<?xml version="1.0" encoding="ISO-8859-1"?><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance">
<front>
<journal-meta>
<journal-id>0120-6230</journal-id>
<journal-title><![CDATA[Revista Facultad de Ingeniería Universidad de Antioquia]]></journal-title>
<abbrev-journal-title><![CDATA[Rev.fac.ing.univ. Antioquia]]></abbrev-journal-title>
<issn>0120-6230</issn>
<publisher>
<publisher-name><![CDATA[Facultad de Ingeniería, Universidad de Antioquia]]></publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id>S0120-62302016000100013</article-id>
<article-id pub-id-type="doi">10.17533/udea.redin.n78a13</article-id>
<title-group>
<article-title xml:lang="en"><![CDATA[Spectral-amplitude encoding CDMA system based on high-speed electronic encoder/decoder structures]]></article-title>
<article-title xml:lang="es"><![CDATA[Sistema de codificación CDMA de amplitud de sub-bandas basado en estructuras de codificación/decodificación electrónica de alta velocidad]]></article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Aguilar-Torrentera]]></surname>
<given-names><![CDATA[Jorge]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
<xref ref-type="aff" rid="A02"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Rodríguez-Cruz]]></surname>
<given-names><![CDATA[Jesús Ramón]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Puente-Ramírez]]></surname>
<given-names><![CDATA[Norma Patricia]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
<contrib contrib-type="author">
<name>
<surname><![CDATA[Rodríguez-Morales]]></surname>
<given-names><![CDATA[Gustavo]]></given-names>
</name>
<xref ref-type="aff" rid="A01"/>
</contrib>
</contrib-group>
<aff id="A01">
<institution><![CDATA[,Universidad Autónoma de Nuevo León Facultad de Ingeniería Mecánica y Eléctrica ]]></institution>
<addr-line><![CDATA[Nuevo León ]]></addr-line>
<country>México</country>
</aff>
<aff id="A02">
<institution><![CDATA[,Universidad Autónoma de Nuevo León Facultad de Ingeniería Mecánica y Eléctrica ]]></institution>
<addr-line><![CDATA[ ]]></addr-line>
</aff>
<pub-date pub-type="pub">
<day>00</day>
<month>03</month>
<year>2016</year>
</pub-date>
<pub-date pub-type="epub">
<day>00</day>
<month>03</month>
<year>2016</year>
</pub-date>
<numero>78</numero>
<fpage>99</fpage>
<lpage>104</lpage>
<copyright-statement/>
<copyright-year/>
<self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_arttext&amp;pid=S0120-62302016000100013&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_abstract&amp;pid=S0120-62302016000100013&amp;lng=en&amp;nrm=iso"></self-uri><self-uri xlink:href="http://www.scielo.org.co/scielo.php?script=sci_pdf&amp;pid=S0120-62302016000100013&amp;lng=en&amp;nrm=iso"></self-uri><abstract abstract-type="short" xml:lang="en"><p><![CDATA[A new method for high-speed Code Division Multiple Access (CDMA) systems that lies on the analogue performance of distributed-based transversal filters is proposed. The method allows spectral-amplitude encoding CDMA system implementations leading to an improvement of orthogonality among users over temporal encoding direct-sequence systems. The maximal degrees of flexibility in the design of transversal filters are considered to generate waveforms that exhibit large temporal variation over the filter span time in accordance with an encoded waveform. Applications of our method to high-speed CDMA are discussed towards the end of the paper.]]></p></abstract>
<abstract abstract-type="short" xml:lang="es"><p><![CDATA[En este artículo se propone un método nuevo para sistemas de multi-canalización por división de código (CDMA, por sus siglas en inglés) para sistemas de alta velocidad, el cual radica en el desempeño analógico de filtros transversales distribuidos. El método permite el diseño de sistemas de codificación de amplitud de sub-bandas CDMA, el cual presenta un mejor desempeño en comparación con aquel que se obtiene al utilizar codificación temporal de secuencia directa. Se considera la máxima flexibilidad en el diseño de filtros transversales para obtener una variación temporal amplia de las formas de onda que se propagan lo largo de la línea de retardo del filtro transversal de acuerdo a una señal codificada espectralmente. Aplicaciones del método a las redes CDMA de alta velocidad se discuten al final del artículo.]]></p></abstract>
<kwd-group>
<kwd lng="en"><![CDATA[Optical fiber CDMA]]></kwd>
<kwd lng="en"><![CDATA[spectral encoding]]></kwd>
<kwd lng="en"><![CDATA[multi-Gbps networks]]></kwd>
<kwd lng="en"><![CDATA[transversal filter]]></kwd>
<kwd lng="en"><![CDATA[distributed amplifier]]></kwd>
<kwd lng="en"><![CDATA[user orthogonality]]></kwd>
<kwd lng="es"><![CDATA[CDMA de fibra óptica]]></kwd>
<kwd lng="es"><![CDATA[codificación espectral]]></kwd>
<kwd lng="es"><![CDATA[Redes a velocidades de multi-Gbit/s]]></kwd>
<kwd lng="es"><![CDATA[filtro transversal]]></kwd>
<kwd lng="es"><![CDATA[amplificador distribuido]]></kwd>
<kwd lng="es"><![CDATA[ortogonalidad]]></kwd>
</kwd-group>
</article-meta>
</front><body><![CDATA[  <font face="Verdana" size="2"></font>     <p align="right"><font size="2" face="Verdana">DOI:  <a href="http://dx.doi.org/10.17533/udea.redin.n78a13">10.17533/udea.redin.n78a13</a></font></p>     <p align="right">&nbsp;</p>     <p align="right"><font size="2" face="Verdana"><b>ART&Iacute;CULO ORIGINAL</b></font></p>     <p>&nbsp;</p>     <p align="center"><font size="4" face="Verdana"><b>Spectral-amplitude encoding CDMA system based on high-speed electronic encoder/decoder structures</b></font></p>     <p>&nbsp;</p>     <p align="center"><font size="3" face="Verdana"><b>Sistema de codificaci&oacute;n CDMA de amplitud de sub-bandas basado en estructuras de codificaci&oacute;n/decodificaci&oacute;n electr&oacute;nica de alta velocidad</b></font></p>     <p align="center">&nbsp;</p>     <p align="center">&nbsp;</p>     ]]></body>
<body><![CDATA[<p><font size="2" face="Verdana"><b><i>Jorge Aguilar-Torrentera*, Jes&uacute;s Ram&oacute;n Rodr&iacute;guez-Cruz, Norma Patricia Puente-Ram&iacute;rez, Gustavo Rodr&iacute;guez-Morales </i></b></font></p>     <p><font size="2" face="Verdana">Universidad Aut&oacute;noma de Nuevo Le&oacute;n, Facultad de Ingenier&iacute;a Mec&aacute;nica y El&eacute;ctrica. Av. Universidad s/n, Ciudad Universitaria, San Nicol&aacute;s de los Garza. C. P. 66455. Nuevo Le&oacute;n, M&eacute;xico.</font></p>     <p><font size="2" face="Verdana">* Corresponding author: Jorge Aguilar Torrentera, e&#8211;mail: <a href="mailto:: jorge.aguilart@uanl.mx">jorge.aguilart@uanl.mx</a> </font></p>     <p>&nbsp;</p>     <p><font size="2" face="Verdana">ISSN&nbsp; 0120&#8211;6230</font></p>     <p><font size="2" face="Verdana">e&#8211;ISSN 2422&#8211;2844</font></p>     <p>&nbsp;</p>     <p align="center"><font size="2" face="Verdana">(Received March 02, 2015</font>; <font size="2" face="Verdana">accepted  October 01, 2015</font>)</p>     <p>&nbsp;</p>     <p>&nbsp;</p> <hr noshade size="1">     ]]></body>
<body><![CDATA[<p><b><font size="3" face="Verdana">ABSTRACT</font></b></p>     <p><font size="2" face="Verdana">A new method for high-speed Code Division Multiple Access (CDMA) systems that lies on the analogue performance of distributed-based transversal filters is proposed. The method allows spectral-amplitude encoding CDMA system implementations leading to an improvement of orthogonality among users over temporal encoding direct-sequence systems. The maximal degrees of flexibility in the design of transversal filters are considered to generate waveforms that exhibit large temporal variation over the filter span time in accordance with an encoded waveform. Applications of our method to high-speed CDMA are discussed towards the end of the paper.</font></p>       <p><font size="2" face="Verdana"><i>Keywords:</i> Optical fiber CDMA, spectral encoding, multi-Gbps networks, transversal filter, distributed amplifier, user orthogonality</font></p> <hr noshade size="1">     <p><b><font size="3" face="Verdana">RESUMEN</font></b></p>     <p><font size="2" face="Verdana">En este art&iacute;culo se propone un m&eacute;todo nuevo para sistemas de multi-canalizaci&oacute;n por divisi&oacute;n de c&oacute;digo (CDMA, por sus siglas en ingl&eacute;s) para sistemas de alta velocidad, el cual radica en el desempe&ntilde;o anal&oacute;gico de filtros transversales distribuidos. El m&eacute;todo permite el dise&ntilde;o de sistemas de codificaci&oacute;n de amplitud de sub-bandas CDMA, el cual presenta un mejor desempe&ntilde;o en comparaci&oacute;n con aquel que se obtiene al utilizar codificaci&oacute;n temporal de secuencia directa. Se considera la m&aacute;xima flexibilidad en el dise&ntilde;o de filtros transversales para obtener una variaci&oacute;n temporal amplia de las formas de onda que se propagan lo largo de la l&iacute;nea de retardo del filtro transversal de acuerdo a una se&ntilde;al codificada espectralmente. Aplicaciones del m&eacute;todo a las redes CDMA de alta velocidad se discuten al final del art&iacute;culo.</font></p>       <p><font size="2" face="Verdana"><i>Palabras clave:</i> CDMA de fibra &oacute;ptica, codificaci&oacute;n espectral, Redes a velocidades de multi-Gbit/s, filtro transversal, amplificador distribuido, ortogonalidad</font></p> <hr noshade size="1">     <p><b><font size="3" face="verdana">1.  Introduction</font></b></p> <font size="2" face="verdana">     <p>For the past years, there   have been major advances in the enabling technology for deploying all-optical   networks in which the associated transport and processing functions remain   entirely in the optical domain. In the field of Optical Code Division Multiple   Access (OCDMA), multi-Gbps networks encompass different functions mainly   relying on optical devices to encode and decode user data. Coherent and   non-coherent encoding schemes have been proposed by making use of the methods   of modulation and detection used in fiber optic communication systems. However   the development of OCDMA networks at a wide scale is yet incomplete mainly   owing to the high-cost incurred in their deployment &#91;1&#93;. In fairly recent   developments, the electronic processing of codes employing distributed-based   transversal filters (DTF's) &#91;2, 3&#93; has been   considered as a technique to employ in multi-Gbps asynchronous networks.   Besides the low-cost incurred in its deployment, the electronic technique   avoids optical losses featured in optical matched filters and it relies on   optical devices solely for transport functions and signal distribution. </p>     <p>Hitherto, the DTF has been   used to generate and correlate high-rate binary sequences in direct sequence   (DS)-CDMA systems. Early work on the filter method confirmed the practicality   of symbol-rate DTF design by achieving zero inter-symbol interference (ISI) in   the reception of high-rate sequences &#91;4&#93;. In other proposal, time-domain   encoding of unipolar pulses was considered in &#91;3&#93; as a method by which code is   impressed on variable delays between consecutive pulses. Nonetheless, the span   time of the filter taped delay line is highly constrained by filter design considerations.   Therefore the distance between consecutive pulses becomes low preventing from   keeping low cross-correlation parameters in the reception of CDMA signals as   more users are added in the network. </p>     <p>The first practical   demonstration of multi-Gchips/s electronic CDMA system for optical access   networks was reported in &#91;2&#93;. Fractionally-spaced transversal filters featuring   a tap gain tuning capability were used to generate encoding patterns with   compensated inter-pulse interference. User data is decoded by obtaining a   correlation pulse in the intended node receiver and comparing its amplitude   against a threshold level. Threshold electronics can work at speeds compatible   with the synchronous operation of the transversal filter (at multi-Gchip/s).   Nonetheless, the large side-lobe cross-correlation output that results from   using quasi-orthogonal codes prevents from increasing the number of   simultaneous users in the network without deteriorating performance. More   recently, an electro-optic encoder/decoder structure in which each   electronically encoded chip modulates a slot or frequency bin to form a   spectrally encoded CDMA signal was proposed &#91;5&#93;. Nonetheless, the structure   requires intensity modulators and a large number of optical devices which makes   the electro-optic approach costly for a network developed at a wide scale. </p>     ]]></body>
<body><![CDATA[<p>From the above, it is   apparent that a straightforward adaptation of the previously proposed encoding   methods to the electronic processing of codes via the DTF method leads to   significant limitations in the development of CDMA networks. In this paper, new   filter structures for use in spectral-amplitude encoding CDMA systems are   introduced. Our proposal is motivated by early work on OCDMA based on spectral   encoding of non-coherent sources &#91;6&#93; in which multiple-user interference is   cancelled out by balanced detection of spectrally encoded pulses. It is found   that the transient characteristics of DTF's are appropriate to synthesize   spectrally-encoded waveforms based on the Spread Time (ST) technique &#91;7&#93;. It is   well-known that in order to keep orthogonality among users, encoder and decoder   functions have to extend beyond the symbol interval. Such a pulse spread is   aimed to ensure minimal overlap between neighboring frequency slots of the   assigned waveforms. Although the filter approach based on distributed amplifier   principles can produce a variety of high-rate pulse filtering functions &#91;8&#93; the   synthesis of spread-in-time signals by DTF's requiring more than 7 or 8 taps is   prohibitive due to filter losses and size constrains. </p>     <p>In the proposed method,   pulse responses are mostly spread over the filter span time, T, by taking   advantage of the low degradation of the rise time parameter of distributed   filter stages. To approximate CDMA functions, waveforms are truncated with a   square pulse of width equal to the filter time span. As a consequence, the   ensuing spectrum consists of a number of sub-bands bearing both code   information and interference; the latter is introduced in the form of sub-band   side-lobes spread over the available bandwidth. The encoder/decoder structures   herein proposed can reduce sub-band interference by a careful selection of   filter functions. Our method is appraised by showing that encoder and decoder   functions with spectral content depending on orthogonal codes result in   suitable matched filtering and multi-user interference rejection capabilities.</p> </font>     <p><b><font size="3" face="verdana">2.  CDMA method</font></b></p> <font size="2" face="verdana">     <p>A scheme of the proposed   CDMA system based on filter structures is illustrated in Figure 1. Each filter   function is synthesized by a finite-impulse response (FIR) that requires   processing short pulses comprising variable delay between consecutive pulses   and multilevel pulse weighting. For such aim, the DTF as a signal processor   that presents the maximal degree of freedom in the design &#91;8&#93; is adopted. The filter function is given by Eq. (1). </p>     <p><img src="img/revistas/rfiua/n78/n78a13e01.gif"></p>     <p>where  <img src="img/revistas/rfiua/n78/n78a13ea01.gif">  , M is the number of sub-bands, <img src="img/revistas/rfiua/n78/n78a13ea02.gif"> is a time window   function, <img src="img/revistas/rfiua/n78/n78a13ea03.gif">; <img src="img/revistas/rfiua/n78/n78a13ea04.gif">, and <img src="img/revistas/rfiua/n78/n78a13ea05.gif"> elsewhere. For brevity, <img src="img/revistas/rfiua/n78/n78a13ea06.gif"> and <img src="img/revistas/rfiua/n78/n78a13ea07.gif"> are referred to as the   phase and the amplitude of the nth-subband, respectively. The sub-bands are   separated by 1/T &#91;Hz&#93; away from side-lobe centers and each sub-band amplitude   and phase are modulated to encode and decode data.</p>     <p>The scheme of the proposed   CDMA system in <a href="#Figura1">Figure 1</a> is described as follows. Each information bit is   encoded by a waveform that conveys code information in sub-band amplitudes <img src="img/revistas/rfiua/n78/n78a13ea08.gif">. At the decoder, input power is split to correlate with two   functions. Briefly speaking, the correlation output of each filter consists of   a number of sub-bands modulated by the amplitudes and phases of the   corresponding filter function. At the upper branch, the correlator function   provides address information in the phase vector <img src="img/revistas/rfiua/n78/n78a13ea09.gif">. The lower-branch function, which is made available to all   decoders, shifts the phases of input sub-bands by the vector <img src="img/revistas/rfiua/n78/n78a13ea10.gif">. In the lower-branch   function all sub-band amplitudes are set to one and the output produces a   reference with which the user correlated spectrum is mixed to produce a new   sub-band with spectral content within the lowpass filter bandwidth. The   bandwidth requirements are equal to the bit-rate. </p>     <p align="center"><a name="Figura1"></a><img src="img/revistas/rfiua/n78/n78a13i01.gif"></p>      <p>A receiver with address <img src="img/revistas/rfiua/n78/n78a13ea11.gif"> will produce the   output as the summation given by Eq. (2). </p>     <p><img src="img/revistas/rfiua/n78/n78a13e02.gif"></p>     ]]></body>
<body><![CDATA[<p>Since the amplitude of each   user sub-band is square raised and user phases are cancelled out in the   demodulation process the receiver can retain only user power. As a consequence   encoding functions are constrained to be positive. Code constructions initially   proposed for spectral-amplitude encoding OCDMA systems &#91;6&#93; are herein   considered to achieve perfect orthogonality among users. When testing with   binary codes, the receiver address function have sub-band amplitudes set to one and the phase differences <img src="img/revistas/rfiua/n78/n78a13ea12.gif"> are chosen from <img src="img/revistas/rfiua/n78/n78a13ea13.gif"> for <img src="img/revistas/rfiua/n78/n78a13ea14.gif">.</font>     <p><b><font size="3" face="verdana">3. Filter design method</font></b></p> <font size="2" face="verdana">     <p>A design method for FIR-based encoder and decoder   filters is introduced. Consider a user encoded with <img src="img/revistas/rfiua/n78/n78a13ea08.gif">, sub-band phases set to the vector <img src="img/revistas/rfiua/n78/n78a13ea15.gif"> and a decoder function   depending on the phase vector <img src="img/revistas/rfiua/n78/n78a13ea16.gif"> . Eq. (3) is the receiver correlation function that comprises   the most significant terms and given by: </p>     <p><img src="img/revistas/rfiua/n78/n78a13e03.gif"></p>     <p>where <img src="img/revistas/rfiua/n78/n78a13ea17.gif"> , ' <img src="img/revistas/rfiua/n78/n78a13ea18.gif"> ' denotes convolution and <img src="img/revistas/rfiua/n78/n78a13ea19.gif"> is equal to <img src="img/revistas/rfiua/n78/n78a13ea20.gif"> . The correlation output of the lower branch, <img src="img/revistas/rfiua/n78/n78a13ea21.gif"> , and its derived function <img src="img/revistas/rfiua/n78/n78a13ea22.gif"> have similar equations   just need to substitute <img src="img/revistas/rfiua/n78/n78a13ea19.gif"> by <img src="img/revistas/rfiua/n78/n78a13ea23.gif">  <img src="img/revistas/rfiua/n78/n78a13ea24.gif"> into Eq. (3). The   first term is the correlation contribution between frequency-aligned sub-band   main-lobes of encoder/decoder functions. In the second term, <img src="img/revistas/rfiua/n78/n78a13ea25.gif"> accounts for the   correlation contribution between encoder/decoder functions with sub-band   side-lobes extending over frequencies that overlap with main-lobe portions thus   representing sub-band interference. Chief among interference products, <img src="img/revistas/rfiua/n78/n78a13ea26.gif"> result in the larger   interference; according to Eq. (3). </p>     <p>A filter design method is introduced to reduce the   effect of frequency overlap so that much of the pulse energy at the output is   due to the demodulation process of frequency aligned sub-band main-lobes. The   mixing between both filter correlation outputs not only involves   frequency-aligned correlated sub-bands but also the cross-term products <img src="img/revistas/rfiua/n78/n78a13ea27.gif"> and <img src="img/revistas/rfiua/n78/n78a13ea28.gif"> . At first sight, for sinusoids of main-lobes and interfering   side-lobe products of same frequency, unwanted sub-bands will fall into the   lowpass filter bandwidth creating potential interference. A straightforward   examination however shows that interference created by some cross products can   be filtered out of the receiver output by a proper choice of phases. In order   to create a number of orthogonal channels, all encoders and decoders are fixed   to the phase vector <img src="img/revistas/rfiua/n78/n78a13ea29.gif">to generate a   reference at the decoders to mix with the (address) correlator output. By this   means, each decoder can be set with a unique phase address. Now, to reduce sub-band   interference, a choice of phases <img src="img/revistas/rfiua/n78/n78a13ea30.gif"> and <img src="img/revistas/rfiua/n78/n78a13ea31.gif"> from <img src="img/revistas/rfiua/n78/n78a13ea32.gif"> for <img src="img/revistas/rfiua/n78/n78a13ea33.gif"> makes the interfering   cross-products odd functions about T, resulting in a smaller interfering signal   at the receiver output. The above phase selections lead to fix <img src="img/revistas/rfiua/n78/n78a13ea34.gif"> to the alternate   sequence vector <img src="img/revistas/rfiua/n78/n78a13ea35.gif">. </p> </font>     <p><b><font size="3" face="verdana">4.  Results</font></b></p> <font size="2" face="verdana">     <p>In order to test the CDMA   method unipolar and bipolar versions of Hadamard codes of length 4 are used.   <a href="#Tabla1">Table 1</a> shows mutually orthogonal codes and also itemizes the corresponding   sub-band phases referred to the alternate vector <img src="img/revistas/rfiua/n78/n78a13ea36.gif"> to achieve zero   cross-correlation, according with Eq. (2). The codework containing all 1's   cannot be considered since a user depending on this code has different power   from the rest, which have the same number of 1's and 0's. </p>     <p align="center"><a name="Tabla1"></a><img src="img/revistas/rfiua/n78/n78a13t01.gif"></p> </font>    <p><font size="2" face="verdana">According with the filter   method, waveform design needs a selection of phases uniformly spaced on the   unit circle such as <img src="img/revistas/rfiua/n78/n78a13ea37.gif"> , 0 and <img src="img/revistas/rfiua/n78/n78a13ea38.gif"> . However, this selection is arbitrary since the receiver   output is phase-invariant and therefore a phase shift can be applied to all   encoder/decoder functions with the aim to reduce inaccuracies in the synthesis. </font></p> <font size="2" face="verdana">    ]]></body>
<body><![CDATA[<p>The main source of   discrepancies are associated with the rise time of practical DTF's, which is   constrained by the filter bandwidth (and approximately equal to the inverse   reciprocal of the input pulse width) making the DTF response unable to keep up   the large variation of some target signals truncated with a rectangular pulse.   This point will be highlighted in a following section.</p>     <p>To test the CDMA scheme,   DTF's were designed using the filter topology previously reported in &#91;4, 9&#93; and   designed by allowing the DTF to have different inter-stage delay and gain   weights, according to a target signal. Code dictates filter design parameters. <a href="#Figura2">Figure   2</a> represents the DTF as a signal processor that affords the maximal flexibility.   In practical filters, broadband delay structures coupled to distributed gain   cells were designed to provide the necessary inter-stage delay. However, some   time mismatch is expected since each constituent stage of a delay line is   designed to feature a finite time delay resolution therefore the required   analogue delay time is obtained approximately by cascading delay stages. </p>     <p align="center"><a name="Figura2" id="Figura2"></a><img src="img/revistas/rfiua/n78/n78a13i02.gif"></p>     <p>Artificial transmission   lines are designed to show linear phase within the filter bandwidth   (approximately equal to a half of the Bragg cut-off frequency). Input pulses of   some tens of picoseconds undergo low dispersion and distortion effects as they   travel down on artificial transmission lines.</p>     <p><a href="#Figura3">Figure 3</a> shows pulse   transient responses of an 8-tap DTF obtained by adjusting separately a given   filter tap to the maximum gain and the remaining tap weights are set to zero.   Those are simulation results based on Advanced Design System (ADSTM). Full   electromagnetic simulation accounting for coupling among the different   monolithic microwave integrated circuits, (MMIC) elements and this was done by   MOMENTUMTM. Those correspond to filter implementations with uniformly spaced   stages. Inter-stage delay time was set to be equal to 25 ps. It shows that the   width of pulses traveling at different filter paths will increase to such a   level that tails from adjacent pulses interfere. High-frequency oscillations   arise owing to multiple reflections in filter stages. Such effects are taken   into consideration for DTF's designs with different inter-stage delays and gain   weights.</p>     <p align="center"><a name="Figura3"></a><img src="img/revistas/rfiua/n78/n78a13i03.gif"></p>     <p>Tap gain adjustment allows   compensating attenuation, pulse broadening and high-frequency oscillations   within the filter span time. Based on the resulting tap transient responses,   algorithms were developed to help in optimizing filter responses.</p>     <p>It is important to mention   that by making the first sub-band equal to zero; <i>c<sub>1</sub></i> and <i>M=5</i> in Eq. (1), sub-band   interference rejection is improved. In the following, the first sub-band   amplitude coefficient was made equal to zero in all DTF functions and <img src="img/revistas/rfiua/n78/n78a13ea39.gif"> is equal to zero to complete the phase vector in Eq. (1). </p>     <p><a href="#Figura4">Figure 4</a> shows the transient   responses of a 7-tap DTF (waveform normalized with its root mean square, r.m.s.)   which was synthesized to perform the reference correlation function. Time and   amplitude mismatches between the DTF function (simulated reference) and the   reference function are noticed. The designed waveform displays a large   oscillation beyond the symbol interval. </p>     <p align="center"><a name="Figura4"></a><img src="img/revistas/rfiua/n78/n78a13i04.gif"></p>     ]]></body>
<body><![CDATA[<p><a href="#Figura5">Figure 5</a> displays encoder   and decoder functions using the filter synthesis. It shows the waveforms of the   encoder (0,0,1,0,1) and the (orthogonal) decoder <img src="img/revistas/rfiua/n78/n78a13ea40.gif">.   Regarding the simulated decoder, it is seen that much of its energy is kept   within the time window. Figure 5 also allows contrasting the encoder function   and the corresponding DTF response; it exhibits large discrepancies at both   edges of the time-window. In fact, the analogue performance of this address   function leads to the worst decoding performance among the other receivers. It   is seen that time truncation of the ideal decoder function needs for   synthesizing initial and late taps of the DTF with high gains leading   necessarily to inaccuracies owing to a large pulse spread beyond the symbol   interval.</p>     <p align="center"><a name="Figura5"></a><img src="img/revistas/rfiua/n78/n78a13i05.gif"></p>     <p>In order to decode user   data, the outputs of both filters have to present temporal alignment previous   to the sub-band demodulation process. In particular; for this decoder (address)   function the finite rise time of the DTF shown in Figure 5 requires introducing   an additional delay line in the filter structure to align both filter   responses. Short transmission lines were introduced in the reference filter   function for such aim. An inter-stage time compensation of about 15 ps in the   first inter-stage delay <img src="img/revistas/rfiua/n78/n78a13ea41.gif"> (see Figure 2) was needed for this receiver.   The late tap was not set to a high gain according with the encoder function   (see Figure 5) because this creates large oscillations that affects even more   user decoding. We shift all the function phases in Table 1 by +1.1 radians. Inaccuracies   associated with time mismatch, finite rise times and high oscillations were   reduced. </p>     <p>In order to give an   assessment of the filter design method in Section 3, <a href="#Figura6">Figure 6</a> allows making   comparisons for two different reference functions used for decoding. This is   archived by considering that both the interferer and decoder are referred to   the same vector <img src="img/revistas/rfiua/n78/n78a13ea42.gif"> or <img src="img/revistas/rfiua/n78/n78a13ea43.gif"> (code matching is only shown for <img src="img/revistas/rfiua/n78/n78a13ea42.gif">   in that figure). Figure 6 shows results of the decoding achieved by the   receiver with address <img src="img/revistas/rfiua/n78/n78a13ea44.gif"> . Code matching and interference rejection are plotted over   the same time and frequency scales for comparison proposes. These results are   spectral components obtained after mixing the address correlation function with   the reference. The inset in Figure 5 shows the time response of the lowpass   filter to the mixer output (time scale not shown for clarity). The lowpass   filter was designed with a 4th-order Butterworth response with cut-off   frequency of 2.0 GHz.</p>     <p align="center"><a name="Figura6"></a><img src="img/revistas/rfiua/n78/n78a13i06.gif"></p>     <p>It is seen in Figure 6 that   the alternate vector <img src="img/revistas/rfiua/n78/n78a13ea42.gif"> provides better interference rejection,   providing a correlation peak ratio of 15:1 at the receiver output when compared   with the correlation peak for the decoder based on the reference vector <img src="img/revistas/rfiua/n78/n78a13ea43.gif">.   High correlation peak ratios (not shown herein) were also obtained for the   decoder with address vector <img src="img/revistas/rfiua/n78/n78a13ea45.gif">   and all the rest of encoders itemized on Table 1. </p>     <p>The lower interference   rejection ratio was obtained for the receiver with address <img src="img/revistas/rfiua/n78/n78a13ea46.gif">.   Results of such function are shown in <a href="#Figura7">Figure 7</a>. The alternate vector <img src="img/revistas/rfiua/n78/n78a13ea42.gif">   provides a marginal improvement over results based on the selection of <img src="img/revistas/rfiua/n78/n78a13ea43.gif">   in both time and frequency responses. The sharp frequency response to the   interferer makes the lowpass Butterworth filter unable to filter out large   interference. In this case, the correlation peak ratio can be increased if a   narrower lowpass filter is used at the mixer output. Additionally, it was   confirmed that in other decoding processes in which the rejection band is not   as narrower as that shown in Figure 7, the filter method in Section 3 improves   consistently the performance of the proposed encoder/decoder structures.</p>     <p align="center"><a name="Figura7"></a><img src="img/revistas/rfiua/n78/n78a13i07.gif"></p> </font>     <p><b><font size="3" face="verdana">5.  Discussion</font></b></p> <font size="2" face="verdana">     <p>The   encoding method proposed in this paper improves interference rejection margins   over previous demonstrations based on DS-CDMA. For instance; when using Gold   sequences of length 7 a correlation peak ratio of the order of 2:1 can be   obtained theoretically. The method based on decoding unipolar pulses shows a   slightly better correlation peak (theoretically a correlation peak ratio of 3:1   &#91;3&#93;). The use of Gold codes of length 7 can create potentially up to 7   quasi-orthogonal channels. However, the processing gain of the CDMA receiver   based on the 7-tap DTF is low in comparison with the cross-correlation variance   of Gold codes. On the other hand, for a truly asynchronous operation, the   cardinality of Optical Orthogonal Codes &#91;10&#93; applied to the DTF method in &#91;3&#93;   yields 2 simultaneous users for a cross-correlation peak constrained to 1.</p>     ]]></body>
<body><![CDATA[<p>In   the proposed encoding method, Hadamard codes of length 4 can provide up to 3   channels. The lower correlation peak obtained by our method was 4:1 for the   receiver that shows the larger discrepancies with the (target) waveform. Large   correlation peaks is a result of the orthogonality of the used codes and the   design of filter functions that allows reducing frequency overlap. In the light   of the large interference rejection margins achieved by our CDMA method, it is   believed that multi-level codes could increase effectively the number   orthogonal or quasi-orthogonal channels negating the need for TF's with large   taped delay lines or increased number of filter taps. Computer search of   unipolar-bipolar codes can be explored for such aim.</p> </font>     <p><b><font size="3" face="verdana">6.  Conclusions</font></b></p> <font size="2" face="verdana">     <p>This   paper introduces a new coding scheme that enables CDMA systems to make use of   the analogue processing of DTF's. In order for the filter to be a suitable   option, its finite-impulse response must approximate to a noise-like signal   which exhibits larger amplitude variations compared with the encoding patterns   used in standard DS-CDMA systems. A filter design method was proposed and its   suitability was tested using simulation results of DTF's specifically designed   for spectral encoding. The ability to correlating high-speed multilevel pulses   by distributed-based transversal filters makes available filter structures that   achieve sub-band encoding and decoding. Transient responses were obtained from   simulations of monolithic integrated transversal filter implementations at   layout level. Advantages of the proposed CDMA system are discussed assuming a   single concurrent user in the network showing better correlation peak ratios   when compared with those of previous demonstrations based on direct sequence   systems. </p> </font>     <p><b><font size="3" face="verdana">6.  References</font></b></p> <font size="2" face="verdana">     <!-- ref --><p> 1.&nbsp;      C. Lam, "To spread or not   spread: the myths of optical CDMA", in <i>13<sup>th</sup> Annual Meeting of the IEEE Lasers and Electro-Optics Society</i> (LEOS), R&iacute;o   Grande, Puerto Rico, 2000, pp. 810-811.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3166461&pid=S0120-6230201600010001300001&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> </p>     <!-- ref --><p> 2.&nbsp;      J. Rosas, J. Ingham, R. Penty   and I. White, "18 Gchips/s electronic CDMA for low-cost optical access networks", <i>Journal of Lightwave Technology</i>, vol.   27, no. 3, pp. 306-313, 2009.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3166463&pid=S0120-6230201600010001300002&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> </p>     <!-- ref --><p> 3.&nbsp;      M. Pimenta, "Design and   modelling of electronic processing circuits for optical code division multiple   access communication networks", Ph.D. thesis, University College London, London, UK, 2009.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3166465&pid=S0120-6230201600010001300003&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --></p>     ]]></body>
<body><![CDATA[<!-- ref --><p> 4.&nbsp;      J. Aguilar and I.   Darwazeh, "Dual Drain-line Distributed Cell Design for Multi-Gbit/s Transversal   Filter Implementations", in <i>IEEE   International Symposium on Circuits and Systems</i> (ISCAS), Kobe, Japan, 2005,   pp. 3958-3961.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3166467&pid=S0120-6230201600010001300004&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> </p>     <!-- ref --><p> 5.&nbsp;  L. Chuan-qi <i>et al.</i>, "A 10 Gbit/s OCDMA System Based   on Electric Encoding and Optical Transmission", <i>Optoelectronics Letters</i>, vol. 9, no. 6, pp. 473-476, 2013.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3166469&pid=S0120-6230201600010001300005&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> </p>     <!-- ref --><p> 6.&nbsp;      M. Kavehrad and D.   Zaccarin, "Optical Code-Division-Multiplexed Systems Based on Spectral Encoding   of Noncoherent Sources", <i>Journal of   Lightwave Technology</i>, vol. 13, no. 3, pp. 534-545, 1995.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3166471&pid=S0120-6230201600010001300006&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> </p>     <!-- ref --><p> 7.&nbsp;      P. Crespo, M. Honig and J.   Salehi, "Spread-Time Code-Division Multiple Access", <i>IEEE   Transactions on Communications</i>, vol. 43, no. 6, pp. 2139-2148, 1995.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3166473&pid=S0120-6230201600010001300007&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> </p>     <!-- ref --><p> 8.&nbsp;      A. Borjak, P. Monteiro,   J. O'Reilly and I. Darwazeh, "High-Speed Generalized   Distributed-Amplifier-Based Transversal-Filter Topology for Optical   Communication Systems", <i>IEEE Transactions   on Microwave Theory and Techniques</i>, vol. 45, no. 8, pp. 1453-1457, 1997.    &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;[&#160;<a href="javascript:void(0);" onclick="javascript: window.open('/scielo.php?script=sci_nlinks&ref=3166475&pid=S0120-6230201600010001300008&lng=','','width=640,height=500,resizable=yes,scrollbars=1,menubar=yes,');">Links</a>&#160;]<!-- end-ref --> </p>     ]]></body>
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