<?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">JCC</journal-id><journal-title-group><journal-title>Journal of Computer and Communications</journal-title></journal-title-group><issn pub-type="epub">2327-5219</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jcc.2015.33008</article-id><article-id pub-id-type="publisher-id">JCC-54727</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>
 
 
  Design of Miniaturized Band-Pass Filter with Composite Right/Left-Handed Transmission Line
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Meng</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fang</surname><given-names>Zhang</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>Xingfang</surname><given-names>Luo</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Laboratory of Nanomaterials and Sensors, School of Physics, Communication and Electronics, Jiangxi Normal University, Nanchang, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>xfluo@jxnu.edu.cn(MZ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>17</day><month>03</month><year>2015</year></pub-date><volume>03</volume><issue>03</issue><fpage>44</fpage><lpage>48</lpage><history><date date-type="received"><day>January</day>	<month>2015</month></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>
 
 
   In this paper, a new miniaturized wide-pass-band filter at U band based on composite right/left- handed transmission line (CRLH TL) is implemented. The CRLH TL contributed to a broadband filter is a balanced structure with a small size of only 1.428 mm*0.5530 mm. The frequency characteristics are simulated and the results show that the 3 dB band width of the proposed filter is about 13.5 GHz from 45.8 GHz to 59.3 GHz. The insertion loss is quite flat through the pass-band and the return loss is relatively low. 
 
</p></abstract><kwd-group><kwd>Miniaturized</kwd><kwd> Composite Right/Left-Handed Transmission Line</kwd><kwd> Bandpass Filter</kwd><kwd> Metamaterial</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Band-pass filters (BPF) are essential components in the modern radar and wireless communication system whose performance can greatly influence the behavior of the whole system. Therefore, small size, flat group delay, better frequency selection characteristic, and broadband filter are needed in practical Engineering. The resonator of the filter is the key device that determines the main characteristics of the filter.</p><p>In 2003, a resonator based on composite right/left-handed transmission line (CRLH TL) [<xref ref-type="bibr" rid="scirp.54727-ref1">1</xref>] is proposed by Caloz [<xref ref-type="bibr" rid="scirp.54727-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.54727-ref3">3</xref>], having attracted great interest from the scientific and engineering field owing to its potential applications of negative effective permeability. As is known, CRLH TL metamaterials are composed of left- handed (LH) and right-handed (RH) components [<xref ref-type="bibr" rid="scirp.54727-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.54727-ref5">5</xref>], which has been approved to be able to realize miniaturization of structure [<xref ref-type="bibr" rid="scirp.54727-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.54727-ref7">7</xref>] utilizing its dispersive phase properties [<xref ref-type="bibr" rid="scirp.54727-ref8">8</xref>]. There are various researches on the application of the ultrawideband (UWB) band pass filter (BPF) with CRLH TL [<xref ref-type="bibr" rid="scirp.54727-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.54727-ref10">10</xref>]. The resonant mode of traditional TL (which is called right-handed TL.) resonator only can be positive and the resonant length is closely related to the size of the resonator. While, the resonant mode of CRLH TL can be any arbitrary integer, and the resonance frequency of CRLH TL only depends on the values of L and C in resonant unit, which results in significantly reducing the size of passive components. The CRLH TL has wide application prospect in the design of filter due to its characteristics of frequency selective and its balanced structure, and which opens up a new way for the design of broadband filter. Moreover, compared with the traditional TL resonator, the structure with CRLH TL has the advantage of low loss.</p><p>At present, millimeter band offers the benefits of the higher guaranteed data rates to some wireless technology, longer distance transmissions and more cost effectiveness than optic systems. With the development of ultra-high speed and high-capacity point-to-point communication systems in recent years, the research of millimeter wave communication is needed to satisfy the demand of broad market. In this paper, a microwave band-pass filter based on CRLH TL at U band is presented.</p></sec><sec id="s2"><title>2. Analysis and Design of the Proposed Bandpass Filter</title><p>The CRLH TL in [<xref ref-type="bibr" rid="scirp.54727-ref2">2</xref>] consists of interdigital capacitance and grounding via stub, and the interdigital capacitor is a multi-finger periodic structure as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><p>An approximate expression for the interdigital capacitance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x5.png" xlink:type="simple"/></inline-formula> is given by [<xref ref-type="bibr" rid="scirp.54727-ref11">11</xref>]</p><disp-formula id="scirp.54727-formula596"><label>, (1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/54727x6.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54727-formula597"><label>, (2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/54727x7.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54727-formula598"><label>. (3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/54727x8.png"  xlink:type="simple"/></disp-formula><p>where N is the number of the interdigital. The proposed CRLH TL is fabricated on a microstrip substrate with dielectric constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x9.png" xlink:type="simple"/></inline-formula> and thickness<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x10.png" xlink:type="simple"/></inline-formula>.</p><p>In this paper, the obtained structure of the bandpass filter with CRLH TL is shown as <xref ref-type="fig" rid="fig2">Figure 2</xref>. A substrate with a relative dielectric constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x11.png" xlink:type="simple"/></inline-formula> of 5.9 and a thickness <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x12.png" xlink:type="simple"/></inline-formula> of 0.1 mm is chosen for the filter design.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> An interdigital capacitor configuration</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/54727x13.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Layout of the proposed band-pass filter (a = 1.428 mm, b = 0.04 mm, c = 0.16 mm, L = 0.2 mm, tt = 0.5530 mm, tw = 0.86 mm)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/54727x14.png"/></fig><p>The size of proposed filter is only 1.428 mm * 0.5530 mm, which is smaller than the traditional filter, then the compact size has been achieved for low-cost microwave monolithic integrated circuit (MMIC) [<xref ref-type="bibr" rid="scirp.54727-ref12">12</xref>]. <xref ref-type="fig" rid="fig3">Figure 3</xref> presents the modified T-typed equivalent circuit of a third-order inline coupling band-pass filter, which consists of one shunt resonator and two series resonators. It is seen here that the series capacitors for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x15.png" xlink:type="simple"/></inline-formula> is realized by two identical interdigital capacitors, while the shunt inductor for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x16.png" xlink:type="simple"/></inline-formula> is realized by a short-circuited stub. The resonant frequency of shut and series are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x17.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x18.png" xlink:type="simple"/></inline-formula> as</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x19.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x19.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x20.png" xlink:type="simple"/></inline-formula>. (4)</p><p>The propagation constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x21.png" xlink:type="simple"/></inline-formula> of the CRLH TL is given by [<xref ref-type="bibr" rid="scirp.54727-ref13">13</xref>]</p><disp-formula id="scirp.54727-formula599"><label>, (5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/54727x22.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x23.png" xlink:type="simple"/></inline-formula>.</p><p>It means that the CRLH TL based on the basic LC circuit supports a forward wave in the RH effect area (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x25.png" xlink:type="simple"/></inline-formula>), where the structure works in the low-pass band, while a backward wave is in the LH effect area (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x26.png" xlink:type="simple"/></inline-formula>), where the structure operates on the high-pass band. In general, there is a stop-band occurs between transition from LH to RH propagation. However, when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x27.png" xlink:type="simple"/></inline-formula>, the proposed CRLH TL filter in this paper is a balanced structure which has a transition frequency <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x29.png" xlink:type="simple"/></inline-formula> without stop-band.</p><p>The dispersion diagram of the obtained balanced CRLH TL filter is shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>. The bandwidth of balanced CRLH TL is from high-pass left-handed cut-off frequency <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x30.png" xlink:type="simple"/></inline-formula> to low-pass right-handed cut-off frequency <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x31.png" xlink:type="simple"/></inline-formula> with no obvious stop-band, and a broad BPF is able to obtained. The cut-off frequencies (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x32.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x33.png" xlink:type="simple"/></inline-formula>) are given below,</p><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> T-type equivalent circuit of the 3rd order band-pass filter</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/54727x34.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Dispersion diagram of composite right/left-handed transmission line</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/54727x35.png"/></fig><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x36.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x37.png" xlink:type="simple"/></inline-formula>. (6)</p><p>According to Equations (1)-(4), the finger width<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x38.png" xlink:type="simple"/></inline-formula>, length<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x39.png" xlink:type="simple"/></inline-formula>, and space<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/54727x40.png" xlink:type="simple"/></inline-formula>, as well as the number of the fingers N determines the dimensions of the interdigital capacitors, and the dimensions of the short-circuited stub, namely, the width and length, which results in an increase in the bandwidth.</p></sec><sec id="s3"><title>3. Results</title><p><xref ref-type="fig" rid="fig5">Figure 5</xref> presents the simulated Scattering (S) parameter frequency responses to band-pass filter. It is observed that the proposed structure has a pass-band characteristic with two obvious transmission poles at 48.6 GHz and 54.4 GHz which provides a good return loss. The 3 dB bandwidth of the implemented filter is about 13.5 GHz from 45.8 GHz to 59.3 GHz, and the relative bandwidth is about 25.7%. Furthermore, the return loss is lower than −13 dB and the insertion loss is relatively flat, implying a good matching impedance. The curve of variation of group delay over the pass-band is shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>. Apparently, it is not a good practice to realize highly selective filters with proposed filter, which meets the broadband requirements.</p></sec><sec id="s4"><title>4. Conclusion</title><p>A new U band band-pass filter based on CRLH TL is presented in this paper. The proposed structure has a smaller size compared with traditional filter. A wide pass-band filter is obtained by using balanced CRLH TL structure, and the simulation results show that the proposed filter has a quite smooth group delay, and the insertion loss is relatively flat in the pass-band which shows that the ripple of pass-band is small enough, implying that the impedance matches better. The miniaturized wide band-pass filter using CRLH TL has certain reference value in the modern radar and wireless communication system of millimeter wave.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work is supported by National Natural Science Foundation of China (Grant Nos. 51361013), Natural</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Scattering parameter of proposed band-pass filter</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/54727x41.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Group delay of the proposed band-pass filter</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/54727x42.png"/></fig><p>Science Foundation of Jiangxi Province of China (Grant Nos. 20122BAB201027) and Science and Technology Support Program of Jiangxi Province of China (Grant Nos. 20121BBE50028).</p></sec><sec id="s6"><title>Cite this paper</title><p>Meng Zhang,Fang Zhang,Xingfang Luo, (2015) Design of Miniaturized Band-Pass Filter with Composite Right/Left-Handed Transmission Line. 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