<?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">JSIP</journal-id><journal-title-group><journal-title>Journal of Signal and Information Processing</journal-title></journal-title-group><issn pub-type="epub">2159-4465</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jsip.2012.33043</article-id><article-id pub-id-type="publisher-id">JSIP-22124</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></subj-group></article-categories><title-group><article-title>
 
 
  Non-Stationary Signal Segmentation and Separation from Joint Time-Frequency Plane
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>bdullah</surname><given-names>Ali Alshehri</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>King Abdulaziz University</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>ashehri@kau.eud.sa</email></corresp></author-notes><pub-date pub-type="epub"><day>31</day><month>08</month><year>2012</year></pub-date><volume>03</volume><issue>03</issue><fpage>339</fpage><lpage>343</lpage><history><date date-type="received"><day>May</day>	<month>7th,</month>	<year>2012</year></date><date date-type="rev-recd"><day>June</day>	<month>11th,</month>	<year>2012</year>	</date><date date-type="accepted"><day>June</day>	<month>24th,</month>	<year>2012</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>
 
 
  Multi-components sinusoidal engineering signals who are non-stationary signals were considered in this study since their separation and segmentations are of great interests in many engineering fields. In most cases, the segmentation of non-stationary or multi-component signals is conducted in time domain. In this paper, we explore the advantages of applying joint time-frequency (TF) distribution of the multi-component signals to identify their segments. The Spectrogram that is known as Short-Time Fourier Transform (STFT) will be used for obtaining the time-frequency kernel. Time marginal of the computed kernel is optimally used for the signal segmentation. In order to obtain the desirable segmentation, it requires first to improve time marginal of the kernel by using two-dimensional Wiener mask filter applied to the TF kernel to mitigate and suppress non-stationary noise or interference. Additionally, a proper choice of the sliding window and its overlaying has enhanced our scheme to capture the discontinuities corresponding to the boundaries of the candidate segments.
 
</p></abstract><kwd-group><kwd>Signal Segmentation; Time-Frequency Distribution; Short-Time Fourier Transform; Non-Stationary; Wiener Masking</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Segmentation of multi-components or non-stationary signals has a considerable degree of importance for processing signals in many fields such as communications, biomedical, seismic and ultrasonic signals. Most of the signal segmentation approaches have been implemented and analyzed in time domain [1-3]. One of their disadvantages that they are statistical based analysis and in most cases they neglect the frequency information and its reflection on the signal dynamic changes over time. Recently, the wavelet transforms and time-frequency analysis have become a good and promise analytical methods due to their two-dimensional analysis [4-7]. Our proposed method is based on joint time-frequency analysis where both time and frequency information has been employed to obtain the desirable segmentation function. &#160;</p><p>This paper is composed of two level of analysis and its structure will be organized accordingly. The first level of this research work deals with improving time-frequency energy spectrum using the two-dimensional (2-D) Wiener masking for de-noising and mitigating any possible interferences that will affect the segmentation process. Second, is to optimize the time marginal of the masked kernel in order to obtain the desired segmentation function. For the rest of this introduction, a brief description of the short-time Fourier transform (STFT) and the 2-D Wiener filter will be provided. In Section 2, we will provide complete details of our approach including the process of denoising TF kernel and all derivations of the signal segmentation. Section 3 has the experimental work which illustrates the graphical results as depicted in the attached figures.</p><sec id="s1_1"><title>1.1. Short-Time Fourier Transform</title><p>In many applications such as speech, biomedical, seismic and other similar signals, we are interested in their frequency contents locally in time since their frequencies content evolve over time. These types of signal called non-stationary signals and using standard and regular Fourier Transform is not useful for analyzing such signals. The frequency information who are localized in time as the case of spikes and high frequency bursts cannot be easily detected from the regular Fourier Transform and joint time-frequency analysis becomes the right analysis tool. Recently, the time-frequency analysis methods have introduced a joint time-frequency energy distribution plane displaying the jointly both time and frequency information. Time-frequency distribution methods who do not show cross terms or negative frequency like STFT and the Discrete Evolutionary Transform (DET) provide a time-frequency distribution plane that is positive and has no cross term as well [8-10]. &#160;</p><p>In STFT, time-localization is a achieved first by windowing the signal by cutting off a slice of it and then taking its Fourier Transform using Fast Fourier Transform (FFT) [9,10]. The magnitude of the STFT kernel is known as the Spectrogram. Moving or sliding the window along the time axis, the relation between the variance of time and frequency can be identified. When the time window is sufficiently narrow, each frame extracted is viewed as stationary so that Fourier transform can be used. The type and length of the sliding window has a direct effect on time and frequency resolutions.</p><p>In Continuous-time STFT, the function is multiplied by a predefined window function which is nonzero for only a short period of time. The Fourier transform of the resulting short or windowed signal will have a two-dimensional representation of the signal written as:</p><p><img src="7-3400209\f46bceb7-acab-422c-b2d5-6271c8079d06.jpg" />where <img src="7-3400209\d97289d7-5bb1-44a3-a32d-aab47336eb42.jpg" /> is the window function, commonly Gaussian bell shape centered around zero, and <img src="7-3400209\48b76cce-d7ea-4023-b9b4-dd07c677efb4.jpg" /> is the signal to be transformed. <img src="7-3400209\7f876663-2280-4ab4-8de9-935a6dc1bf24.jpg" />is the time-frequency kernel or the STFT resulted from the Fourier Transform of<img src="7-3400209\734ad45e-7516-41f4-9027-9fcfd1f601e0.jpg" />. This kernel is a complex matrix representing the magnitude and phase of the transformed signal over time and frequency domains.&#160;</p><p>For the discrete representation of STFT, the data signal is broken up into equal chunks or frames. To reduce the artifacts at the boundary, these frames usually overlap each other. In similar way, each frame is Fourier transformed and output complex result will be added to get the final matrix representing the signal magnitude and phase for each point in time and frequency. This can be expressed as:</p><p><img src="7-3400209\ffd46f6f-6a76-489d-a1ad-0e7c7a73647e.jpg" />where <img src="7-3400209\84affb19-6b84-401e-9f2e-3ce9697393ee.jpg" /> is the signal and <img src="7-3400209\ffecf6df-00b8-43da-bf90-b3089805d8ef.jpg" /> is the window. The shifting m and the frequency ω are discrete since the STFT in most typical applications is performed on a computers or microprocessors using the Fast Fourier Transform algorithm FFT.</p><p>The magnitude squared of the STFT yields the Spectrogram of the function:</p><p><img src="7-3400209\7d274924-8f3a-4693-a239-95699be93441.jpg" /></p><p>which shows the distribution of the power spectral density of the signal <img src="7-3400209\bee59fb1-181f-4e3a-9447-f4d81b694632.jpg" /> [9,10]. The time and frequency marginals of STFT were defined as</p><p><img src="7-3400209\9c1f5659-a4b5-4715-85e4-d4c7d0ff4561.jpg" />and</p><p><img src="7-3400209\1f9c6f40-d0bf-47a4-9ebb-c713cc3aeadf.jpg" />where N is the frequency samples and M is the number of time frames.</p></sec><sec id="s1_2"><title>1.2. Wiener Filtering</title><p>The wiener masking is an estimate that can be found by minimizing the mean-square error [<xref ref-type="bibr" rid="scirp.22124-ref11">11</xref>],</p><p><img src="7-3400209\4545cf2f-3816-4300-a6d7-5d44b39ee7de.jpg" /></p><p>where <img src="7-3400209\12c848b9-cc9a-4fc0-a94d-6ec752029828.jpg" /> is the output of a linear time-varying mask.</p><p>In order to minimized the error, the estimator was defined in [<xref ref-type="bibr" rid="scirp.22124-ref11">11</xref>] to have the following Wold-Cramer representation</p><p><img src="7-3400209\cff0831f-3783-41f8-b8d5-bed2cdb0bfcd.jpg" /></p><p>where <img src="7-3400209\a23b5438-9b1c-410e-9307-f0ac64cbe0ed.jpg" /> is the evolutionary time-frequency kernel of the signal<img src="7-3400209\ea3f1909-3d53-4201-b93a-8809f828db3f.jpg" />, and <img src="7-3400209\541c28dc-7345-472d-92fe-ef1e6a83147b.jpg" /> is the masking function [12-14].</p><p>According to orthogonality principles the minimization of <img src="7-3400209\46d4a97b-18d5-43d5-abfe-811403e99018.jpg" /> is</p><p><img src="7-3400209\d62d52b5-0ec5-44ee-83cb-457fe4384e23.jpg" /></p><p>and is equivalent to</p><p><img src="7-3400209\6c0b1a85-b98f-4dab-8059-ea2e7d681420.jpg" /></p><p>where<img src="7-3400209\513fb0e8-9cbb-4799-9b8f-da9d352960e0.jpg" />.</p><p>To minimize the above equation <img src="7-3400209\8b1d28ae-7577-4eb5-b8f2-e9fcb88676ae.jpg" /> must equal to</p><p><img src="7-3400209\c0fb2e60-6d31-4e16-abf9-4b458bf48c57.jpg" /></p><p>to give the mask</p><disp-formula id="scirp.22124-formula133592"><label>(1)</label><graphic position="anchor" xlink:href="7-3400209\9eb415bb-1398-42c3-ac70-363ac393893f.jpg"  xlink:type="simple"/></disp-formula><p>as the ratio of the spectra of the reference signal <img src="7-3400209\f87670e6-ee49-49bc-aedc-8130833e7cc6.jpg" /> and that of the true received signal<img src="7-3400209\67df06f8-c1c3-4daf-89f1-b38b8a00724b.jpg" />.</p></sec></sec><sec id="s2"><title>2. Signal Segmentation from Improved Time-Frequency Plane</title><p>The regular time-frequency kernel obtained from STFT or Spectrogram does not completely satisfy the time and frequency marginals of the signal. Any further improvement in terms of kernel’s time and frequency resolution will make it possible for the estimated kernel to closely satisfy time marginal condition. Theoretically, our scheme has the capability of providing the necessary improvements according to the following:</p><p>1) For constructing the Spectrogram or STFT, a prober window type with optimal length has to occur first in order to get the desirable level of time and frequency resolution. Furthermore, a high resolution of the power spectral or energy density will provide a good estimate of both time and frequency marginals who are the key success factors leading to optimal signal segmentation.</p><p>2) Improving the joint time-frequency power spectral density by means of Wiener masking scheme will suppress and mitigate any undesired non-stationary noise or interference. The wiener masking scheme has to be applied into the time-frequency kernel obtained from STFT and not directly to the signal itself.</p><p>The block diagram of the proposed system is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref> where a white Gaussian noise is added to the original signal to give<img src="7-3400209\518e3aec-ef1a-472e-b103-c89af8b6607b.jpg" />, as the real time signal.</p><p>At the processing side, the STFT algorithm was performed to compute the time-frequency kernel for both received and reference signals as the only two required inputs for Wiener masking,</p><disp-formula id="scirp.22124-formula133593"><label>(2)</label><graphic position="anchor" xlink:href="7-3400209\27a876d5-7152-4060-9983-6a5386056480.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.22124-formula133594"><label>(3)</label><graphic position="anchor" xlink:href="7-3400209\39bf27e0-d706-4442-9433-4732a7250f6c.jpg"  xlink:type="simple"/></disp-formula><p>The experimental testing of several known windows shows that hamming window with a length<img src="7-3400209\6ace6fb0-b18d-4662-a08b-d573b870d8d8.jpg" />, and time shift <img src="7-3400209\35e6918c-c6ac-46fa-b71d-19ea4ef735e5.jpg" /> gives the highest desirable time and frequency resolution.</p><p>The mask <img src="7-3400209\2204100e-d0f3-4eba-9605-afc6de43b1a4.jpg" /> defined in (1) then can be created from the two above kernels to be</p><disp-formula id="scirp.22124-formula133595"><label>(4)</label><graphic position="anchor" xlink:href="7-3400209\fe72d541-4849-44f5-9875-5eadf5061b3d.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="7-3400209\e4806f2c-36b0-4586-9e8a-11ad136e0d21.jpg" />, and <img src="7-3400209\5f8f138c-d3f1-4544-b249-4dee8da5186c.jpg" /> are the spectrum of the reference and received signal respectively.</p><p>The improved time-frequency spectrum can be obtained using the mask <img src="7-3400209\2e4d483a-0625-41af-9f62-fa9897c8abe7.jpg" /> to get</p><disp-formula id="scirp.22124-formula133596"><label>(5)</label><graphic position="anchor" xlink:href="7-3400209\ab0b20dd-8c42-4089-9c53-b0902b706198.jpg"  xlink:type="simple"/></disp-formula><p>or</p><disp-formula id="scirp.22124-formula133597"><label>(6)</label><graphic position="anchor" xlink:href="7-3400209\fa036d7c-6792-4eaa-8054-9c3e81839b61.jpg"  xlink:type="simple"/></disp-formula><p>as an estimate of the original time-frequency kernel of the processed signal.</p><p>The time marginal of the improved time-frequency spectrum Y<sub>m</sub> can be obtain as</p><disp-formula id="scirp.22124-formula133598"><label>(7)</label><graphic position="anchor" xlink:href="7-3400209\6558cbbd-9899-43ed-aa49-1703f120247a.jpg"  xlink:type="simple"/></disp-formula><p>and its length equals to the total number of overlapping segments or time window frames that comes from chunking or windowing the original signal using the widow<img src="7-3400209\941c049e-4f71-4683-ad4f-cf250cb9bee4.jpg" />.</p><p>Unfortunately, in STFT the time marginal does not satisfy time marginal, <img src="7-3400209\b7ebc62e-3657-4fa9-9c52-2b92c41e986a.jpg" />condition and therefore will not give the correct signal segmentation to indicate the boundary of its amplitude or frequency changes. Further signal processing is needed at this stage and nonlinear interpolation must be employed to interpolate the data signal to the original data points. Due to the nonlinearity of the function<img src="7-3400209\d350301d-cc4c-4417-ace8-9e0878cfd14c.jpg" />, a second order Lagrangian interpolation polynomial is used as</p><disp-formula id="scirp.22124-formula133599"><label>(8)</label><graphic position="anchor" xlink:href="7-3400209\1e800006-47e9-49a6-a978-3ff2dc01c7ef.jpg"  xlink:type="simple"/></disp-formula><p>where n stands for the n<sup>th</sup> order polynomial and</p><disp-formula id="scirp.22124-formula133600"><label>(9)</label><graphic position="anchor" xlink:href="7-3400209\f6cfdb54-0529-4eab-b657-5fbfa735d58e.jpg"  xlink:type="simple"/></disp-formula><p>is a weighting function that includes a product on <img src="7-3400209\5a069d4a-1e94-442a-ac65-f89148380e49.jpg" /> terms with terms of j = 1 omitted. The resulted interpolated function then has a time samples of length equals to the length of the original signal.</p></sec><sec id="s3"><title>3. Simulation and Results</title><p>To prove the validity of our approach we will carry it out to a real application and running its algorithms for a multi-component signal and therefore, we will be able to display the TF kernel and its marginals. Now, let us consider the following multi-component signal<img src="7-3400209\d9c3af53-3514-41fe-ab5f-43749f7aefc6.jpg" />,</p><p><img src="7-3400209\fece8650-505e-42d4-9a18-d8b5b42e4bc6.jpg" /></p><p>is composed of three equal segments each with different frequency. A white Gaussian noise is added to the total signal to give<img src="7-3400209\73262bc9-a573-4402-995e-8171f802a892.jpg" />, and with a signal to noise ratio SNR equal to 3 dB, as one of the worst cases when the interference noise has a large power. The noisefree signal and the corrupted one are shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) and (b) respectively.</p><p>According to our segmentation system shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, the STFT is applied for both, the noise-free signal<img src="7-3400209\401833de-13f7-4b4d-be30-b3b576da7e9e.jpg" />, and the reference signal<img src="7-3400209\b0460665-fe06-4a1e-bb2f-cd0a5c92dd39.jpg" />. The two spectrums are computed to be used as the input values for the Wiener mask. The TF spectrum of the noisy signal is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref> which displays the effect of the Gaussian noise. We notice that the energy components of the noise is spread all over the entire TF plane displaying a poor time marginal.</p><p>The Wiener masking scheme is applied according to the algorithm defined in (5) (6), and the estimated TF kernel obtained from the Wiener masking output is shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>. Notice that the power of the interference noise has been mitigated allowing to estimate a noise-less TF kernel of the processed signal<img src="7-3400209\8d68d4bf-ef23-4432-8c5f-87fa1ef53fbe.jpg" />. As expected, this estimated/computed kernel provides a better time marginal that will enhance the segmentation process.</p><p>In fact, the estimated function which represents the time marginal defined in (7) has a length equals to the total number of signal frames or windows and is less than the signal length. Therefore, this segmentation function needs to be interpolated to equal length of the original signal as defined in (8) and (9). Figures 4(a)-(d) displays the results starting from the noise-free signal<img src="7-3400209\921d9c10-259b-4ed2-a737-4eef086b2e9b.jpg" />, noisy signal<img src="7-3400209\1ca68b83-902c-4f7b-a0eb-56685d6ec1c8.jpg" />, poor time marginal function <img src="7-3400209\228bff79-9616-4c63-857f-242a4ad28565.jpg" /> obtained from the noisy TF kernel, and finally the estimated time marginal function <img src="7-3400209\4323d218-7e96-4340-986d-1b78caa6662c.jpg" /> computed from the improved TF kernel. The computed time marginal function <img src="7-3400209\88a0d6bf-14cb-4e90-9891-72506a1ab14a.jpg" /> shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>(d) provides the desired segmentations of the signal which identifies the boundaries between any two candidate segments.</p></sec><sec id="s4"><title>4. Conclusion</title><p>We have shown that with an efficient windowing for Short-time Fourier transform followed by 2-D Wiener filtering will provide a strong segmentation scheme which separates the multi-segments of non-stationary signals. In this work we have considered the 2-D Wiener masking or filtering to improve the resolution of the time-frequency kernel as crucial step which provides a good estimate of the time marginal. We should also mention that this approach depends mainly on the prober selection of the sliding window and its length for the STFT.</p></sec><sec id="s5"><title>5. Acknowledgements</title><p>This article was funded by Deanship of Scientific Research (DSR), King Abdulaziz University, Jeddah. The author, therefore, acknowledges with thanks DSR technical and financial support.</p></sec><sec id="s6"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.22124-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">C. Panagiotakis and G. Tziritas, “A Speech/Music Discriminator Based on RMS and Zero-Crossing,” IEEE Transactions on Multimedia, Vol. 7, No. 1, 2005, pp. 155-166. doi:10.1109/TMM.2004.840604</mixed-citation></ref><ref id="scirp.22124-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">S. Mahmoodi and B. Sharif, “Signal Segmentation and Denoising Algorithm Based on Energy Optimization,” Signal Processing, Vol. 85, No. 9, 2005, pp. 1845-1851.  
doi:10.1016/j.sigpro.2005.03.016</mixed-citation></ref><ref id="scirp.22124-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">H. Azami, K. Mohammadi and B. Bozorgtabar, “An Improved Signal Segmentation Using Moving Average and Savitzky-Golay Filter,” Journal of Signal and Information Processing, Vol. 3, No. 1, 2012, pp. 39-44.  
doi:10.4236/jsip.2012.31006</mixed-citation></ref><ref id="scirp.22124-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">H. Hassanpour and S. M. Anisheh, “An Improved Adaptive Signal Segmentation Method Using Fractal Dimension,” IEEE Conference on Information Science, Signal Processing and their Applications, Kuala Lumpur, 10-13 May 2010, pp. 720-723.</mixed-citation></ref><ref id="scirp.22124-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">S. M. Anisheh and H. Hassanpour, “Adaptive Segmentation with Optimal Window Length Scheme using Fractal Dimension and Wavelet Transform,” International Journal of Engineering, Vol. 22, No. 3, 2009, pp. 257-268.</mixed-citation></ref><ref id="scirp.22124-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">G. Proakis and M. Salehi, “Communication Systems Engineering,” Prentice Hall, Upper Saddle River, 1994.</mixed-citation></ref><ref id="scirp.22124-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">R. G. Lyons, “Digital Signal Processing,” Prentice Hall, Upper Saddle River, 2004. </mixed-citation></ref><ref id="scirp.22124-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">L. Cohen, “Time-Frequency Analysis,” Prentice Hall, Englewood Cliffs, 1995.</mixed-citation></ref><ref id="scirp.22124-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">M. H. Ackroyd, “Short-Time Spectra and Time-Fre- quency Energy Distributions,” Journal of Acoustical Society of America, Vol. 50, No. 5A, 1971, pp. 1229-1231.  
doi:10.1121/1.1912761</mixed-citation></ref><ref id="scirp.22124-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">R. Suleesathira, L. F. Chaparro and A. Akan, “Discrete Volutionary Transform for Time-Frequency Signal Ana- lysis,” Journal of the Franklin Institute, Vol. 337, No. 4, 2000, pp. 347-364.</mixed-citation></ref><ref id="scirp.22124-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">H. Khan and L. F. Chaparro, “Formulation and Implementation of the Non-Stationary Evolutionary Wiener Filtering,” Signal Processing, Vol. 76, No. 3, 1999, pp. 243-267. </mixed-citation></ref><ref id="scirp.22124-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">L. F. Chaparro and A. A. Alshehri, “Jammer Excision in Spread Spectrum Communications via Wiener Masking and Frequency-Frequency Evolutionary Transform,” 2003 IEEE International Conference on Acoustics, Speech, and Signal Processing, Vol. 4, 6-10 April 2003, pp. 473-476.</mixed-citation></ref><ref id="scirp.22124-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">L. F. Chaparro, R. Suleesathira, A. Akan and B. Unsal, “Instantaneous Frequency Estimation Using Discrete Evolutionary Transform for Jammer Excision,” 2001 IEEE International Conference on Acoustics, Speech, and Signal Processing, Salt Lake City, 7-11 May 2001, pp. 3525-3528.</mixed-citation></ref><ref id="scirp.22124-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">A. A. Alshehri, L. F. Chaparro and A. Akan, “Evolutionary Wiener Mask Receiver for Multiuser Direct Sequence Spread Spectrum,” Proceedings of EUSIPCO-2005, September 2005.</mixed-citation></ref></ref-list></back></article>