<?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">IJMPCERO</journal-id><journal-title-group><journal-title>International Journal of Medical Physics, Clinical Engineering and Radiation Oncology</journal-title></journal-title-group><issn pub-type="epub">2168-5436</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijmpcero.2016.51009</article-id><article-id pub-id-type="publisher-id">IJMPCERO-64021</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><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Automatic Anomaly Detection of Respiratory Motion Based on Singular Spectrum Analysis
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>un’ichi</surname><given-names>Kotoku</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>Shinobu</surname><given-names>Kumagai</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>Ryouhei</surname><given-names>Uemura</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Susumu</surname><given-names>Nakabayashi</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>Takenori</surname><given-names>Kobayashi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Graduate School of Medical Technology, Teikyo University, Tokyo, Japan</addr-line></aff><aff id="aff2"><addr-line>Central of Radiology, Teikyo University Hospital, Tokyo, Japan</addr-line></aff><pub-date pub-type="epub"><day>03</day><month>02</month><year>2016</year></pub-date><volume>05</volume><issue>01</issue><fpage>88</fpage><lpage>95</lpage><history><date date-type="received"><day>2</day>	<month>February</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>26</month>	<year>February</year>	</date><date date-type="accepted"><day>29</day>	<month>February</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The realization of automatic anomaly detection of respiratory motion could be very useful to prevent accidental damage during radiation therapy. In this paper, we proposed an automatic anomaly detection method using singular value decomposition analysis. Before applying this method, the investigator needs a normal respiratory motion data of a patient. From these data, a trajectory matrix representing normal time-series feature is created. Decomposing the matrix, we obtained the feature of normal time series. Then, we applied the same procedure to real-time data and obtained real-time features. Calculating the similarity of those feature matrixes, an anomaly score was obtained. Patient motion was observed by a depth camera. In our simulation, two types of motion e.g. cough and sudden stop of breathing were successfully detected, while gradual change of respiratory cycle frequency was not detected clearly.
 
</p></abstract><kwd-group><kwd>Anomaly Detection</kwd><kwd> Respiratory Motion</kwd><kwd> Singular Spectrum Analysis</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Monitoring of a patient has been an important but tedious work for medical staffs. The automatic anomaly detection for respiratory motion is very critical to conduct radiation therapy safely.</p><p>The difficulty of anomaly detection causes from the fact that 1) almost all of respiratory curves show base- line drift, 2) amplitudes of respiratory motions vary sometimes up to 300%, 3) frequency of respiratory cycle sometimes changes [<xref ref-type="bibr" rid="scirp.64021-ref1">1</xref>] . Because of these characteristics, simple threshold method tends to fail for detection of anomaly motion.</p><p>There has been some useful anomaly detection algorithm for industrial use. Those algorithms are classified into two categories: model based algorithm and model free algorithm. Typical examples of model based approach are auto regressive (AR) model [<xref ref-type="bibr" rid="scirp.64021-ref2">2</xref>] and Kalman filter algorithm [<xref ref-type="bibr" rid="scirp.64021-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.64021-ref5">5</xref>] . An example of model-free approach is singular spectrum analysis. The merit of model-free approach is an ability to deal with unexpected motion error and easy implementation. An example of this type of approach is singular spectrum analysis. It is a non-parametric method to extract characteristics of time-series data. There have been a few examples for an application of change point detection [<xref ref-type="bibr" rid="scirp.64021-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.64021-ref7">7</xref>] , however, few researchers have reported on anomaly detection of respiratory motion.</p><p>In this paper, we tried to apply an anomaly detection algorithm based on singular spectrum analysis to a respiratory curve of a patient.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Measurement</title><p>In this study, we applied the singular decomposition technique to measured respiratory motion obtained by a depth camera (Microsoft Kinect v1). First, we will describe how we measured respiratory curve. In the next section, we will explain the detail of algorithm to detect anomaly motion.</p><p>To monitor the respiratory motion, contact-less sensor was desirable. As a low-price sensor, our group has been using a Kinect sensor. Kinect sensor obtained depth data to a target from a shift of projected infrared patterns and the accuracy was 3 - 4 mm. To reduce the noise, we applied Ueda’s algorithm to the raw data of Kinect sensor. The sampling rate was 5 fps. The detail of this system was described in Kumagai et al. [<xref ref-type="bibr" rid="scirp.64021-ref8">8</xref>] .</p><p>For testing performance, one of the authors simulated two types of anomaly motion, e.g. cough, sudden stop of breathing.</p></sec><sec id="s2_2"><title>2.2. Anomaly Detection Method</title><p>To detect an anomaly motion, we first extracted the feature of the time-series data with window length w based on singular value spectrum analysis [<xref ref-type="bibr" rid="scirp.64021-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.64021-ref10">10</xref>] .</p><p>Let normal (or reference) time-series data be<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x6.png" xlink:type="simple"/></inline-formula>. We can define a trajectory matrix as</p><disp-formula id="scirp.64021-formula765"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-2660190x7.png"  xlink:type="simple"/></disp-formula><p>The matrix holds the feature of normal time series data at a reference time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x8.png" xlink:type="simple"/></inline-formula> with look-back time of w. k was set to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x9.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.64021-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.64021-ref10">10</xref>] .</p><p>Similarly, we can define a matrix representing current states (at time t) of respiratory motion as,</p><disp-formula id="scirp.64021-formula766"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-2660190x10.png"  xlink:type="simple"/></disp-formula><p>For example, window length w was set to 40 (= 8 sec). k was set to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x11.png" xlink:type="simple"/></inline-formula>.</p><p>Next, we decomposed the matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x12.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x13.png" xlink:type="simple"/></inline-formula> using singular value decomposition</p><disp-formula id="scirp.64021-formula767"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-2660190x14.png"  xlink:type="simple"/></disp-formula><p>here <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x15.png" xlink:type="simple"/></inline-formula> is an orthogonal matrix and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x16.png" xlink:type="simple"/></inline-formula> is an orthogonal matrix and W is a diagonal matrix with singular values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x17.png" xlink:type="simple"/></inline-formula> and there is a constraint of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x18.png" xlink:type="simple"/></inline-formula>.</p><p>From this decomposition of matrix, the matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x19.png" xlink:type="simple"/></inline-formula> can be approximated as</p><disp-formula id="scirp.64021-formula768"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-2660190x20.png"  xlink:type="simple"/></disp-formula><p>This is an example of well-known spectrum decomposition of a matrix. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x21.png" xlink:type="simple"/></inline-formula>, in the similar manner, we obtain the following formula</p><disp-formula id="scirp.64021-formula769"><graphic  xlink:href="http://html.scirp.org/file/9-2660190x22.png"  xlink:type="simple"/></disp-formula><p><xref ref-type="fig" rid="fig1">Figure 1</xref> shows the singular values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x23.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x24.png" xlink:type="simple"/></inline-formula>. From this figure, we set m to 5 to approximate the time series data. Therefore, the matrices were approximated as</p><disp-formula id="scirp.64021-formula770"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-2660190x25.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64021-formula771"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-2660190x26.png"  xlink:type="simple"/></disp-formula><p>Then we defined a matrix representing the feature of time series of the reference signals as</p><disp-formula id="scirp.64021-formula772"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-2660190x27.png"  xlink:type="simple"/></disp-formula><p>Similarly, a matrix representing features of current status was defined as</p><disp-formula id="scirp.64021-formula773"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-2660190x28.png"  xlink:type="simple"/></disp-formula><p>To measure the similarity of two time series, we calculated canonical angle of two matrices as</p><disp-formula id="scirp.64021-formula774"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-2660190x29.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x30.png" xlink:type="simple"/></inline-formula> is a two norm of a matrix calculated by a root of the maximum singular value of the matrix. Note that the cosine of canonical angle is within 0 and 1, as an anomaly score, we can define</p><disp-formula id="scirp.64021-formula775"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-2660190x31.png"  xlink:type="simple"/></disp-formula><p>This score represents the anomaly of the current time window compared with the reference time window.</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Singular values of X<sub>1</sub> (circle) and X<sub>2</sub> (cross).</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-2660190x32.png"/></fig></fig-group></sec><sec id="s2_3"><title>2.3. Performance Test</title><p>The anomaly detection can be divided into six steps.</p><p>1. Measurement of normal (not including anomaly events) respiratory motion.</p><p>2. Calculation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x33.png" xlink:type="simple"/></inline-formula></p><p>3. Measurement of respiratory motion.</p><p>4. Calculation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x34.png" xlink:type="simple"/></inline-formula></p><p>5. Calculation of anomaly score from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x35.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-2660190x36.png" xlink:type="simple"/></inline-formula></p><p>6. If the anomaly score exceeds the threshold, then the algorithm judged anomaly event occurred.</p><p>In the Step1, we measured a respiratory curve of a patient under normal situation (not suffered from anomaly events).</p><p>To test our algorithm, we measured the reference respiratory motion and normal respiratory motion by a volunteer. Then the time-series data were retrospectively analyzed using our algorithm. All algorithms were implemented using R language [<xref ref-type="bibr" rid="scirp.64021-ref11">11</xref>] .</p><p>Based on the algorithm, we performed real-time prediction of respiratory motion using our respiratory monitoringsystem [<xref ref-type="bibr" rid="scirp.64021-ref8">8</xref>] . The algorithm was implemented by python language.</p></sec></sec><sec id="s3"><title>3. Results</title><p>In our study, we applied an anomaly detection algorithm based on singular spectrum analysis.</p><p>Measurement data was obtained by a depth camera.</p><p>As a reference of normal respiratory curve, a normal respiratory motion was recorded with a depth camera. The obtained data was shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. The interval of dashed lines represents an interval to be used for singular spectrum analysis. Obviously, the length of interval strongly affects calculation results of anomaly score. The choice of window length w will be discussed in the discussion section later.</p><p>To simulate anomaly motions, the four types of anomaly motion were tested. <xref ref-type="fig" rid="fig3">Figure 3</xref> shows an anomaly score when cough events occurred. <xref ref-type="fig" rid="fig4">Figure 4</xref> shows an anomaly score when breathing was suddenly stopped. As</p><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> A reference respiratory curve obtained by a depth camera. An interval between dashed lines were used to calculate the trajectory matrix X<sub>1</sub></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-2660190x37.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> An example of cough events simulated by a volunteer. Two peaks at around 60 s and 120 s represent the cough events. The blue curve repre- sents the respiratory curve, while the red curve represents the anomaly score calculated by Equation (10)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-2660190x38.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> An example of breathing stop simulated by a volunteer. The red curve represents the respiratory curve, while the blue curve represents the anomaly score calculated by Equation (10)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-2660190x39.png"/></fig><p>can be seen, the two types of events (cough and sudden stop of breathing) was successfully detected as a sudden increase of anomaly score. On the other hand, gradual increase of respiratory period was not clearly detected by this method.</p><p>Real-time anomaly detection was tested as shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>. The red curve represents the anomaly score. Simulated breathing stop was successfully detected by this algorithm.</p></sec><sec id="s4"><title>4. Discussion</title><p>Prior works have suggested that a general algorithm to detect anomaly motion would be difficult. This paper tried to overcome the difficulty using singular spectrum analysis.</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> A snapshot of real-time anomaly detection. Depth data (blue curve) and Anomaly score (red curve) are shown</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-2660190x40.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Window length dependencies of anomaly score in the case of breathing stop</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-2660190x41.png"/></fig><p>The window length w is a main parameter of the analysis. The result depends on the parameter. However, there has been no universal selection rule. Therefore, we analyzed a respiratory curve with different length and compared them by visual inspection.</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> shows anomaly scores with different time window w for a sudden stop of breathing event. As shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>, smaller window length tends to increase time resolution of anomaly detection, while the score itself tends to be noisy. Therefore, window length of 8 sec (w = 40) seemed to be appropriate for this situation. We did the same way to the cough events and obtained the <xref ref-type="fig" rid="fig7">Figure 7</xref>. We found the same tendency in the figure and determined the window length to be 8 sec. The optimum window length, however, depends on a patient.</p><p>There has a limitation, however, in this algorithm. One of the demerit in our method is the difficulty of the simple and explicit interpretation of the anomaly model. There has no clear-cut threshold to alarm an error. Users should be aware of these difficulties.</p><p>The merit of this approach is the fact that no a priori modeling of anomaly motion is required. Because anomaly motion is defined as a deviation from the normal motion, an explicit pre-implementation of anomaly mode is considered to be difficult. Using this algorithm, an unexpected anomaly motion could be detected. Hence, this algorithm will be a good supporting tool for medical staffs.</p></sec><sec id="s5"><title>5. Conclusion</title><p>We have demonstrated that automatic anomaly detection of respiratory motion using singular spectrum analysis was successful in the cough and sudden stop of breathing. The clinical use of this algorithm will be very hopeful.</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Window length dependencies of anomaly score in the case of cough</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/9-2660190x42.png"/></fig></sec><sec id="s6"><title>Acknowledgements</title><p>This work was supported by JSPS KAKENHI Grant Number 15K08703 and partly supported by JSPS Core-to- Core Program (No. 23003).</p></sec><sec id="s7"><title>Cite this paper</title><p>Jun’ichi Kotoku,Shinobu Kumagai,Ryouhei Uemura,Susumu Nakabayashi,Takenori Kobayashi, (2016) Automatic Anomaly Detection of Respiratory Motion Based on Singular Spectrum Analysis. International Journal of Medical Physics, Clinical Engineering and Radiation Oncology,05,88-95. doi: 10.4236/ijmpcero.2016.51009</p></sec></body><back><ref-list><title>References</title><ref id="scirp.64021-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Ruan, D., Fessler, J.A., Balter, J.M. and Keall, P.J. (2009) Real-Time Profiling of Respiratory Motion: Baseline Drift, Frequency Variation and Fundamental Pattern Change. Physics in Medicine and Biology, 54, 4777-4792. http://dx.doi.org/10.1088/0031-9155/54/15/009</mixed-citation></ref><ref id="scirp.64021-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">McCall, K.C. and Jeraj, R. (2007) Dual-Component Model of Respiratory Motion Based on the Periodic Autoregressive Moving Average (Periodic Arma) Method. 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