<?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">ENG</journal-id><journal-title-group><journal-title>Engineering</journal-title></journal-title-group><issn pub-type="epub">1947-3931</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/eng.2021.131005</article-id><article-id pub-id-type="publisher-id">ENG-106801</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject></subj-group></article-categories><title-group><article-title>
 
 
  Non-Cooperative Spectrum Sensing Based on Cyclostationary Model of Digital Signals in the Context of Cognitive Radio
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jean-Marie</surname><given-names>Kadjo</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>Raoule</surname><given-names>Agoua</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>Aliou</surname><given-names>Bamba</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>Adama</surname><given-names>Konaté</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>Olivier</surname><given-names>Asseu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>LASTIC, ESATIC, Abidjan, C&amp;amp;#244;te d’Ivoire</addr-line></aff><pub-date pub-type="epub"><day>12</day><month>01</month><year>2021</year></pub-date><volume>13</volume><issue>01</issue><fpage>56</fpage><lpage>70</lpage><history><date date-type="received"><day>18,</day>	<month>December</month>	<year>2020</year></date><date date-type="rev-recd"><day>24,</day>	<month>January</month>	<year>2021</year>	</date><date date-type="accepted"><day>27,</day>	<month>January</month>	<year>2021</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>
 
 
  This paper addresses the problem of the opportunistic spectrum access in Cognitive Radio. Indeed, most spectrum sensing algorithms suffer from a high computational cost to achieve the detection process. They need a prior knowledge of signal characteristics and present a bad performance in low Signal to Noise Ratio (SNR) environment. The choice of the optimal detection threshold is another issue for these spectrum sensing algorithms. To overcome the limits of spectrum detectors, we propose in this paper, a blind detection method based on the cyclostationary features of communication signals. Our detector evaluates the level of hidden periodicity contained in the observed signal to make decision on the state of a bandwidth. In order to reduce the computational cost, we take advantage of the FFT Accumulation Method to estimate the cyclic spectrum of the observed signal. Then, we generate the Cyclic Domain Profile of the cyclic spectrum which allows us to evaluate the level of the hidden periodicity in the signal. This level of periodicity is quantified through the crest factor of Cyclic Domain Profile, which represents the decision statistic of the proposed detector. We have established the analytic expression of the optimal threshold of the detection and the probability of detection to evaluate the performance of the proposed detector. Simulation results show that the proposed detector is able to detect the presence of a communication signal on a bandwidth in a very low SNR scenario.
 
</p></abstract><kwd-group><kwd>Spectrum Sensing</kwd><kwd> Cyclostaionarity</kwd><kwd> FFT Accumulation Method</kwd><kwd> Cyclic Spectrum</kwd><kwd> Spectrum Coherence</kwd><kwd> Cognitive Radio</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In this paper, we propose the Cyclostationary Features based Detection (CFD) algorithm based on a spectral analysis of the cyclostationarity of digital communications signals. By definition, a cyclostationary process is a random process in which the statistical characteristics are periodic or quasi-periodic [<xref ref-type="bibr" rid="scirp.106801-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref3">3</xref>]. The strategy of detection based on cyclostationarity consists of developing algorithms to detect hidden periodicities of the observed signal. In digital communications, this cyclostationarity is due to coding, multiplexing and modulation techniques, which generate hidden frequencies in the spectrum of the transmitted signal [<xref ref-type="bibr" rid="scirp.106801-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref5">5</xref>]. Since the detection of an unoccupied frequency band amounts to detect the presence or absence of a communication signal on this frequency band, a spectral analysis of the cyclostationarity of the received signal can then help in the detection of unoccupied spectral bands. The CFD acts in a non-cooperative context [<xref ref-type="bibr" rid="scirp.106801-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref7">7</xref>]. It does not require a prior knowledge of the characteristics of the PU signal and remains effective in a very low SNR channel. Our cyclostationary detection approach is divided into two main stages:</p><p>• First, we adapt the Fast Fourier transform Accumulation Method (FAM) algorithm to estimate the cyclic spectrum of the observed signal.</p><p>• Then, we generate the Cyclic Domain Profile (CDP) which allows us to evaluate the level of the hidden periodicity in the signal. This level of periodicity is quantified through the Crest Factor (CF) of CDP, which represents the decision statistic of CFD.</p><p>During the detection phase, the CFD compares the CF of the received signal to a predetermined threshold. The simulations which we carried out through the Receiver Operating Characteristic (ROC) curves show the robustness of our detection method.</p><p>The rest of this paper is organized into five sections. In Section 2, we briefly present the properties of cyclostationary processes. Section 4 presents the FAM algorithm used to estimate the cyclic spectrum. The principle of the detector is presented in Section 5. We end this paper with Sections 6 and 7 which respectively present the results of our simulations and the conclusion.</p></sec><sec id="s2"><title>2. Cyclostationnarity</title><p>The first works on the cyclostationarity of communication signals were published in 1958 by Bennett [<xref ref-type="bibr" rid="scirp.106801-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref8">8</xref>]. Subsequently, Gudzenko [<xref ref-type="bibr" rid="scirp.106801-ref9">9</xref>], Markelov [<xref ref-type="bibr" rid="scirp.106801-ref10">10</xref>] and Gladyshev [<xref ref-type="bibr" rid="scirp.106801-ref11">11</xref>] will be interested in the theory of cyclostationarity and study various aspects including the non-parametric spectral analysis of processes Cyclostationnaire (CS) [<xref ref-type="bibr" rid="scirp.106801-ref9">9</xref>], the study of CS processes in a Gaussian context [<xref ref-type="bibr" rid="scirp.106801-ref10">10</xref>] and the analysis of processes Almost Cyclo-Stationnary (ACS) [<xref ref-type="bibr" rid="scirp.106801-ref11">11</xref>]. In a series of publications, Herbst provides tools for analyzing periodic or nearly periodic variance processes [<xref ref-type="bibr" rid="scirp.106801-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref15">15</xref>]. Kamp&#233; de F&#233;rier [<xref ref-type="bibr" rid="scirp.106801-ref16">16</xref>] and Parzen [<xref ref-type="bibr" rid="scirp.106801-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref18">18</xref>] for their part are interested in the spectral analysis of the cyclostationarity of natural phenomena and Monin [<xref ref-type="bibr" rid="scirp.106801-ref19">19</xref>] proposes the use of cyclostationarity in the analysis of weather data. One of the pioneers of cyclostationarity since the 1980s is William Gardner who, apart from the probabilistic theory of cyclostationarity developed by Gladyshev [<xref ref-type="bibr" rid="scirp.106801-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref22">22</xref>], lays the foundations of the non-probabilistic theory of cyclostationarity [<xref ref-type="bibr" rid="scirp.106801-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref24">24</xref>]. This non-probabilistic theory consists of extracting sinusoidal components by a quadratic transformation of the cyclostationary signal. However, the two approaches (probabilistic and non-probabilistic) give similar results and are linked by the cyclo-ergodicity of cyclostationary processes. This cyclo-ergodicity states that the limits of the temporal averages and the statistical averages of the cyclic characteristics converge towards the same values [<xref ref-type="bibr" rid="scirp.106801-ref25">25</xref>].</p><p>Today, cyclostationarity is exploited in various fields including telecommunications [<xref ref-type="bibr" rid="scirp.106801-ref5">5</xref>], mechanics [<xref ref-type="bibr" rid="scirp.106801-ref26">26</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref27">27</xref>] and astronomy [<xref ref-type="bibr" rid="scirp.106801-ref28">28</xref>].</p><p>The cyclostationarity is defined as an extension of the concept of stationarity or as a special case of non-stationarity. Such a signal is defined by a periodicity at order n of its statistics [<xref ref-type="bibr" rid="scirp.106801-ref29">29</xref>]. A CS or ACS process is defined in the strict sense or in the broad sense.</p><p>Let X ( t ) be a real-value continuous-time stochastic process. The process X ( t ) is said to be Cyclo-Stationary (CS) with period T<sub>0</sub> in the strict sense of the order n if and only if its probabilistic characteristics are T<sub>0</sub>-periodic [<xref ref-type="bibr" rid="scirp.106801-ref5">5</xref>]. Which means in other words that: ∀ t ∈ ℝ ,   ∀ k ∈ ℤ ,   ∀ x ∈ ℝ n ,   ∃ T 0 ∈ ℝ + :</p><p>F X ( t ) ( x ) = F X ( t + k T 0 ) ( x ) (1)</p><p>When the process X ( t ) contains several periodicities, the process is named a polycyclostationary process. Thus, X ( t ) is said to be polyclostationary in the strict sense with the periods T 0 , T 1 , ⋯ , T P if and only if its statistical properties are periodic in time with the periods T 0 , T 1 , ⋯ , T P [<xref ref-type="bibr" rid="scirp.106801-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref25">25</xref>].</p><p>Let X ( t ) be a real-value continuous-time stochastic process. The process X ( t ) is said to be CS of period T<sub>0</sub> in the broad sense if and only if its statistics of order 1 (its mean) and of order 2 (its autocorrelation function) vary periodically over time with a period T<sub>0</sub>.</p><p>In the rest of this paper, we will focus on cyclostationarity in the wide sense to develop our CFD detector which only exploits the statistical properties of second order of the digital communications signal.</p><p>The theory of second order cyclostationarity is based on the autocorrelation function of the stochastic process. Considering that in practice, the observed signal is only one realization of the cyclostationary process, we will deal in the continuation with the second order cyclostationarity of digital communications signals.</p><p>A centered signal x ( t ) is said to be second-order cyclostationary, in the wide sense, if its autocorrelation function R x ( t , τ ) defined by:</p><p>R x ( t , τ ) ≜ E [ x ( t + τ 2 ) x * ( t − τ 2 ) ] (2)</p><p>is a T<sub>0</sub>-periodic function for each τ ; which means in other words that: ∀ k ∈ ℤ * ,</p><p>R x ( t + k T 0 , τ ) = R x ( t , τ ) (3)</p><p>where τ denotes the time offset (correlation variable). T<sub>0</sub> is called the cyclic period. It is a period hidden in the signal x ( t ) ; E [ . ] denotes the expectation [<xref ref-type="bibr" rid="scirp.106801-ref30">30</xref>].</p><p>Since the auto-correlation function R x ( t , τ ) is T<sub>0</sub>-periodic in t for each shift τ , then it can therefore be decomposed into Fourier series in the form:</p><p>R x ( t , τ ) = ∑ k = 1 K     R x k α 0 ( τ ) ⋅ e j 2 π k α 0 t (4)</p><p>where α 0 = 1 / T 0 denotes the fundamental cyclic frequency and K the number of harmonics.</p><p>The quantity R x k α 0 ( τ ) is called the cyclic correlation function [<xref ref-type="bibr" rid="scirp.106801-ref24">24</xref>]. According to [<xref ref-type="bibr" rid="scirp.106801-ref24">24</xref>], R x k α 0 ( τ ) is given by:</p><p>R x k α 0 ( τ ) ≜ 1 T 0 ∫ − T 0 2 T 0 2 R x ( t , τ ) ⋅ e − j 2 π k α 0 t d t (5)</p><p>When its autocorrelation function contains several cyclic periods (hidden periodicities) T 0 , T 1 , T 2 , ⋯ , the signal x ( t ) is said to be polycyclostationary [<xref ref-type="bibr" rid="scirp.106801-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref31">31</xref>]. The polycyclostationary model is most suitable for digital communications signals. Thus, by adopting the polycyclostationary model for the signal x ( t ) , the autocorrelation function R x ( t , τ ) of x ( t ) becomes [<xref ref-type="bibr" rid="scirp.106801-ref31">31</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref32">32</xref>]:</p><p>R x ( t , τ ) ≜ ∑ α ∈ A R x α ( τ ) ⋅ e j 2 π α t (6)</p><p>where A = { α 0 , α 1 , ⋯ , α N } is a numbered set containing all the possible cyclic frequencies α and the Fourier coefficients R x α ( τ ) .</p><p>R x α ( τ ) ≜ l i m T → ∞ 1 T ∫ − T 2 T 2     R x ( t , τ ) ⋅ e − j 2 π α t d t (7)</p><p>denote the cyclic autocorrelation function.</p><p>By analogy with the Power Spectral Density, the Fourier transform of the cyclic autocorrelation function is called density function of the cyclic correlation or cyclic spectrum [<xref ref-type="bibr" rid="scirp.106801-ref24">24</xref>]:</p><p>S x α ( ν ) ≜ ∫ − ∞ + ∞   R x α ( τ ) ⋅ e − j 2 π ν τ d τ (8)</p><p>The estimation of the quantities defined by Equations (7) and (8) constitutes the cyclic spectral analysis.</p></sec><sec id="s3"><title>3. Cyclic Spectral Analysis</title><p>Let w ( t ) be a sliding window of unit area and not zero over the interval [ − T 2 , T 2 ] . The adequate estimator of the cyclic autocorrelation function R x α ( τ )</p><p>of the observation x ( t ) for t ∈ [ t 0 − T / 2 , t 0 + T / 2 ] is the cyclic correlogram R x ( T ) ( α , t ) defined by [<xref ref-type="bibr" rid="scirp.106801-ref31">31</xref>]:</p><p>R x ( T ) ( α , τ ) ≜ ∫ ℝ     w ( t − t 0 ) x ( t + τ ) x &#175; ( t ) e − j 2 π α t d t (9)</p><p>x &#175; represents the conjugate of x ( t ) . The cyclic correlogram R x ( T ) ( α , τ ) is a consistent estimator of R x α ( τ ) [<xref ref-type="bibr" rid="scirp.106801-ref31">31</xref>]. The letter T superscript of R x ( T ) ( α , τ ) denotes the width of the sliding window w ( t ) .</p><p>Assuming w ( t ) = r e c t ( t / T ) / T , we show that the cyclic autocorrelation function is equivalent to [<xref ref-type="bibr" rid="scirp.106801-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref33">33</xref>]:</p><p>R x ( T ) ( α , τ ) = 1 T ∫ − T 2 + T 2   x ( t + τ 2 ) x &#175; ( t − τ 2 ) ⋅ e − j 2 π α t d t (10)</p><p>By introducing e − j π α ( τ 2 − τ 2 ) = 1 into the equation eqref Equation Autocor Cyclic2, we end up with:</p><p>R x ( T ) ( α , τ ) = 1 T ∫ − T 2 T 2   x ( t + τ 2 ) e − j 2 π α ( t + τ 2 ) x &#175; ( t − τ 2 ) e − j 2 π α ( t − τ 2 ) d t = 1 T { z ( α , τ ) ∗ z &#175; ( α , − τ ) } (11)</p><p>where z ( α , τ ) = x ( t + τ 2 ) e − j 2 π α ( t + τ 2 ) and * denotes the convolution product operator.</p><p>The Fourier transform of the cyclic correlogram R x ( T ) ( α , τ ) gives the cyclic periodogram I ( T ) ( α , ν ) [<xref ref-type="bibr" rid="scirp.106801-ref31">31</xref>]:</p><p>I ( T ) ( α , ν ; t ) ≜ 1 T T F { R x ( T ) ( α , τ ) } = 1 T T F { z ( α , τ ) ∗ z &#175; ( α , − τ ) } = 1 T X T ( t , ν + α 2 ) X &#175; T ( t , ν − α 2 ) (12)</p><p>where X T ( t , ν ) is the Short Term Fourier Transform of x ( t ) defined as follows:</p><p>X T ( t , ν ) ≜ ∫ t − T 2 t + T 2     x ( u ) e − j 2 π ν u d u (13)</p><p>X T ( t , ν + α 2 ) is named the complex demodulate [<xref ref-type="bibr" rid="scirp.106801-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref34">34</xref>].</p><p>The cyclic periodogram I ( T ) ( α , ν ; t ) is a non-consistent estimator of the cyclic spectrum S x α ( ν ) . As in the case of stationary processes, consistency can be obtained by temporal or frequency averaging of I ( T ) ( α , ν ; t ) . We then obtain two estimators of the cyclic spectrum: the frequency-averaged cyclic periodogram G x ( Δ t , Δ ν ) ( α , ν ) and the time-averaged cyclic periodogram S x ( Δ t , Δ ν ) ( α , ν ) [<xref ref-type="bibr" rid="scirp.106801-ref31">31</xref>]:</p><p>G x ( Δ t , Δ ν ) ( α , ν ) = 1 Δ ν ∫ ν − Δ ν / 2 ν + Δ ν / 2     I ( Δ t ) ( α , λ ; t ) d λ (14)</p><p>S x ( Δ t , Δ ν ) ( α , ν ) = 1 Δ t ∫ t 0 − Δ t / 2 t 0 + Δ t / 2     I ( 1 / Δ ν ) ( α , ν ; t ) d t (15)</p><p>with Δ t the duration of observation of the signal x ( t ) and Δ ν the frequency resolution.</p><p>S x ( Δ t , Δ ν ) ( α , ν ) and G x ( Δ t , Δ ν ) ( α , ν ) are defined by a frequency resolution Δ ν and a cyclic frequency resolution Δ α .</p><p>Δ t denotes the duration of observation of the signal x ( t ) and T the duration (or width) of the sliding window (apodization window), we have [<xref ref-type="bibr" rid="scirp.106801-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref31">31</xref>]:</p><p>Δ α = 1 Δ t (16)</p><p>Δ ν = 1 T (17)</p><p>To obtain a fine estimate of the cyclic spectrum, the Grenander uncertainty condition must be respected [<xref ref-type="bibr" rid="scirp.106801-ref35">35</xref>]:</p><p>Δ t ⋅ Δ ν ≫ 1 (18)</p><p>It states that for a better estimate of the cyclic spectrum, the duration T of the apodization window w ( t ) must be much less than the observation duration Δ t of the signal x ( t ) to analyze [<xref ref-type="bibr" rid="scirp.106801-ref35">35</xref>].</p><p>The estimators S x ( Δ t , Δ ν ) ( α , ν ) and G x ( Δ t , Δ ν ) ( α , ν ) of S x α ( ν ) are asymptotically equivalent [<xref ref-type="bibr" rid="scirp.106801-ref31">31</xref>]:</p><p>lim Δ ν → 0 lim Δ t → ∞ S x ( Δ t , Δ ν ) ( α , ν ) = lim Δ ν → 0 lim Δ t → ∞ G x ( Δ t , Δ ν ) ( α , ν ) = S x α ( ν ) (19)</p><p>However, in [<xref ref-type="bibr" rid="scirp.106801-ref34">34</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref35">35</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref36">36</xref>], the authors show that the cyclic spectrum estimators based on temporal smoothing are more efficient in terms of computation time and provide a finer estimate.. Consequently, we will focus in the rest of our work in methods based on temporal smoothing. The most used temporal smoothing algorithms are:</p><p>• FAM [<xref ref-type="bibr" rid="scirp.106801-ref36">36</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref37">37</xref>] algorithm;</p><p>• Spectral Correlation Algorithm (SSCA) algorithm [<xref ref-type="bibr" rid="scirp.106801-ref36">36</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref37">37</xref>].</p><p>The FAM algorithm is faster and more efficient than the SSCA algorithm. Our detection model therefore uses the FAM algorithm to estimate the cyclic spectrum of the observed signal.</p></sec><sec id="s4"><title>4. FFT Accumulation Method</title><p>Let x ( n ) , n ∈ ℤ be the discrete signal obtained by uniform sampling of the continuous signal x ( t ) , t ∈ ℝ . Let N be the number of samples observed during the duration Δ t , Δ t = N T e and N P the number of samples contained in the sliding window w ( n ) ; T = N P T e ; T e denotes the sampling period. The cyclic spectrum estimator by time averaging is written [<xref ref-type="bibr" rid="scirp.106801-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref38">38</xref>]:</p><p>S x ( N , 1 N P ) ( α , ν ) = 1 N ∑ n = 0 N − 1 1 N P X T ( n , ν + α 2 ) X &#175; ( n , ν − α 2 ) = 1 N ∑ n = 0 N − 1 1 N P T F { w ( k ) x ( n − k ) e − j 2 π ( α 2 ) ( n − k ) T e }     T F { [ w ( k ) x ( n − k ) &#175; ] e + j 2 π ( α 2 ) ( n − k ) T e } (20)</p><p>The FAM algorithm for Fast Fourier Transform Accumulation Method, based on Equation (20), takes advantage of the advantages of the Fast Fourier Transform (Fast Forier Transform (FFT)) to reduce the computational cost of the spectrum cyclic. It divides the dual-frequency plane ( ν , α ) into sub-blocks</p><p>( ν i , α i ), then calculates the estimates of the cyclic spectrum S x ( N , 1 N P ) ( α i , ν i ) of each sub-block using the FFT. It is constitued of three main stages:</p><p>1) The computation of complex demodulates X T ( n , ν + α 2 ) and of their conjugates X &#175; T ( n , ν − α 2 ) to obtain the spectral composition of the signal.</p><p>2) The two-by-two product between complex demodules and their conjugates corresponds to the calculation of the cyclic correlogram</p><p>I ( T ) ( α , ν ; n ) = 1 T X T ( n , ν + α 2 ) X &#175; T ( n , ν − α 2 ) .</p><p>3) The computation of FFT of I ( T ) ( α , ν ; n ) to obtain the estimation of cyclic spectrum S x ( N , 1 N P ) ( α , ν ) .</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref> summerizes the different stages of FAM algorithm.</p></sec><sec id="s5"><title>5. Detection Modeling</title><p>Let s ( t ) be the signal of the primary user (PU) and y ( t ) the signal observed by the secondary user (SU):</p><p>y ( t ) = θ ⋅ h ( t ) s ( t ) + b ( t ) (21)</p><p>where h ( t ) denotes the impulse response of the channel, θ a Boolean variable and b ( t ) a Gaussian white noise of variance σ b 2 .</p><p>The hypotheses H 0 and H 1 are as follows:</p><p>• H 0 : no communication signal; θ = 0 ;</p><p>• H 1 : communication signal presence; θ = 1 .</p><p>The fundamental idea of detection consists in measuring the level of hidden periodicity in the signal y ( t ) .</p><p>To measure this hidden periodicity, we first define the Cyclic Domain Profile or CDP D ( α ) which contains the maximum values of the cyclic spectrum S y α ( ν ) :</p><p>D ( α ) = max ν ‖ S y α ( ν ) ‖ (22)</p><p>Next, we define the crest factor F c of the CDP D ( α ) which will serve as the decision statistic T C F D of the CFD:</p><p>T C F D = F c = max α D ( α ) 1 2 N ∑ k = 1 2 N D 2 ( α k ) (23)</p><p>The detection criterion is given by:</p><p>T C F D ≷ H 0 H 1 λ C F D (24)</p><p>λ C F D is the detection threshold predetermined according to the desired P f a [<xref ref-type="bibr" rid="scirp.106801-ref39">39</xref>].</p><p>In order to analytically approach the optimal detection threshold λ C F D , we must estimate the Probability Density Function (PDF) of the crest factor F c under H 0 . Equation (23) shows that the calculation of F c is based on a maximization function; we can therefore approach the PDF of F c both under H 0 and under H 1 by the PDF f Z ( z ) of generalized extreme value or Generalized Extreme Value (GEV) of parameters ( μ , σ , ξ ) defined by [<xref ref-type="bibr" rid="scirp.106801-ref40">40</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref41">41</xref>] [<xref ref-type="bibr" rid="scirp.106801-ref42">42</xref>]:</p><p>f Z ( z ) = 1 σ ( 1 + ξ z − μ σ ) ( − 1 ξ − 1 ) exp [ − ( 1 + ξ z − μ σ ) − 1 / ξ ] (25)</p><p>with μ location parameter; σ the scale parameter and ξ ∈ ℝ the shape parameter.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows us the evolution of F c under H 0 and under H 1 for a SNR = −11 dB. We define the probability of false alarm P f a by:</p><p>P f a = ∫ λ C F D + ∞   f Z / H 0 ( z ) d z (26)</p><p>with:</p><p>{ μ 0 = μ / H 0 σ 0 = σ / H 0 ξ 0 = ξ / H 0 (27)</p><p>P f a becomes as follows:</p><p>P f a = ∫ λ C F D + ∞ 1 σ 0 [ 1 + ξ 0 z − μ 0 σ 0 ] − 1 ξ 0 − 1 exp [ − ( 1 + ξ 0 z − μ 0 σ 0 ) − 1 / ξ 0 ] d z (28)</p><p>Using the change of variable u = 1 + ξ 0 z − μ 0 σ 0 , we obtain:</p><p>P f a = 1 ξ 0 ∫ ( 1 + ξ 0 λ C F D − μ 0 σ 0 ) + ∞ 1 u u ξ 0 exp [ 1 u ξ 0 ] d u = [ exp [ − u − 1 / ξ 0 ] ] ( 1 + ξ 0 λ C F D − μ 0 σ 0 ) + ∞ P f a = 1 − exp [ − ( 1 + ξ 0 λ C F D − μ 0 σ 0 ) − 1 / ξ 0 ] (29)</p><p>From Equation (29), we determine the optimal detection threshold λ C F D as follows:</p><p>λ C F D = σ 0 ξ 0 [ ( ln ( 1 1 − P f a ) ) − ξ 0 − 1 ] + μ 0 (30)</p><p>With:</p><p>{ μ 1 = μ / H 1 σ 1 = σ / H 1 ξ 1 = ξ / H 1 (31)</p><p>the probability of detection P d can be defined by:</p><p>P d = ∫ λ + ∞ f Z / H 1 ( z ) d z P d = 1 − e − [ 1 + ξ 1 λ − μ 1 σ 1 ] − 1 / ξ 1 (32)</p><p>Equations (29) and (32) allow to establish the relation between P d et al. P f a :</p><p>P d = 1 − exp { − [ 1 + ξ 1 σ 0 ξ 0 [ ( ln ( 1 1 − P f a ) ) − ξ 0 − 1 ] + μ 0 − μ 1 σ 1 ] − 1 / ξ 1 } (33)</p><p>A delicate part in this approximation is the estimation of the parameters ξ , σ , k of the probability density function GEV. To do this, we use the Optimal Biased Robust Estimator (OBRE) algorithm proposed in [<xref ref-type="bibr" rid="scirp.106801-ref40">40</xref>] to estimate the parameters μ , σ and ξ . OBRE is a robust estimator based on Maximum Likelihood or gls mle. <xref ref-type="table" rid="table1">Table 1</xref> gives some values of the parameters μ , σ and ξ of the GEV probability density function of F c under H 1 obtained for different values of SNR.</p></sec><sec id="s6"><title>6. Simulations and Results</title><p>In order to compare the theoretical and experimental results, we generate the performance curves P d as a function of Signal Noise Ratio (SNR) and the Reciever Operating Characteristics (ROC) curves. These simulations are performed on different types of signals (16-QAM, QPSK, BPSK, 4-ASK). We group the simulation parameters in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> shows a concordance between the theoretical and experimental performance curves P d as a function of SNR for a 16-QAM signal. We generated the theoretical curve from Equation (33) and the experimental curve using Monte Carlo simulations (1000 iterations). Thus according to the theory, our detector is able to detect a communication signal in a Gaussian channel as soon as the signal to noise ratio SNR ≥ −11 dB with a detection probability P d = 0.9 for a P f a = 0.05 . These results are consistent with those obtained experimentally.</p><p>To analyse the evolution of the P d as a function of the P f a , we use the roc curves. <xref ref-type="fig" rid="fig4">Figure 4</xref> gives the theoretical and experimental ROC curves of the CFD on a 16-QAM signal in a Gaussian channel with a SNR = −11 dB. The theoretical curve is generated by Equation (33) and the experimental curve is obtained by Monte Carlo simulations. We can note through these results the similarity between the two curves.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Value of μ , σ and ξ under H 1 based on the SNR</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >SNR (dB)</th><th align="center" valign="middle" >−14</th><th align="center" valign="middle" >−12</th><th align="center" valign="middle" >−10</th><th align="center" valign="middle" >−9</th><th align="center" valign="middle" >−8</th><th align="center" valign="middle" >−7</th><th align="center" valign="middle" >−6</th></tr></thead><tr><td align="center" valign="middle" >ξ 1</td><td align="center" valign="middle" >−0.033</td><td align="center" valign="middle" >−0.104</td><td align="center" valign="middle" >−0.098</td><td align="center" valign="middle" >−0.124</td><td align="center" valign="middle" >−0.1016</td><td align="center" valign="middle" >−0.0804</td><td align="center" valign="middle" >−0.1286</td></tr><tr><td align="center" valign="middle" >σ 1</td><td align="center" valign="middle" >0.439</td><td align="center" valign="middle" >0.528</td><td align="center" valign="middle" >0.557</td><td align="center" valign="middle" >0.627</td><td align="center" valign="middle" >0.647</td><td align="center" valign="middle" >0.663</td><td align="center" valign="middle" >0.718</td></tr><tr><td align="center" valign="middle" >μ 1</td><td align="center" valign="middle" >5.76</td><td align="center" valign="middle" >6.326</td><td align="center" valign="middle" >7.126</td><td align="center" valign="middle" >7.673</td><td align="center" valign="middle" >8.19</td><td align="center" valign="middle" >8.839</td><td align="center" valign="middle" >9.533</td></tr></tbody></table></table-wrap><p>The detector based on the cyclostationary characteristics of the signal acts in a quasi-blind context. It has no knowledge of the characteristics of the signal emitted by the PU. Therefore, we compare it to the classic detector based on the energy level. We notice that the probability of detection of the CFD is almost identical to that of the Energy-based Detection (ED). For a false alarm probability set at P f a = 0.05 , we obtained (<xref ref-type="fig" rid="fig5">Figure 5</xref>) P d C F D = 0.99 and P d E D = 0.97 in a channel where the SNR = −10 dB.</p><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Simulation parameters of CFD</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  colspan="3"  >64-QAM, 16-QAM, BPSK, 4-ASK Signal</th></tr></thead><tr><td align="center" valign="middle" >User</td><td align="center" valign="middle" >Parameters</td><td align="center" valign="middle" >Values</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >Primary</td><td align="center" valign="middle" >Sampling rate F e</td><td align="center" valign="middle" >128 kHz</td></tr><tr><td align="center" valign="middle" >Data rate</td><td align="center" valign="middle" >16 kHz</td></tr><tr><td align="center" valign="middle" >bandwidth W</td><td align="center" valign="middle" >21.6 kHz</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >Secondary</td><td align="center" valign="middle" >Observation duration Δ t</td><td align="center" valign="middle" >16 ms</td></tr><tr><td align="center" valign="middle" >Number of samples N</td><td align="center" valign="middle" >2048</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >Frequency resolution</td><td align="center" valign="middle" >Δ α</td><td align="center" valign="middle" >62.5 Hz</td></tr><tr><td align="center" valign="middle" >Δ ν</td><td align="center" valign="middle" >1 kHz</td></tr></tbody></table></table-wrap></sec><sec id="s7"><title>7. Conclusion</title><p>Detecting the Primary User (PU) signal, in a very weak SNR condition, is one of the most difficult tasks in cognitive radio. In this paper, we have proposed a non-cooperative detection model which is able to detect the signal of PU in low SNR scenario. This detection model exploits the cyclostationary features of communication signals. This cyclostationarity can be revealed through cyclic spectral analysis. Thus, after the estimation of the cyclic spectrum using the FFT Accumulation Method (FAM) algorithm, we generate the Cyclic Domain Profile (CDP). Then, we quantify this level of periodicity using the CDP crest factor. We use the CDP crest factor as the decision statistic to detect the state of the channel (busy or not). We approached the probability density function of the crest factor, which allowed us to analytically determine the optimal detection threshold, the probabilities of false alarm and detection. The simulations carried out subsequently show a strong similarity between the theoretical results and the experimental results. Cyclostationary Feature based Detection is an efficient detector. In low SNR scenario, it is able to detect a digital communication signal up to SNR = −11 dB. Our work on CFD shows that the CDP makes it possible to visualize the hidden frequencies of the observed signal on the one hand and on the other hand that the CF is a characteristic quantity of the modulation technique. We propose, in future works, to exploit these two tools (the CDP and the Crest Factor) to develop an algorithm, which is able to detect the signal of the PU and also to distinguish the signal of a PU from the signal of a SU, by using the principle of modulation recognition.</p></sec><sec id="s8"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s9"><title>Cite this paper</title><p>Kadjo, J.-M., Agoua, R., Bamba, A., Konat&#233;, A. and Asseu, O. (2021) Non-Cooperative Spectrum Sensing Based on Cyclostationary Model of Digital Signals in the Context of Cognitive Radio. Engineering, 13, 56-70. https://doi.org/10.4236/eng.2021.131005</p></sec><sec id="s10"><title>List of Abbreviations</title><p>CDP: Cyclic Domain Profile</p><p>CFD: Cyclostationary Features based Detection</p><p>COR: Caract&#233;ristique Op&#233;rationnelle du R&#233;cepteur</p><p>CS: Cyclostationnary</p><p>ED: Energy based-Detection</p><p>FAM: Fast fourier transform Accumulation Method</p><p>CF: Crest Factor</p><p>FFT: Fast Forier Transform</p><p>GEV: Generalized Extreme Value</p><p>MLE: Maximum Likewood Estimator</p><p>OBRE: Optimal Biased Robust Estimator</p><p>OFDM: Strip Spectral Correlation Algorithm</p><p>PU: Primary User</p><p>ROC: Receiver Operating Characteristic</p><p>SNR: Signal Noise Ratio</p><p>SU: Secondary User</p></sec></body><back><ref-list><title>References</title><ref id="scirp.106801-ref1"><label>1</label><mixed-citation publication-type="book" xlink:type="simple">Gardner, W. (1986) Introduction to Random Process with Applications to Signals and Systems. Gardner, W., Ed., North-Holland, Macmillan, New York.</mixed-citation></ref><ref id="scirp.106801-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Gardner, W.A. (1986) Statistical Spectral Analysis: A Nonprobabilistic Theory. Prentice-Hall, Inc.,Tokyo.</mixed-citation></ref><ref id="scirp.106801-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Gardner, W. (1991) Exploitation of Spectral Redundancy in Cyclostationary Signals. IEEE Signal Processing Magazine, 8, 14-36. https://doi.org/10.1109/79.81007</mixed-citation></ref><ref id="scirp.106801-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Prithiviraj, V., Sarankumar, B., Kalaiyarasan, A., Praveen, P. and Signh, N. (2011) Cyclostionary Analysis Method of Spectrum Sensing for Cognitive Radio. Wireless VITAE, IEEE, Chennai, India, 1-5.  
https://doi.org/10.1109/WIRELESSVITAE.2011.5940821</mixed-citation></ref><ref id="scirp.106801-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Gardner, W. (1994) Cyclostationarty in Communications and Signal Processing. IEEE Press, New York.</mixed-citation></ref><ref id="scirp.106801-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Tom, C. (1995) Investigation and implementation of computationally-efficient algorithm for cyclic spectral analysis. Master’s Thesis, Carleton University Ottawa, Ontario, Canada.</mixed-citation></ref><ref id="scirp.106801-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Jang, M. (2014) Blind Cyclostationary Spectrum Sensing in Cognitive Radios. IEEE Communications Letters, 8, 393-396.  
https://doi.org/10.1109/LCOMM.2014.012714.132507</mixed-citation></ref><ref id="scirp.106801-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Kotz, S. and Nadarajah, S. (2000) Extreme Value Distributions: Theory and Applications. World Scientific. https://doi.org/10.1142/p191</mixed-citation></ref><ref id="scirp.106801-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">De Haan, L. and Ferreira, A. (2007) Extreme Value Theory: An Introduction. Springer Science &amp; Business Media.</mixed-citation></ref><ref id="scirp.106801-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Dupuis, D. and Field, C. (1998) Robust Estimation of Extremes. Canadian Journal of Statistics, 26, 199-215. https://doi.org/10.2307/3315505</mixed-citation></ref><ref id="scirp.106801-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Kay, S.M. (1993) Fundamentals of Statistical Signal Processing. Prentice Hall PTR.</mixed-citation></ref><ref id="scirp.106801-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Tom, C. (1995) Cyclostationary Spectral Analysis of Typical Satcom Signals Using the FFT Accumulation Method. Defence Research Establishement Ottawa, Ontario, Canada, Technical Report 1280.</mixed-citation></ref><ref id="scirp.106801-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">(1993) A Review of Digital Spectral Correlation Analysis: Theory and Implementation. Article 6 in Part II of Cyclostationarity in Communications and Signal Processing, Gardner, W.A., Ed., IEEE Press, New York, 455-479.</mixed-citation></ref><ref id="scirp.106801-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Robert, R., Brown, W. and Loomis, H. (1991) Computationally Efficient Algorithms for Cyclic Spectral Analysis. Signal Processing Magazine, 8, 38-49.  
https://doi.org/10.1109/79.81008</mixed-citation></ref><ref id="scirp.106801-ref15"><label>15</label><mixed-citation publication-type="book" xlink:type="simple">Pace, P. (2009) Detecting and Classifying Low Probability of Intercept Radar. 2nd Edition, House, A., Ed., Artech House, Boston, London.</mixed-citation></ref><ref id="scirp.106801-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Brown, W. and Loomis, H. (1993) Digital Implementation of Spectral Correlation Analyzers. IEEE Transactions on Signal Processing, 41, 703-720.  
https://doi.org/10.1109/78.193211</mixed-citation></ref><ref id="scirp.106801-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Brown, W. (1987) On the Theory of Cyclostationary Signals. Ph.D. Dissertation, University of California, Davis, California, USA.</mixed-citation></ref><ref id="scirp.106801-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Kadjo, J.-M., Yao, K.C. and Mansour, A. (2016) Blind Detection of Cyclostationary Features in the Context of Cognitive Radio. IEEE International Symposium on Signal Processing and Information Technology (ISSPIT), Limassol, Cyprus, December 2016, 150-155. https://doi.org/10.1109/ISSPIT.2016.7886025</mixed-citation></ref><ref id="scirp.106801-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Napolitano, A. (2016) Cyclostationarity: New Trends and Applications. Signal Processing, 120, 385-408. https://doi.org/10.1016/j.sigpro.2015.09.011</mixed-citation></ref><ref id="scirp.106801-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Sutton, P.D., Nolan, K.E. and Doyles, L.E. (2008) Cyclostationary Signatures in Pratical Cognitive Radio Applications. IEEE Journal on Selected Areas in Communications, 26, 13-24. https://doi.org/10.1109/JSAC.2008.080103</mixed-citation></ref><ref id="scirp.106801-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Roussel, J. (2014) Modélisation cyclostationnaire et séparation de sources des signaux électromyographiques. Ph.D. dissertation, Université d’Orléans, France.</mixed-citation></ref><ref id="scirp.106801-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Weber, R. and Faye, C. (1998) Real Time Detector for Cyclostationary Rfi in Radio Astronomy. 9th European Signal Processing Conference (EUSIPCO 1998), Island of Rhodes, 8-11 September 1998, 1-4.</mixed-citation></ref><ref id="scirp.106801-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Randall, R.B., Antoni, J. and Chobsaard, S. (2001) The Relationship between Spectral Correlation and Envelope Analysis in the Diagnostics of Bearing Faults and Other Cyclostationary Machine Signals. Mechanical Systems and Signal Processing, 15, 945-962. https://doi.org/10.1006/mssp.2001.1415</mixed-citation></ref><ref id="scirp.106801-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Capdessus, C. (1992) Aide au diagnostic des machines tournantes par traitement du signal. Ph.D. Dissertation, Institut National Polytechnique de Grenoble, Grenoble.</mixed-citation></ref><ref id="scirp.106801-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">Rostaing, P. (1997) Détection de signaux modulés en exploitant leurs propriétés cyclostationnaires: Application aux signaux sonar. Ph.D. Dissertation, Université de Nice, Nice.</mixed-citation></ref><ref id="scirp.106801-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">Gardner, W. and Spooner, C. (1992) Signal Interception: Performance Advantages of Cyclic-Feature Detector. IEEE Transactions on Communications, 40, 149-159.  
https://doi.org/10.1109/26.126716</mixed-citation></ref><ref id="scirp.106801-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">Gardner, W. (1986) The Spectral Correlation Theory of Cyclostationary Time-Series. Signal Processing, Elsevier Science Publishers, 11, 13-36.  
https://doi.org/10.1016/0165-1684(86)90092-7</mixed-citation></ref><ref id="scirp.106801-ref28"><label>28</label><mixed-citation publication-type="other" xlink:type="simple">Dandawate, A.V. and Giannakis, G.B. (1995) Asymptotic Theory of Mixed Time Averages and kth-Order Cyclic-Moment and Cumulant Statistics. IEEE Transactions on Information Theory, 41, 216-232.  
https://doi.org/10.1109/18.370106</mixed-citation></ref><ref id="scirp.106801-ref29"><label>29</label><mixed-citation publication-type="other" xlink:type="simple">Dehay, D. and Hurd, H. (1994) Representation and Estimation for Periodically and Almost Periodically Correlated Random Processes. Cyclostationarity in Communications and Signal Processing, IEEE Press, New York, 295-328.</mixed-citation></ref><ref id="scirp.106801-ref30"><label>30</label><mixed-citation publication-type="other" xlink:type="simple">Gladyshev, E. (1963) Periodically and Almost-Periodically Correlated Random Processes with a Continuous Time Parameter. Theory of Probability Its Applications, 8, 173-177. https://doi.org/10.1137/1108016</mixed-citation></ref><ref id="scirp.106801-ref31"><label>31</label><mixed-citation publication-type="other" xlink:type="simple">Monin, A. (1963) Stationary and Periodic Time Series in the General Circulation of the Atmosphere. Proceedings of the Symposium on Time Series Analysis, Wiley, New York, 144-151.</mixed-citation></ref><ref id="scirp.106801-ref32"><label>32</label><mixed-citation publication-type="other" xlink:type="simple">(1961) Spectral Analysis of asymptotically Stationary Time Series. Stanford University Calif. Applied Mathematics and Statistics Lab, Tech. Rep.</mixed-citation></ref><ref id="scirp.106801-ref33"><label>33</label><mixed-citation publication-type="other" xlink:type="simple">Parzen, E. (1963) On Spectral Analysis with Missing Observations and Amplitude Modulation. Sankhyā: The Indian Journal of Statistics, Series A, 25, 383-392.</mixed-citation></ref><ref id="scirp.106801-ref34"><label>34</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>de Feriet</surname><given-names> J.K. </given-names></name>,<etal>et al</etal>. (<year>1962</year>)<article-title>Correlation and Spectrum of Asymptotically Stationary Random Functions</article-title><source> Mathematical Studies</source><volume> 30</volume>,<fpage> 55</fpage>-<lpage>67</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.106801-ref35"><label>35</label><mixed-citation publication-type="other" xlink:type="simple">Herbst, L.J. (1964) Spectral Analysis in the Presence of Variance Uctuations. Journal of the Royal Statistical Society: Series B (Methodological), 26, 354-360.  
https://doi.org/10.1111/j.2517-6161.1964.tb00568.x</mixed-citation></ref><ref id="scirp.106801-ref36"><label>36</label><mixed-citation publication-type="other" xlink:type="simple">Herbst, L. (1965) The Statistical Fourier Analysis of Variances. Journal of the Royal Statistical Society: Series B (Methodological), 27, 159-165.  
https://doi.org/10.1111/j.2517-6161.1965.tb00598.x</mixed-citation></ref><ref id="scirp.106801-ref37"><label>37</label><mixed-citation publication-type="other" xlink:type="simple">Herbst, L.J. (1963) Periodogram Analysis and Variance Uctuations. Journal of the Royal Statistical Society: Series B (Methodological), 25, 442-450.  
https://doi.org/10.1111/j.2517-6161.1963.tb00527.x</mixed-citation></ref><ref id="scirp.106801-ref38"><label>38</label><mixed-citation publication-type="other" xlink:type="simple">Herbst, L., et al. (1963) Almost Periodic Variances. The Annals of Mathematical Statistics, 34, 1549-1557. https://doi.org/10.1214/aoms/1177703887</mixed-citation></ref><ref id="scirp.106801-ref39"><label>39</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Gladyshev</surname><given-names> E. </given-names></name>,<etal>et al</etal>. (<year>1961</year>)<article-title>Periodically Correlated Random Sequence</article-title><source> Soviet Mathematics</source><volume> 2</volume>,<fpage> 385</fpage>-<lpage>388</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.106801-ref40"><label>40</label><mixed-citation publication-type="other" xlink:type="simple">Markelov, V. (1966) Axis Crossings and Relative Time of Existence of a Periodically Nonstationary Random Process. Soviet Radiophysics, 9, 440-443.  
https://doi.org/10.1007/BF01046009</mixed-citation></ref><ref id="scirp.106801-ref41"><label>41</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Gudzenko</surname><given-names> L. </given-names></name>,<etal>et al</etal>. (<year>1959</year>)<article-title>On Periodically Nonstationary Processes</article-title><source> Radiotekhnika i Electronika</source><volume> 4</volume>,<fpage> 1062</fpage>-<lpage>1064</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.106801-ref42"><label>42</label><mixed-citation publication-type="other" xlink:type="simple">Bennett, W.R. (1958) Statistics of Regenerative Digital Transmission. The Bell System Technical Journal, 37, 1501-1542.  
https://doi.org/10.1002/j.1538-7305.1958.tb01560.x</mixed-citation></ref></ref-list></back></article>