<?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">IJCNS</journal-id><journal-title-group><journal-title>International Journal of Communications, Network and System Sciences</journal-title></journal-title-group><issn pub-type="epub">1913-3715</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijcns.2017.108B029</article-id><article-id pub-id-type="publisher-id">IJCNS-78410</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>
 
 
  A Circulated Block Transmission Scheme for FTN Signaling
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mingqi</surname><given-names>Li</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>Shihao</surname><given-names>Lai</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>Yaqiu</surname><given-names>Peng</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Wireless Communication Research Center for New Media, Shanghai Advanced Research Institute, CAS, Shanghai, China</addr-line></aff><aff id="aff2"><addr-line>University of Chinese Academy of Sciences, Beijing, China</addr-line></aff><pub-date pub-type="epub"><day>14</day><month>08</month><year>2017</year></pub-date><volume>10</volume><issue>08</issue><fpage>269</fpage><lpage>279</lpage><history><date date-type="received"><day>July</day>	<month>4,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>August</month>	<year>11,</year>	</date><date date-type="accepted"><day>August</day>	<month>14,</month>	<year>2017</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>
 
 
  
    Fast-Than-Nyquist (FTN) transmission is a promising method to improve the spectrum efficiency for future wireless communication systems. However, this benefit of FTN is at the price of inducing the inter-symbol interference (ISI), which increases the complexity of the receiver. In this paper, a circulated block transmission scheme for FTN signaling, i.e. CB-FTN system is proposed. The detail implementation structure of CB-FTN transceiver is presented, in which the ISI caused by FTN transmission is canceled by the frequency-domain equalization (FDE), and the inter-block interference (IBI) caused by the multi-path channel is overcome by the cyclic-prefix. The postprocessing signal to noise ratio (pSNR) is analyzed for the CB-FTN receiver with zero-forcing FDE in AWGN channel, which is verified by the simulation results. Moreover, the BER performances and computational complexity of CB-FTN system are compared with the existed scheme. 
  
 
</p></abstract><kwd-group><kwd>FTN</kwd><kwd> ISI</kwd><kwd> Frequency-Domain Equalization</kwd><kwd> Post-Processing SNR</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>How to further improve the spectrum efficiency of transmission scheme is one of major issues for future wireless communication systems. Non-orthogonal transmission technologies have opened a door for the breakthrough in the above challenge. One of potential solutions is faster-than-Nyquist (FTN) signaling, which was first studied by Mazo in 1975. It was shown that by intentionally introducing inter-symbol inference (ISI), FTN signaling with sinc pulse can achieve 25% higher symbol rate than Nyquist signaling in additive white Gaussian noise (AWGN) channels [<xref ref-type="bibr" rid="scirp.78410-ref1">1</xref>]. The investigations in [<xref ref-type="bibr" rid="scirp.78410-ref2">2</xref>] show that the more practical root raised cosine (RRC) pulse, rather than the sinc shaping pulses, can also apply in FTN signaling. In [<xref ref-type="bibr" rid="scirp.78410-ref3">3</xref>] a discrete time form of FTN signaling is introduced, which enables same bite-error-rate (BER) performance as continuous FTN signaling with much lower cost computation.</p><p>Although the FTN signaling can improve the spectrum efficiency, the inevitable inter-symbol interference (ISI) has to be properly addressed to guarantee the error performance. Therefore, the major concern in FTN signaling is the detection algorithms [<xref ref-type="bibr" rid="scirp.78410-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.78410-ref5">5</xref>]. Since frequency domain equalization (FDE) is a computation-efficient method to mitigate the ISI, it is also widely applied to FTN systems [<xref ref-type="bibr" rid="scirp.78410-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.78410-ref7">7</xref>].</p><p>Except the equalizer designed for the FTN receiver, some efforts are also put into designing the FTN transmission schemes [<xref ref-type="bibr" rid="scirp.78410-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.78410-ref9">9</xref>]. In order to remove the effects of the ISI, a cyclic prefix (CP) based FTN block transmission scheme is addressed in [<xref ref-type="bibr" rid="scirp.78410-ref8">8</xref>], which will produce a loss of transmission efficiency. In [<xref ref-type="bibr" rid="scirp.78410-ref9">9</xref>], a CP and cyclic suffix (CS)-assisted symbol block transmission for FTN signaling is presented to overcome the above shortage. However, the redundant symbol- based CP/CS inserting and sample-based CP/CS discarding operations are needed before and after pulse-shaping filtering respectively, so as to avoid increasing transmission overhead to deal with the ISI. Nevertheless, such pro- cessing will bring about additional computational complexity at the transmitter.</p><p>In [<xref ref-type="bibr" rid="scirp.78410-ref10">10</xref>] and [<xref ref-type="bibr" rid="scirp.78410-ref11">11</xref>], a sample-based circular block transmission scheme is proposed for the filter-bank based wireless communication systems. Due to the specially designed circulated-sample-blocking operation performed after pulse- shaping filtering, the outputs of pulse-filtering are circular sample blocks. Therefore, the CP padding, utilized to cancel the inter-block interference (IBI) caused by multi-path channel, will not bring about the additional out-of-band leakage, which, otherwise, will be induced by the discontinuity between the CP and sample block.</p><p>In this paper, we proposed a circulated block transmission scheme for FTN signaling, i.e. CB-FTN system. By circulated sample blocking and CP padding, the CB-FTN system can achieve higher transmission rate than that of Nyquist system and meanwhile eliminate the IBI by FDE with the estimated channel frequency response. In addition, by exploiting the circulation property of the sample block, the ISI can be canceled by FDE with the circular self-correlation function of pulse-shaping filter as well.</p></sec><sec id="s2"><title>2. Sampling of FTN Signaling</title><p>The continuous-time FTN signaling can be expressed as</p><disp-formula id="scirp.78410-formula450"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x2.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x3.png" xlink:type="simple"/></inline-formula> is the input constellation symbols, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x4.png" xlink:type="simple"/></inline-formula>is the impulse response of T-orthogonal Nyquist pulse-shaping filter with unit energy. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x5.png" xlink:type="simple"/></inline-formula>is the time squeezing factor, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x6.png" xlink:type="simple"/></inline-formula>.</p><p>Assume <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x7.png" xlink:type="simple"/></inline-formula> is integer times of the sampling interval<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x8.png" xlink:type="simple"/></inline-formula>, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x9.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x10.png" xlink:type="simple"/></inline-formula>is a integer. Then, the sampled discrete-time FTN signaling can be obtained as</p><disp-formula id="scirp.78410-formula451"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x11.png"  xlink:type="simple"/></disp-formula><p>By properly system parameters designing, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x12.png" xlink:type="simple"/></inline-formula>can also be set to be integer times of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x13.png" xlink:type="simple"/></inline-formula>, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x14.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x15.png" xlink:type="simple"/></inline-formula> can be viewed as the up-sampling rate of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x16.png" xlink:type="simple"/></inline-formula>. Therefore, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x17.png" xlink:type="simple"/></inline-formula>is a N-orthogonal discrete Nyquist pulse-shaping filter, and satisfies the orthogonal condition</p><disp-formula id="scirp.78410-formula452"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x18.png"  xlink:type="simple"/></disp-formula><p>where L is the length of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x19.png" xlink:type="simple"/></inline-formula>. In fact, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x20.png" xlink:type="simple"/></inline-formula>, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x21.png" xlink:type="simple"/></inline-formula>, (1) and (2) become Nyquist transmission.</p></sec><sec id="s3"><title>3. CB-FTN System Model</title><sec id="s3_1"><title>3.1. Structure of CB-FTN Transmitter</title><p>The structure of the CBT-FTN transmitter is illustrated in <xref ref-type="fig" rid="fig1">Figure 1</xref>. We suppose that the input constellation symbol sequence is segmented, and, w.l.o.g., one of symbol segments, i.e. one data symbol block, can be expressed as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x22.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x23.png" xlink:type="simple"/></inline-formula>. Note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x24.png" xlink:type="simple"/></inline-formula> and D are the index and the number of symbols transmitted during each symbol block, respectively.</p><p>After the FTN filtering, the output signal could be expressed as</p><disp-formula id="scirp.78410-formula453"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x25.png"  xlink:type="simple"/></disp-formula><p>Then, by circulated blocking processing, the output signal could be given by</p><p><img data-original="http://html.scirp.org/file/78410x26.png" />,<img data-original="http://html.scirp.org/file/78410x27.png" /> (5)</p><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x28.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x29.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x30.png" xlink:type="simple"/></inline-formula>denotes the Modulo-Q operation.</p><p>Finally, the data block is padded with CP to form the circularly sample- blocked FTN signaling<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x31.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3_2"><title>3.2. Structure of CB-FTN Receiver</title><p>The structure of the CB-FTN receiver is illustrated as in <xref ref-type="fig" rid="fig2">Figure 2</xref>. Assume the</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Structure of CB-FTN transmitter</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78410x32.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Structure of CB-FTN receiver</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78410x33.png"/></fig><p>circularly blocked FTN signaling <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x34.png" xlink:type="simple"/></inline-formula> is passed through the wireless channel, which does not change during one sample block period, and perfect frequency and timing synchronization are achieved at the receiver.</p><p>After the CP removing from the received signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x35.png" xlink:type="simple"/></inline-formula>, the output is given as</p><disp-formula id="scirp.78410-formula454"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x36.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x37.png" xlink:type="simple"/></inline-formula> is the channel impulse response with power delay profile less than the CP length, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x38.png" xlink:type="simple"/></inline-formula>is the complex-valued AWGN with variance<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x39.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x40.png" xlink:type="simple"/></inline-formula> denotes the cyclic convolution.</p><p>Assume the perfect channel estimation is achieved and zero-forcing (ZF) equalization is applied, the output of channel equalization could be expressed as</p><disp-formula id="scirp.78410-formula455"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x41.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x42.png" xlink:type="simple"/></inline-formula> is the inverse system of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x43.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x44.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x45.png" xlink:type="simple"/></inline-formula>.</p><p>If ignoring the effects of AWGN, the output of circulated match-filtering becomes</p><disp-formula id="scirp.78410-formula456"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x46.png"  xlink:type="simple"/></disp-formula><p>Let</p><disp-formula id="scirp.78410-formula457"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x47.png"  xlink:type="simple"/></disp-formula><p>then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x48.png" xlink:type="simple"/></inline-formula>. Thus, we have</p><p><img data-original="http://html.scirp.org/file/78410x49.png" />,<img data-original="http://html.scirp.org/file/78410x50.png" /> (10)</p><p>Hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x51.png" xlink:type="simple"/></inline-formula>can be viewed as the equivalent impulse response of the ISI caused by FTN time squeezing. Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x52.png" xlink:type="simple"/></inline-formula> is known at receiver, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x53.png" xlink:type="simple"/></inline-formula>can be calculated beforehand. Thus by FDE, the transmitted signal could be estimated as</p><disp-formula id="scirp.78410-formula458"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x54.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x56.png" xlink:type="simple"/></inline-formula> are the vector expression of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x57.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x58.png" xlink:type="simple"/></inline-formula> respectively, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x59.png" xlink:type="simple"/></inline-formula>is the estimated value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x60.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x61.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x62.png" xlink:type="simple"/></inline-formula> are the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x63.png" xlink:type="simple"/></inline-formula> Fourier transform and inverse Fourier transform matrix, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x64.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x65.png" xlink:type="simple"/></inline-formula>is the equalization matrix.</p></sec></sec><sec id="s4"><title>4. Post-Processing SNR Analysis in AWGN Channel</title><p>The vector form of the transmitted CB-FTN signal without the CP can be described as</p><disp-formula id="scirp.78410-formula459"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x66.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x67.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x68.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x69.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x70.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x71.png" xlink:type="simple"/></inline-formula> denotes a vector obtained by cyclic down shifting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x72.png" xlink:type="simple"/></inline-formula> row of vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x73.png" xlink:type="simple"/></inline-formula>.</p><p>At the receiver, after CP removing and Q-tone channel FDE, the output signal can be given as</p><disp-formula id="scirp.78410-formula460"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x74.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x75.png" xlink:type="simple"/></inline-formula> is the AWGN vector. Since the channel frequency response matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x76.png" xlink:type="simple"/></inline-formula> for AWGN channel, the equalization matrix for channel FDE can be designed as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x77.png" xlink:type="simple"/></inline-formula>. As a result, the received signal can be reduced as</p><disp-formula id="scirp.78410-formula461"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x78.png"  xlink:type="simple"/></disp-formula><p>After circulated match-filtering, the output signal becomes</p><disp-formula id="scirp.78410-formula462"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x79.png"  xlink:type="simple"/></disp-formula><p>According to (9), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x80.png" xlink:type="simple"/></inline-formula>is a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x81.png" xlink:type="simple"/></inline-formula> circulated symmetric matrix, and</p><disp-formula id="scirp.78410-formula463"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x82.png"  xlink:type="simple"/></disp-formula><p>Therefore, the first term of (15) can be viewed as the output of vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x83.png" xlink:type="simple"/></inline-formula> circulated convoluting with vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x84.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x85.png" xlink:type="simple"/></inline-formula>.</p><p>If the FDE utilized to cancel the ISI, the detect metric vector of demodulated symbols can be expressed as</p><disp-formula id="scirp.78410-formula464"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x86.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x87.png" xlink:type="simple"/></inline-formula> is the diagonal FDE matrix.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x88.png" xlink:type="simple"/></inline-formula>, and</p><disp-formula id="scirp.78410-formula465"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x89.png"  xlink:type="simple"/></disp-formula><p>For ZF FDE, the ISI equalization matrix is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x90.png" xlink:type="simple"/></inline-formula>, then,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x91.png" xlink:type="simple"/></inline-formula>. As a result, the signal components, i.e. the first term in (17), can be given as</p><disp-formula id="scirp.78410-formula466"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x92.png"  xlink:type="simple"/></disp-formula><p>Assume <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x93.png" xlink:type="simple"/></inline-formula> is the i.i.d. (independent and identically distributed) complex constellation symbols with zero mean and unit energy, the average energy of the signal in (19) can be given by</p><disp-formula id="scirp.78410-formula467"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x94.png"  xlink:type="simple"/></disp-formula><p>The noise components, i.e. the second term in (17) can be written as</p><disp-formula id="scirp.78410-formula468"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x95.png"  xlink:type="simple"/></disp-formula><p>The covariance matrix of noise vector can be expressed as</p><disp-formula id="scirp.78410-formula469"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x96.png"  xlink:type="simple"/></disp-formula><p>Let</p><disp-formula id="scirp.78410-formula470"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x97.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.78410-formula471"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x98.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x99.png" xlink:type="simple"/></inline-formula> is a diagonal matrix, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x100.png" xlink:type="simple"/></inline-formula> is a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x101.png" xlink:type="simple"/></inline-formula> circulated symmetric matrix. Hence, the covariance matrix of noise becomes as</p><disp-formula id="scirp.78410-formula472"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x102.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.78410-formula473"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x103.png"  xlink:type="simple"/></disp-formula><p>Therefore, we have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x104.png" xlink:type="simple"/></inline-formula>, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x105.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x106.png" xlink:type="simple"/></inline-formula>.</p><p>Then by (26), the variance of the noise can be given by</p><disp-formula id="scirp.78410-formula474"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x107.png"  xlink:type="simple"/></disp-formula><p>As a result, by (20) and (25), the post-processing SNR can be described as</p><disp-formula id="scirp.78410-formula475"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x108.png"  xlink:type="simple"/></disp-formula><p>In fact, for Nyquist transmission, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x109.png" xlink:type="simple"/></inline-formula>in (9) equals to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x110.png" xlink:type="simple"/></inline-formula>. According to the N-orthogonal property of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x111.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x112.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x113.png" xlink:type="simple"/></inline-formula>, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x114.png" xlink:type="simple"/></inline-formula>. There- fore, by (18),<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x115.png" xlink:type="simple"/></inline-formula>. Then the post-processing SNR is reduced as</p><disp-formula id="scirp.78410-formula476"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78410x116.png"  xlink:type="simple"/></disp-formula></sec><sec id="s5"><title>5. Performance Evaluation of CB-FTN</title><p>The performances of the proposed scheme are evaluated in this section. The system parameters for simulations are presented in <xref ref-type="table" rid="table1">Table 1</xref>.</p><sec id="s5_1"><title>5.1. The Effects of the ISI Caused by FTN Time Squeezing</title><p>In order to achieve higher spectrum efficiency, the CB-FTN system stuffs more data symbols in one data block than Nyquist system, which will cause the ISI within one block inevitably. Due to the cyclic property of CB-FTN signaling, according to (9), the equivalent impulse response of the ISI caused by FTN time</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> System parameters</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Parameters</th><th align="center" valign="middle"  colspan="2"  >Simulation Systems</th></tr></thead><tr><td align="center" valign="middle" >Nyquist rate transmission</td><td align="center" valign="middle" >FTN rate transmission</td></tr><tr><td align="center" valign="middle" >Modulation scheme</td><td align="center" valign="middle"  colspan="2"  >QPSK</td></tr><tr><td align="center" valign="middle" >Type of pulse-shaping filter</td><td align="center" valign="middle"  colspan="2"  >RRC</td></tr><tr><td align="center" valign="middle" >Roll-off factor</td><td align="center" valign="middle"  colspan="2"  >0.3</td></tr><tr><td align="center" valign="middle" >Length of filter (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x117.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle"  colspan="2"  >241</td></tr><tr><td align="center" valign="middle" >Up-sampling rate (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x118.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle"  colspan="2"  >20</td></tr><tr><td align="center" valign="middle" ># of shift samples of shaping filtering (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x119.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >16, 18</td></tr><tr><td align="center" valign="middle" ># of symbols carried by one circulated block (D)</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" >Length of circulated block (Q)</td><td align="center" valign="middle" >320</td><td align="center" valign="middle" >320, 360</td></tr><tr><td align="center" valign="middle" >Time squeezing ratio (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x120.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.8, 0.9</td></tr><tr><td align="center" valign="middle" >Spectrum efficiency (bps/Hz)</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2.5, 2.22</td></tr></tbody></table></table-wrap><p>squeezing is symmetric, as shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>(a). We also notice that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x121.png" xlink:type="simple"/></inline-formula> trends to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x122.png" xlink:type="simple"/></inline-formula>, when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x123.png" xlink:type="simple"/></inline-formula> increases to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x124.png" xlink:type="simple"/></inline-formula>, i.e. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x125.png" xlink:type="simple"/></inline-formula>to 1. As shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>(b), frequency selectivity of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x126.png" xlink:type="simple"/></inline-formula> becomes severe with the decrease of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x127.png" xlink:type="simple"/></inline-formula>, i.e. the high frequency components of transmitted signal is suppressed.</p></sec><sec id="s5_2"><title>5.2. Post-Processing SNR with ZF-FDE for ISI Cancelation</title><p><xref ref-type="fig" rid="fig4">Figure 4</xref> presents the both theoretical and simulated post-processing SNR of the CB-FTN receiver with zero-forcing FDE for ISI cancelation in AWGN channel. As shown in the <xref ref-type="fig" rid="fig4">Figure 4</xref>(a), the post-processing SNR is increased with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x128.png" xlink:type="simple"/></inline-formula>. Due to the severe frequency selectivity, the post-processing SNR is much lower than the received SNR when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x129.png" xlink:type="simple"/></inline-formula>, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x130.png" xlink:type="simple"/></inline-formula>. Meanwhile, for Nyquist rate transmission, i.e. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x131.png" xlink:type="simple"/></inline-formula>or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x132.png" xlink:type="simple"/></inline-formula>, the post-processing SNR is equal to the received SNR. Furthermore, within the received SNR range, the theoretical results are well matched with the simulation results.</p><p>In order to implement FDE with fast Fourier transform, the length of circulated block <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula> should be chosen as a power of two. For example, if set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x134.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x135.png" xlink:type="simple"/></inline-formula>, we can get<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x136.png" xlink:type="simple"/></inline-formula>. When the up-sampling rate of pulse-shaping is set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x137.png" xlink:type="simple"/></inline-formula>, it can be obtained that the time squeezing ratio<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x138.png" xlink:type="simple"/></inline-formula>. <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) compares the post-processing SNRs of the CB-FTN system with different sample block length. As shown in the figure, with the same time squeezing ratio<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x139.png" xlink:type="simple"/></inline-formula>, the systems with different <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x140.png" xlink:type="simple"/></inline-formula> achieve the similar performances. With the increasing of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x141.png" xlink:type="simple"/></inline-formula>, the post-processing SNR is increased slightly, because the frequency selectivity of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x142.png" xlink:type="simple"/></inline-formula> is reduced a little with the increase of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x143.png" xlink:type="simple"/></inline-formula>.</p><p>The BER performances of CB-FTN system with turbo coding and ZF-FDE are illustrated in <xref ref-type="fig" rid="fig5">Figure 5</xref>. By comparing with <xref ref-type="fig" rid="fig4">Figure 4</xref>(a), it can be noticed that the effects of time squeezing ratio on the BER performance are similar to that on post-processing SNR. Moreover, BER performances of CB-FTN system are almost the same as that of the scheme proposed in [<xref ref-type="bibr" rid="scirp.78410-ref9">9</xref>], that is because the principle</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Time-/frequency domain property of c(d).</title></caption><fig id ="fig3_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78410x144.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78410x145.png"/></fig></fig-group><p>of transmitters of both schemes are similar, but with different implementation structure.</p><p>As mentioned in above section, the scheme in [<xref ref-type="bibr" rid="scirp.78410-ref9">9</xref>] needs symbol-based CP/CS inserting and sample-based CP/CS removing operations before and after pulse- shaping filtering respectively, which will increase the computational complexity of transmitter. For example, if set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x146.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x147.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x148.png" xlink:type="simple"/></inline-formula>, i.e. Q =</p><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Post-processing SNR with ZF-FDE. (a) With different<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x151.png" xlink:type="simple"/></inline-formula>. (b) With different<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x152.png" xlink:type="simple"/></inline-formula>.</title></caption><fig id ="fig4_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78410x149.png"/></fig><fig id ="fig4_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78410x150.png"/></fig></fig-group><p>512, the length of symbol-based CP/CS should be<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78410x153.png" xlink:type="simple"/></inline-formula>, so as to form the circulated sample block. Consequently, an additional 50% of computational complexity is needed, since the CP/CS with total length 16, which will be discarded before final transmission, should be passed through the pulse- shaping filter for transmission of 32 data symbols. However, the above redundant</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> BER performance in AWGN channel</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78410x154.png"/></fig><p>operations are unnecessary for the CB-FTN transmitter utilizing circulated blocking operation to form the circulated sample block, which is equivalent to only 32 data symbols passed through the pulse-shaping filter.</p></sec></sec><sec id="s6"><title>6. Conclusion</title><p>In this paper, a circulated block transmission scheme is proposed for FTN signaling, i.e. CB-FTN system. By circulated sample blocking and CP padding, the FDE can be utilized to cancel the IBI induced by wireless multipath channel. Moreover, by exploiting the circulation property of the sample block, the ISI caused by FTN filtering, can be eliminated by FDE with the circular self-corre- lation function of pulse-shaping filter as well. The equivalent impulse response and effects of the ISI are illustrated and analyzed by simulation. The theoretical post-processing SNR are analyzed for the CB-FTN receiver with ZF FDE in AWGN channel, which is verified by the simulation results. Moreover, the BER performances of the CB-FTN system are illustrated and compared with the existed scheme. It can be found that both schemes have very close BER performances, but the former has much lower computational complexity of transmitter than the latter.</p></sec><sec id="s7"><title>Acknowledgements</title><p>This work is supported by the International cooperation project of National Natural Science Foundation of China (No. 6146136001), and the capability improvement project of Zhangjiang Administrative Committee of Shanghai Municipality (No. 2016-14).</p></sec><sec id="s8"><title>Cite this paper</title><p>Li, M.Q., Lai, S.H. and Peng, Y.Q. (2017) A Circulated Block Transmission Scheme for FTN Signaling. Int. J. Communications, Network and System Sciences, 10, 269-279. https://doi.org/10.4236/ijcns.2017.108B029</p></sec></body><back><ref-list><title>References</title><ref id="scirp.78410-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Mazo, J. (1975) Faster-than-Nyquist Signaling. 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