed where objects are small [<xref ref-type="bibr" rid="scirp.48206-ref36">36</xref>] . Sperm cells occupy small areas on every frame. In addition, the subsequent analysis such as computing percent motility and curvilinear velocity are defined based on point localization. Therefore, in this paper the point representation was used to locate the sperms. Due to free movement of sperm, the sperms do not have invariant appearances and their average intensity may change a long time. Therefore, object representations which are based on shape and boundaries of an object were not considered in this paper. <xref ref-type="fig" rid="fig1">Figure 1</xref> depicts five consecutive frames of a singular sperm. Each frame includes sperm elliptic boundary and a line which illustrates its head direction. It shows that the head direction doesn’t change necessarily smoothly. In conclusion, in this study a head-independent sperm tracking algorithm was addressed.</p></sec><sec id="s2_6"><title>2.6. State Space Model</title><p>In this paper, in order to model sperm movement the expansion of Taylor series around sperm head position was used in which center of the target sperm is shown by variable x. This expansion around x leads to the sperm motion equation:</p><disp-formula id="scirp.48206-formula1741"><label>(8)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\0560ed9d-ff81-4acb-b884-75900219f89d.png"/></disp-formula><disp-formula id="scirp.48206-formula1742"><label>(9)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\d25c052c-12d7-4c43-8a10-299b96b9b202.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\25fb8e2c-fea4-40a8-af63-9ebb1fa339a7.png" xlink:type="simple"/></inline-formula> and T denotes the time interval between two consecutive frames. Although, using higher order equations bring complex models, a large number of particles are required to reach accurate estimation. So, because of calculating higher order derivatives the computational cost extremely goes up. Hence, truncated Taylor series including only first order derivative was used and the rest of series were modeled by a Gaussian random process denoted by <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\fdd91bb1-5ddc-487b-989e-72081da1808b.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.48206-ref37">37</xref>] . For simplification, a vector representation was utilized in which two-di- mensional (2D) position and velocity explain the state of motion. The state vector variables is <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\042c8608-a233-4af1-a08b-9fadf0e3fb7e.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\fe951653-9ada-463b-91c5-463e83e1c2cc.png" xlink:type="simple"/></inline-formula> denotes the target position and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\b5789f12-87b4-4f44-bf99-262109d4063c.png" xlink:type="simple"/></inline-formula> shows its velocity. Equation (9) can be written as:</p><fig-group id="fig1"><caption><title>Figure 1</title><p> Variation in size, shape and direction of a low contrast sperm during image acquisition</p></caption><fig id ="fig1_1"><label>(a) (b) (c) (d) (e)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\ee6ddbf9-276a-41fd-bf42-a31077cc9c20.png"/></fig></fig-group><disp-formula id="scirp.48206-formula1743"><label>(10)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\863a12e8-7a62-45d4-b07d-26a241eb7523.png"/></disp-formula><disp-formula id="scirp.48206-formula1744"><label>(11)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\0cd993ff-d772-4a70-ba83-96c70aa3fe77.png"/></disp-formula><p>where A is the transition matrix and C shows the gain matrix [<xref ref-type="bibr" rid="scirp.48206-ref17">17</xref>] .</p></sec><sec id="s2_7"><title>2.7. Likelihood</title><p>Euclidian distance is common criterion to measure the likelihood. In this paper also the distance between the positions and the velocities were computed for the particles.</p><disp-formula id="scirp.48206-formula1745"><label>(12)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\2da03224-98df-4f51-9af4-b3cd0302f3e3.png"/></disp-formula><disp-formula id="scirp.48206-formula1746"><label>(13)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\6c01ccbe-27dd-4dd2-adb0-c5111cd16c63.png"/></disp-formula><disp-formula id="scirp.48206-formula1747"><label>(14)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\5715a97d-f781-4d35-b8a7-99e8f08b5f37.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\8dbc4ae6-b38e-4376-8884-f8d703924aff.png" xlink:type="simple"/></inline-formula> shows the most probable measurement for target sperm position. For combining normalized distances, a simple definition was used.</p><disp-formula id="scirp.48206-formula1748"><label>(15)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\8c40dd3f-eebc-48b2-9a35-e67ab0fae49d.png"/></disp-formula><p>After acquiring total distance, the likelihood probability can be calculated as:</p><disp-formula id="scirp.48206-formula1749"><label>(16)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\f822392e-142a-43f5-979b-77367f648f76.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\9e6b81bd-f4ef-4b2c-8162-6317388f44b5.png" xlink:type="simple"/></inline-formula> denotes noise standard deviation of measurements [<xref ref-type="bibr" rid="scirp.48206-ref18">18</xref>] .</p></sec><sec id="s2_8"><title>2.8. Segmentation and Detection</title><p>Watershed segmentation algorithm is based on topography of intensity. This method comprises principle concepts of other segmentation methods such as thresholding, edge detection and growing region. Furthermore, Watershed includes contiguous boundaries [<xref ref-type="bibr" rid="scirp.48206-ref38">38</xref>] . In this method based on topography of intensity, each area in an image is divided into three categories. First category, called minimum regions, belongs to local minimum intensity areas. Second category, called catchment basin, depicts a set of points if a droplet of water drips there, then, it slips down towards a specific minimum region. Third category, called watershed lines, refers to the areas where droplets of water have the same chance to slip down towards adjacent minimum regions.</p><p>The main goal in this method is finding watershed lines. At the beginning, assume that minimum regions are punched and water gradually goes up from the minimum intensity to the maximum. If level of water is determined by<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\6c37779f-9e24-4fef-a823-71ee14b9fbde.png" xlink:type="simple"/></inline-formula>; magnitude of l will change from minimum intensity up to maximum. If <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\dfd9edae-c1e3-41d1-b377-6dc5cbdfeb21.png" xlink:type="simple"/></inline-formula> denotes the regions relied under the surface of water level<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\47bbf0a4-2d15-487d-9a39-1ccccca2e025.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\c0ddb185-462a-4fc8-95cc-c84dcdb58b4d.png" xlink:type="simple"/></inline-formula>will comprise the regions under level<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\409d8b2f-a7b9-49d6-978c-6407d72c5b61.png" xlink:type="simple"/></inline-formula>. Therefore, there are three possible states between <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\9b40c5b1-8125-4529-9995-87e4e1f33c5c.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\d6378359-c376-433d-8fcb-723171e1f3c8.png" xlink:type="simple"/></inline-formula> as follows:</p><p>1)<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\3ff659a2-b611-46ee-b50a-b0755535960c.png" xlink:type="simple"/></inline-formula>.</p><p>2) <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\35889979-4a20-4f4d-9210-c3dcd71b5310.png" xlink:type="simple"/></inline-formula>and includes only one flooded catchment basin under level<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\0687f9a1-6e6b-4b04-8e5a-6f5af0d1ef8b.png" xlink:type="simple"/></inline-formula>.</p><p>3) <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\bc371730-4021-4341-9673-10b49a7a4f54.png" xlink:type="simple"/></inline-formula>and includes more than one flooded catchment basin under level<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\ffe0c35a-391b-47d1-b345-bb7ede38a25f.png" xlink:type="simple"/></inline-formula>.</p><p>Third state happens just when a new catchment basin is flooded with water, so a new dam is constructed to prevent.</p><p>The watershed algorithm suffers from over-segmentation [<xref ref-type="bibr" rid="scirp.48206-ref38">38</xref>] especially in occlusion senses, moreover the smoothing filter decreases the possibility of discrimination between occluded sperms. Thus, in this study, a local region around the single target was used to apply Otsu thresholding [<xref ref-type="bibr" rid="scirp.48206-ref39">39</xref>] , then a binary watershed algorithm based on specific distance transform was employed to reach final sperm segments. The experience showed that this approach reduces the over-segmentations. Eventually, the segments whose sizes were in the range of a sperm were labeled and their centers were determined.</p><p>In binary watershed algorithm, the distance between each 0 pixel and the nearest 1 pixel is defined as basis of the transform. The distance has different definitions, however based on [<xref ref-type="bibr" rid="scirp.48206-ref40">40</xref>] , the best definition for segmenting correlated objects in binary images is the chessboard distance which is defined as:</p><disp-formula id="scirp.48206-formula1750"><label>(17)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\1ad0e1eb-3fb8-40bb-8ad4-29ca181cfc59.png"/></disp-formula><p>Therefore, the chessboard distance was applied for binary watershed segmentation.</p><p>In order to avoid superfluous measurements, only a specific neighborhood around the estimated position of the target sperm att was considered. All detection process was performed in this area called “search window”. On one hand, if search window is too small (i.e. as same as a sperm head), the algorithm will not be able to distinguish whether an occlusion has been occurred or not. On the other hand, if it is too large, it may accommodate several sperms which bewilder the algorithm. Hence, there is a tradeoff between large window and algorithm complexity. The image system provided <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\9d65849d-226a-4f17-bc26-a3aea86aee78.png" xlink:type="simple"/></inline-formula> resolution under which the progressive sperms were able to move more than two pixels in each frame. Moreover, watershed algorithm needed to compute fast fourier transform (FFT) for which a window of size <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\a273001b-4e2f-4946-a17b-9a4a88861cbc.png" xlink:type="simple"/></inline-formula> brings faster performance. Consequently, a <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\8ec71875-6e84-4176-83c8-0bfe50ae3988.png" xlink:type="simple"/></inline-formula> search window was assigned for the detection.</p></sec></sec><sec id="s3"><title>3. Tracking and Occlusion Detection</title><p>The tracking began by selecting a singular sperm in a frame. Center of each detected segment which had fulfilled the sperm size constraint was considered as <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\b697edec-5ad8-4be7-82ca-b60230a75f09.png" xlink:type="simple"/></inline-formula> (see <xref ref-type="fig" rid="fig2">Figure 2</xref>). Since the search window had a specific size, only limited number of sperms was detected. Afterward, the distance between <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\4e8b8517-6f75-47b6-96e6-9171c3510cf0.png" xlink:type="simple"/></inline-formula> and last position of the target sperm at <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\b49615eb-2948-42fe-ae9c-c2195f938577.png" xlink:type="simple"/></inline-formula> was computed. Finally, position and displacement of every <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\0dd08329-1b6f-4107-b3f9-92b804c9e154.png" xlink:type="simple"/></inline-formula> were saved as the measurements. <xref ref-type="fig" rid="fig2">Figure 2</xref> shows search window at t where detection algorithm labels only two of four segments. The two segments, smaller than sperm head, are rejected. Also y<sup>1</sup> and y<sup>2</sup> are taken part in target selection where the two arrows in <xref ref-type="fig" rid="fig2">Figure 2</xref> represent their displacements.</p><p>In this paper, in order to improve target detection and avoid mistracking after occlusions, three stages were defined for target sperm called “before occlusion”, “occlusion” and “after occlusion”.</p><p>• Before occlusion shows that the target sperm never had an occlusion along its trajectory or it has passed occlusion stage already.</p><p>• Occlusion shows the stage when the detection algorithm is not able to make distinction between the target and occluded sperms. The basic idea is that detecting a mass, remarkably larger than sperm size, is the sign of occlusion.</p><p>• After occlusion shows the stage when an occlusion has been obviated and detection algorithm is able to separate the target again.</p><p>If the target sperm is in before occlusion or occlusion stages, the closest <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\9de8eeda-64a5-4f45-a11e-5a7ecf2de76e.png" xlink:type="simple"/></inline-formula> to approximate state x<sub>MMSE</sub> will be the most likely position for the target sperm shown by<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\809e0746-c5a1-4b84-9066-17b046917ebc.png" xlink:type="simple"/></inline-formula>. The main problem appears when the target sperm is in after occlusion stage, since the nearest distance cannot be trusted any more. In this case, history of the target sperm movements is utilized to discern it. Hence, the average direction and velocity of the target along three prior frames were calculated:</p><disp-formula id="scirp.48206-formula1751"><label>(18)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\66c9a561-aba4-4f64-b847-ee68663ec4f0.png"/></disp-formula><disp-formula id="scirp.48206-formula1752"><label>(19)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\cd638d56-82d9-43c4-989d-d5cab565fc15.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\5dd32585-5fc1-4481-832b-6f1740e539d2.png" xlink:type="simple"/></inline-formula> denotes the moment at which the sperms has just separated. Thus, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\fcfd2e39-0dcb-449a-891e-14aac710afa9.png" xlink:type="simple"/></inline-formula>after occlusion is determined by the estimated position of the target sperm using<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\696c39da-d573-4a35-b397-272fde501f50.png" xlink:type="simple"/></inline-formula>.</p><fig id="fig2"><label>Figure 2</label><caption><p> Labeling sperms in the search window. Of all detected objects only the two meeting the sperm constraints are labeled as y<sup>1</sup> and y<sup>2</sup></p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\5f4ca527-2fe2-42e4-8e9a-d56b595185d1.png"/></fig><p>Following the determination of<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\b27a85f2-4f86-49f1-8638-c419625d267d.png" xlink:type="simple"/></inline-formula>, those particles which are closer to <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\9c8be0d9-9752-4671-adac-1371a5bef65a.png" xlink:type="simple"/></inline-formula> in terms of position and velocity, are allocated more weights. The distance between measurements obtained from <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\c9a0fafa-ce93-4fea-a9be-087cd704ade4.png" xlink:type="simple"/></inline-formula> and particles were computed by Equations (12), (13) and (14) and the likelihood was measured by Equations (15) and (16).</p></sec><sec id="s4"><title>4. Implementation</title><p>200 particles were used for tracking. On the assumption that <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\0703d350-f2a8-4921-aeb7-bc2d666fbc1b.png" xlink:type="simple"/></inline-formula> is uncorrelated, particles were propagated throughout the search window where their initial weights had been assigned 1/N. Then, the weighting was performed using likelihood function. In addition, the systematic resampling was utilized to avoid generating ineffective or too dominant particles [<xref ref-type="bibr" rid="scirp.48206-ref41">41</xref>] . Finally, using minimum mean square error estimation, approximate state was computed as follows:</p><disp-formula id="scirp.48206-formula1753"><label>(20)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\055164ad-4020-483b-8b18-56e734aba7bc.png"/></disp-formula><p>Using<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\13f1296f-442d-440a-89b6-372cc48f2732.png" xlink:type="simple"/></inline-formula>, next position of search window was determined:</p><disp-formula id="scirp.48206-formula1754"><label>(21)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\c730f0e9-ad78-4e62-9660-a65d017e179d.png"/></disp-formula><disp-formula id="scirp.48206-formula1755"><label>(22)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\d45720e0-6d79-4f35-aca0-dca8e8cbc4c8.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\05a2494f-7cf6-497f-94aa-d9db349c10da.png" xlink:type="simple"/></inline-formula> denotes center of Search Window.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> depicts flowchart of the algorithm which explains how this algorithm uses the measurements to change the weights of the particles regarding the stage of the target sperm.</p></sec><sec id="s5"><title>5. Results and Discussions</title><p>In this section, different steps of the sperm tracking algorithm used for the microscopic sperm images are discussed.</p><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows the result of morphological filtering and background removing. As shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>, not only the sperms were highlighted, but also average intensity of the background was decreased intensely so that the sperms were observed as bright objects.</p><p>As the second step in preprocessing, the median adaptive background removing technique was responsible for eliminating imaging artifacts and very slow moving non-sperm cells. <xref ref-type="fig" rid="fig4">Figure 4</xref>(c) displays the preprocessed image after adaptive median background removing and open filtering. In the obtained image both the marker and noisy pixels have been disappeared drastically.</p><p>After preprocessing, in tracking, this is the sperm occlusion determines approach of the algorithm in selecting proper criteria for diagnosing the target sperm. <xref ref-type="fig" rid="fig5">Figure 5</xref> schematically exhibits the algorithm manner toward sperm occlusion via the three consecutive frames. The solid ellipse shows the target and the dashed one denotes a pesky sperm. <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\cbbefe28-1e4f-46d8-b08d-bc141455a7bb.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\ad8fa366-6e2c-44dd-8622-04771b0ec464.png" xlink:type="simple"/></inline-formula> are the detected segment centers, t is time, and the dashed square refers to the search window. The small solid circles show the previous target sperm positions selected by the algorithmwhile the small hollow circle shows the predicted position for the target sperm in each frame. In the frame <xref ref-type="fig" rid="fig5">Figure 5</xref>(a), the target is in the before-occlusion status and the arrows reveal the distance between x<sub>MMSE</sub> and the segments</p><fig id="fig3"><label>Figure 3</label><caption><p> Flowchart of the proposed low contrast sperm tracking algorithm</p></caption><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\fbfeb218-74b7-48e9-95b3-94d5f4ede222.png"/></fig><fig-group id="fig4"><caption><title>Figure 4</title><p> Video preparation. (a) Original image; (b) Morphological filtering; (c) Back- ground removing</p></caption><fig id ="fig4_1"><label>(a) (b) (c)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\341f9db0-56b6-4c33-a63b-b85de34267ad.png"/></fig></fig-group><fig-group id="fig5"><caption><title>Figure 5</title><p> The scheme of sperm tracking in a occlusion scene. (a) Before occlusion; (b) Occlusion; (c) After occlusion</p></caption><fig id ="fig5_1"><label>(a) (b) (c)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\0d901ffb-a791-4844-a809-9d2ee52cc975.png"/></fig></fig-group><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\e8c5b27e-02db-4af6-a779-807a93a84f46.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\d3a6ec3e-dd1e-40e5-b59f-a20bb89a31bf.png" xlink:type="simple"/></inline-formula>. According to the nearest distance criterion <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\c8f63a08-1c5b-4b6e-a9a3-9c73f85cc56e.png" xlink:type="simple"/></inline-formula> is selected as the sperm position. In the frame <xref ref-type="fig" rid="fig5">Figure 5</xref>(b), the occlusion occurs so that the watershed algorithm detects a unique segment. So, merely <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\38175042-8129-4cf6-8bfa-edd6a1fe953f.png" xlink:type="simple"/></inline-formula> is observed and considered as the sperm position. Eventually in frame <xref ref-type="fig" rid="fig5">Figure 5</xref>(c), the pesky sperm which is assumingly unwilling to travel long distance, causes misdetection, if the nearest distance criterion is applied for tracking. In such scenarios, in this paper the average velocity was used to predict the new target position as shown by the hollow square. Afterward, proximity to the new point was the criterion for <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\f1fcd8eb-fdcf-4488-a3fd-ea7258cd9e51.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\917ae874-4636-4ec5-92d3-21072c56981f.png" xlink:type="simple"/></inline-formula>.</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> represents operation of the algorithm for real data in which 4 consecutive frames discover a real sperm occlusion scene. Figures 6(a1)-(a4) display distance transform of the search area around the target sperm after thresholding. As you can see in this raw (a) although the chessboard distance has usually acceptable performance for sperm discrimination however, some cases like <xref ref-type="fig" rid="fig6">Figure 6</xref>(a2) challenge it. Therefore, based on size of the detected object an occlusion is flagged.</p><p>Figures 6(b1)-(b4) denote object boundaries corresponding to Figures 6(a1)-(a4) including single points referring to the target sperm positions selected by the algorithm. The marker points show the algorithm success in coping sperm occlusion problem.</p><p>In order to assess the method, two groups of patients were established. The proficiency and compatibility of the method with the categories of sperm motility was evaluated using the first group including 20 videos where a target sperm from different movement categories was selected from each video so that it had no occlusion along its trajectory. In contrast, to evaluate the robustness of the algorithm against the occlusion, 30 videos were considered so that the chosen sperms had one or more occlusion during their paths.</p><p>In the first hand, an expert was asked to label the target in each frame. Then, every sperm was tracked by the algorithm. The comparison between the manual track and the algorithm result was fulfilled by object tracking error (OTE) [<xref ref-type="bibr" rid="scirp.48206-ref21">21</xref>] which measures errors in every frame as:</p><disp-formula id="scirp.48206-formula1756"><label>(23)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\ab64ab1d-bbbf-4f9e-b511-1726d3282ed0.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\748b39ac-cfee-41b4-965c-2e6ef70587ca.png" xlink:type="simple"/></inline-formula> denotes the manual sperm position and n is number of frames until the sperm exits the scene. In each group, the average tracking errors was determined. In the case that a sperm hides or the tracker misses the target, the correspondent error extremely increases. Thus, in order to avoid the misconception caused by this phenomenon, average error was computed for only sperms which were tracked completely. <xref ref-type="table" rid="table1">Table 1</xref> illustrates the results of low contrast sperm tracking for both groups. Of all 20 sperms with no occlusion in their path, only one sperm was missed. This can be interpreted as the ability and compatibility of the algorithm in tracking all sperm categories. <xref ref-type="fig" rid="fig7">Figure 7</xref> shows the trajectories detected by the algorithm for the sperms of different types of motility.</p><p>Also, the algorithm achieved satisfactory results in the case of occlusion scenes. In this respect, <xref ref-type="table" rid="table2">Table 2</xref> shows the accuracy and the average tracking error in each group. When a sperm is crossing another, it is hard to locate the target sperm even for an expert, therefore the second group shows higher average tracking error. However, through the eyes of specialists, this range of error has trivial influence on subsequent examinations.</p></sec><sec id="s6"><title>6. Conclusions</title><p>This paper described different phases of single sperm tracking including preprocessing and localization with special attention to be devoted to properly adapting them to moving sperm objects and the occlusion problem. Although it has been trying to cope with sperm occlusion through advanced imaging device such as laser and acoustic waves, this paper attempted to find a solution by virtue of a sheer algorithmic approach which helps small laboratories to be involved with this research field without having access to modern electronic equipments.</p><p>In the case of preprocessing, the sperm movements were smoothed to reduce the effect of the low sampling rate, using a spatio-temporal Gaussian filter. In addition, an adaptive background removing technique was applied to expunge the impact of non-sperm moving objects and undesirable artifacts in the slides. Although appearance-based methods, such as template matching, are able to segment low-contrast sperms, they are hardly able to separate the target sperm from occluded one because low-contrast sperms do not adhere strictly to shape-based regularities. Nonetheless, it is still possible to take advantage of some constraints on sperms’ shape and size. In this paper, object-oriented morphological filters and the size constraints were used to feature the sperm objects and eliminate the waste debris.</p><p>On one side, complex segmentation methods increase computations. On the other side, simple methods are</p><fig-group id="fig6"><caption><title>Figure 6</title><p> Four consecutive frames showing a target sperm from before collision until distancing from the other sperm. (a) Denotes chessboard distance transform; (b) Watershed segmentation and labeling the target sperm</p></caption><fig id ="fig6_1"><label>(a1) (a2) (a3) (a4)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\8846ad92-2bb2-47fc-97f5-cf5e8a60eb6d.png"/></fig><fig id ="fig6_2"><label>(b1) (b2) (b3) (b4)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\0cd1c5dd-d7ca-4069-9b2d-cde70667ef10.png"/></fig></fig-group><fig-group id="fig7"><caption><title>Figure 7</title><p> Representation of the performance of the algorithm in tree types of sperm movement. (a) Rapid progressive motility; (b) Slow progressive motility; (c) Non-pro- gressive motility</p></caption><fig id ="fig7_1"><label>(a) (b) (c)</label><graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\2-1990057x\704a67ab-7c67-4940-8f2d-aa686eaceef1.png"/></fig></fig-group><table-wrap id="table1"  position="float"><object-id pub-id-type="pii">Table 1</object-id><label>Table 1</label><caption><p>. The results of sperm tracking for two groups</p></caption><table><thead><tr><th align="center" valign="middle" >Tracking</th><th align="center" valign="middle" >20 sperms</th><th align="center" valign="middle" >30 sperms</th></tr></thead><tbody><tr><td align="center" valign="middle" >Complete</td><td align="center" valign="middle" >19</td><td align="center" valign="middle" >26</td></tr><tr><td align="center" valign="middle" >Comparative</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >Wrong</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td></tr></tbody></table></table-wrap><table-wrap id="table2"  position="float"><object-id pub-id-type="pii">Table 2</object-id><label>Table 2</label><caption><p>. The accuracy and error of the algorithm for two groups</p></caption><table><thead><tr><th align="center" valign="middle" >Group</th><th align="center" valign="middle" >Accuracy</th><th align="center" valign="middle" >Error</th></tr></thead><tbody><tr><td align="center" valign="middle" >20 sperms</td><td align="center" valign="middle" >95</td><td align="center" valign="middle" >3.56</td></tr><tr><td align="center" valign="middle" >30 sperms</td><td align="center" valign="middle" >86.66</td><td align="center" valign="middle" >5.63</td></tr></tbody></table></table-wrap><p>not effectively able to cope with the sperm occlusion problem. Gray Watershed algorithm counts as a powerful segmentation method, however internal changes of intensity in a small object causes over-segmentation in Gray Watershed method. Therefore, in this paper, the binary watershed algorithm based on the chessboard distance transform was utilized. In addition, combination of the thresholding and the binary watershed algorithm provided high-efficiency sperm segmentation.</p><p>The proposed low-contrast sperm tracking method is a plain and efficient solution to the occlusion problem. In contrast to statistical tracking methods, selecting complex weighting techniques to encompass all sperm movement categories, the proposed method defines three stages for each target sperm to reduce the compositional cost and improve the performance of tracking. In this regard, extra computations are carried out only when an occlusion occurs which saves the operation time. In addition, all computations were limited to a search window. It was designed so that it had the minimum size for searching space and was large enough to monitor sperm occlusions.</p><p>The result showed that the switchable weight particle filtering has the great ability to track low-contrast sperms. 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