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ANOVELMETHODFORDESIGNINGDUALFREQUENCYSLOTPATCHANTENNASWITHTWOPOLARIZATIONSWUDI1,OHISHIBASHIHIDEKAZU2,SEOKAZUYUKI2,INAGAKINAOKI31DEPARTMENTOFCOMMUNICATIONENGINEERING,SHANGHAIUNIVERSITY,SHANGHAI200072,CHINA2KOJIMAR3NAGOYAINSTITUTEOFTECHNOLOGY,NAGOYA4668555,JAPANABSTRACTTHISPAPERPRESENTSANEWMETHODFORDESIGNINGADUALFREQUENCYPATCHANTENNAWITHCIRCULARANDLINEARPOLARIZATIONSDUALFREQUENCYOPERATIONSAREBEHAVEDBYETCHINGTWONARROWSLOTSCLOSETOTHERADIATINGEDGESOFARECTANGULARPATCHTHECIRCULARPOLARIZATIONATTHELOWERRESONANTFREQUENCYOFTHEDUALFREQUENCYANTENNACANBEACHIEVEDBYSETTINGAPERTURBATIONSEGMENTATANAPPROPRIATELOCATIONINTHEPATCHELEMENT,ANDPLACINGTHEFEEDPOINTONTHEDIAGONALAXISSEVERALEXPERIMENTALRESULTSOFADESIGNEDANTENNASHOWTHEGOODCHARACTERISTICSFORCIRCULARANDLINEARPOLARIZATIONSATBOTHRESONANTFREQUENCIESCLCNUMBERTN8211DOCUMENTCODEAKEYWORDSDUALFREQUENCYSLOTPATCHANTENNASLINEARPOLARIZATIONCIRCULARPOLARIZATIONINRADARANDCOMMUNICATIONSYSTEMS,DUALFREQUENCYOPERATIONSAREOFTENREQUIREDSPECIALLY,INMODERNMOBILEGLOBALPOSITIONSYSTEMGPS,ITWILLBEDESIRABLETHATONEOFTWOFREQUENCIESISTHECIRCULARPOLARIZATIONPLANARANTENNAHASBEENINVESTIGATEDFORMULTIFREQUENCYVERYWELLSINCEITISADVANTAGEOUSINLOWCOST,LOWWEIGHTANDCONFORMABILITYEARLYDUALFREQUENCYPLANARANTENNAISMULTILAYEREDSTACKEDPATCHSTRUCTURE,ANDTHERADIATINGELEMENTISUSEDTOBECIRCULAR1,ANNULAR2,RECTANGULAR3ANDTRIANGULARPATCHES4RECENTLY,ADUALFREQUENCYANTENNAISINTRODUCEDINWHICHTHESTRUCTUREISDINGLELAYERPATCHWITHTWOSLOTSCLOSETOTHERADIATINGEDGES,ANDGOODPERFORMANCESOFSIMULTANEOUSIMPEDANCEMATCHINGANDGAINAREDEMONSTRATEDFORBOTHRESONANTFREQUENCIESHOWEVER,ALLTHECONVENTIONALINVESTIGATIONSAREONLYFORTHECASEINWHICHTHEANTENNAPOLARIZATIONISLINEAR,WHILETHEDUALFREQUENCYANTENNAWITHCIRCULARPOLARIZATIONHASNOTBEENTOUCHEDYETINTHISPAPER,WEPRESENTADESIGNMETHODOFADUALFREQUENCYANTENNAWITHCIRCULARANDLINEARPOLARIZATIONSBASEDONTHECONVENTIONALINVESTIGATIONFORTHEDUALFREQUENCYLINEARPOLARIZATIONANTENNA57,TWORESONANTFREQUENCIESAREDETERMINEDBYADJUSTINGTHESIZEOFTHEPATCHELEMENTANDTHESLOT,ASWELLASTHELOCATIONOFTHESLOTINTHEELEMENTTHEKEYTOOBTAINACIRCULARPOLARIZATIONFORANANTENNAISTOSATISFYTHECONDITIONFOREXCITINGCIRCULARPOLARIZATION,IE,THECIRCULARPOLARIZATIONCANBEEXCITEDBYSETTINGTHEPERTURBATIONSEGMENT,ATANAPPROPRIATELOCATIONINTHEPATCHELEMENT,ANDBYPLACINGTHEFEEDPOINTONTHEDIAGONALAXISWEHAVEEXPERIMENTALLYOBTAINEDTHECIRCULARANDTHELINEARPOLARIZATIONSATBOTHLOWERANDUPPERFREQUENCIES,ANDSOMEEXPERIMENTALRESULTSWILLBEDEMONSTRATEDONTHEREFLECTIONLOSSATINPUTPORTANDTHERADIATIONPATTERNOFTHEANTENNA1CONFIGURATIONOFCONVENTIONALDUALFREQUENCYPATCHANTENNAFIGURE1SHOWSACONFIGURATIONOFACONVENTIONALDUALFREQUENCYANTENNAWITHLINEARPOLARIZATIONTWORESONANTFREQUENCIESAREBEHAVEDBYETCHINGTWOSLOTSCLOSEANDPARALLELTOTHERADIATINGEDGES,ANDTHELOWERRESONANTFREQUENCYISDETERMINEDBYTHEOUTLINESIZEOFTHEPATCHELEMENT,WHILETHEUPPERRESONANTFREQUENCYISDETERMINEDBYTHESIZEANDTHEPOSITIONOFTHETWOSLOTSINTHEPATCHELEMENTBECAUSETHESLOTSARECLOSELYLOCATEDTOTHERADIATINGEDGES,AMINORPERTURBATIONOFTHETM10MODECANBEEXPECTEDASFORUNPERTURBEDTM30MODE,SINCETHESLOTSARELOCATEDWHERETHECURRENTSHALLBESIGNIFICANT,THECURRENTWILLBESTRONGLYMODIFIED,ANDAPERTURBEDTM30RADIATIONPATTERNSIMILARTOTHETM10MODECANBEOBTAINEDOUROBJECTINTHISINVESTIGATIONISTOOBTAINADUALFREQUENCYANTENNAWITHBOTHPOLARIZATIONINWHICHTHELOWERFREQUENCYISWITHACIRCULARPOLARIZATIONANDTHEUPPERFREQUENCYISWITHALINEARPOLARIZATIONFORASQUAREPATCHANTENNAWITHLENGTHOFTWOPARALLELSUBTENDSOFTHEPATCHELEMENTINORDERTOSETAPERTURBATIONSEGMENTAREAOFSFEDBYONEPORT,AWAYTOEXCITEACIRCULARPOLARIZATIONISTOEXTENDTHES,ANDPLACETHEFEEDINGPOINTONTHEDIAGONALAXISWHENANAPPROPRIATEPERTURBATIONISSELECTED,ACIRCULARPOLARIZATIONWITHAGOODAXIALRATIOCANBEOBTAINEDFIG1CONFIGURATIONOFCONVENTIONALDUALFREQUENCYANTENNA2DESIGNINGFORDUALFREQUENCYSLOTPATCHANTENNASWITHTWOPOLARIZATIONSINACONVENTIONALINVESTIGATIONFORDUALFREQUENCYWITHLINEARPOLARIZATION57,TOENSUREAGOODRADIATIONEFFICIENCYATBOTHFREQUENCIES,THEASPECTRATIOBETWEENTHETWOSIDESOFTHEPATCHISTAKENINTHERANGE1078LWANDTHELOWERFREQUENCYISDETERMINEDBY2“2/,LRRCFLTWHERECISTHEVELOCITYOFLIGHTINFREESPACE,ISTHEEFFECTIVEPERMITTIVITYGIVENBYR31210,2RYXXAND41504WLWL5“,RGTHERE610361,28074LN25185XYGYXANDTHEUPPERFREQUENCYISDETERMINEDBY72/,HRRCFLLDWTINABOVEEXPRESSION,THEPARAMETERSOFW,L,T,W,D,LAREREFERREDTOFIG2,ANDTHEISTHEDIELECTRICCONSTANTOFTHESUBSTRATEHOWEVER,INTHISSTUDY,INORDERTOOBTAINRACIRCULARPOLARIZATIONATTHELOWERRESONANTFREQUENCY,THEASPECTRATIOOFTHEOUTLINESIZEOFTHEPATCHWILLBECHANGEDSOTHATTHEMENTIONEDFORMULASABOVEWILLNOTBECOMPLETELYSATISFIEDFIG2CONFIGURATIONOFDUALFREQUENCYWEPRESENTADESIGNMETHODFORDUALFREQUENCYSLOTPATCHANTENNAWITHTWOPOLARIZATIONASFOLLOWSSTEP1DESIGNASQUAREPATCHANTENNAWITHTHEDESIRABLELOWERFREQUENCYF10BYUSINGACONVENTIONALMETHODSTEP2ETCHTWOSLOTSCLOSEANDPARALLELTOTHERADIATINGTOBEHAVETHEDUALFREQUENCIESOPERATIONBYUSINGEQ7HOWEVERTHELOWERRESONANTFREQUENCYF10WILLCHANGE,SINCETHESLOTSMODIFYTHECURRENTDISTRIBUTIONOFTHETM10STEP3ADJUSTTHESIZEOFTHEANTENNAELEMENTTOOBTAINTHEDESIREDLOWERRESONANTFREQUENCYSTEP4ADJUSTTHELENGTHANDTHEWIDTHOFTHESLOTSTOOBTAINTHEUPPERRESONANTFREQUENCYF30STEP5SETPERTURBATIONSEGMENTANDPLACETHEFEEDPOINTONTHEDIAGONALAXISOFTHEANTENNATOOBTAINTHECIRCULARPOLARIZATIONATTHELOWERRESONANTFREQUENCYF103EXPERIMENTALRESULTSANDDISCUSSIONWEEXPERIMENTALLYDESIGNEDADUALFREQUENCYPATCHANTENNAWITHTWOPOLARIZATIONSFIGURE2SHOWSTHECONFIGURATIONOFTHEANTENNA,ANDTHESPECIFICATIONSARELISTEDINTABLE1INTHISCONFIGURATIONOFTHEANTENNA,WEEXTENDEDTHELEDGEOFTHEPATCHANTENNATOSETTHEPERTURBATIONSEGMENT,ANDPLACEDTHEFEEDPOINTONTHEDIAGONALAXISTOACHIEVETHECIRCULARPOLARIZATIONTABLE1SPECIFICATIONSOFADUALFREQUENCYPATCHANTENNAWITHTWOPOLARIZATIONGPSVICSFREQUENCY/GHZ157525POLARIZATIONCIRCULARLINEARRETURNLOSS1515GAIN3DBIC5DBIFIGURE3SHOWSAMEASUREDREFLECTIONLOSSOFADESIGNEDDUALFREQUENCYANTENNAFEDBY50COAXIALPROBEFROMTHISFIGURE,ITCANBEOBSERVEDTHATTWORESONANTFREQUENCIESAREACHIEVESATDESIREDFREQUENCIES1575GHZAND250GHZ,WHICHWILLBEEMPLOYEDTOMOBILEGLOBALPOSITIONSYSTEMGPSANDVEHICLEINFORMATIONCOMMUNICATIONSYSTEMVICS,ANDAGOODSIMULTANEOUSIMPEDANCEMATCHINGWASOBTAINEDFORREFLECTIONLOSSVALUES17DBAT1575GHZAND27DBAT25GHZFIG3FREQUENCYCHARACTERISTICSOFREFLECTIONLOSSFIGURE4SHOWSTHEAXIALRATIOVARIATIONWITHTHEFREQUENCYFORTHISDESIGNEDANTENNAITISSEENTHATTHEBESTVALUEOFTHEAXIALRATIOISABOUT1DBAT1575GHZFIG4FREQUENCYCHARACTERISTICSOFAXIALRATIOFIGURE5SHOWSTHEMEASUREDIMPEDANCECHARACTERISTICSOFTHEANTENNAINCORRESPONDENCEWITHFIG3ITDEMONSTRATEDTHATAPERTURBATIONISSETFORCIRCULARPOLARIZATIONATLOWERFREQUENCY1575GHZFIG5FREQUENCYCHARACTERISTICSOFINPUTIMPEDANCEFIGURE6SHOWSTHERADIATIONPATTERNOFTHECIRCULARPOLARIZATIONOFTHEDESIGNEDANTENNAATTHELOWERRESONANTFREQUENCY1575GHZINTHISFIGURE,WEUSEDTHEUNITDBICFORGAIN,WHICHCANBECALCULATEDASFOLLOWSWHERE,GMAXDBIDENOTESTHEMEASUREDMAX/20120LOGARGDBICIMAXIMUMGAININDBI,ARISTHEMEASUREDAXIALRATIOAGAINOF37DBICWASFOUNDFORPATCHANTENNAWITHCIRCULARPOLARIZATIONAT1575GHZFIG6RADIATIONPATTERNOFCIRCULARPOLARIZATIONFINALLY,THERADIATIONPATTERNOFTHELINEARPOLARIZATIONATTHEUPPERFREQUENCY25GHZISSHOWNINFIG7THISISTHEPERTURBEDTM30MODE,HOWEVER,BECAUSETHETWOSLOTSEXISTINTHEPATCH,THESHAPEOFTHERADIATIONPATTERNOFTHEPERTURBEDTM30MODEBECOMESSIMILARTOTHATOFTM10MODEAGAINOF5DBIWASOBTAINEDFORPATCHANTENNAWITHLINEARPOLARIZATIONAT25GHZFIG7RADIATIONPATTERNOFLINEARPOLARIZATION4CONCLUDINGREMARKSANOVELDESIGNMETHODFORADUALFREQUENCYPATCHANTENNAWITHBOTHCIRCULARANDLINEARPOLARIZATIONISPRESENTEDINTHISPAPERTWORESONANTFREQUENCIESAREBEHAVEDBYETCHINGTWOSLOTSCLOSETOTHERADIATINGEDGESINTHERECTANGULARPATCH,ANDTHECIRCULARPOLARIZATIONATTHELOWERRESONANTFREQUENCYISACHIEVEDBYSETTINGAPERTURBATIONSEGMENTINTHEPATCHELEMENT,ANDBYPLACINGTHEFEEDPOINTONTHEDIAGONALAXISADUALFREQUENCYANTENNAWITHBOTHPOLARIZATIONS,WHICHWILLBEUSEDTOGPSANDVICSFORMOBILECOMMUNICATION,ISDESIGNEDBYUSINGPRESENTEDMETHODASFORMEASUREDRESULT,ITDEMONSTRATEDTHATTHEDESIGNEDANTENNAHASTWORESONANTFREQUENCY,INWHICHONEISACIRCULARPOLARIZATIONWITHANAXIALRATIO1DBANDGAIN37DBICATLOWERFREQUENCY,ANDTHEOTHERISALINEARPOLARIZATIONWITH5DBIATTHEUPPERFREQUENCYREFERENCES1LONGSA,WALTONMDADUALFREQUENCYSTACKEDCIRCULARDISCANTENNAJIEEETRANSANTENNASPROPAGAT,1979,AP272702732DAHELEJS,LEEKF,WONGDPDUALFREQUENCYTACKEDANNULARRINGMICROSTRIPANTENNAJIEEETRANS,1987,AP3511128112853WANGJ,FRALICHR,WUC,ETALMULTIFUNCTIONALAPERTURECOUPLEDSTACKANTENNAJELECTRONLETT,1990,2625206720684MIRSCHEKARSYANKALD,HASSANIHRCHARACTERISTICSOFSTACKEDRECTANGULARANDTRIANGULARPATCHANTENNASFORDUALBANDAPPLICATIONAIEE8THICAPC1993EDINBURGH5MACIS,BFFIGENTILIG,AVITABILEGSINGLE2LAYERDUAL2FREQUENCYPATCHANTENNAJELECTRONICSLETTERS,1993,2916144114436MACIS,BIFFIGENTILIG,PIAZZESIP,ETALDUALBANDSLOTLOADEDPATCHANTENNAJIEEEPROCEEDINGSH,1995ACIS,BFFIGENTILIGDUALFREQUENCYPATCHANTENNASJIEEEANTENNASANDPROPAGATIONMAGAZINE,1997,3961320新的双频双极化开槽微带天线的设计方法吴迪,大石桥秀和,漱尾和之,蹈垣直树(1上海大学通信学院,上海20072;2小岛总合研究所,爱知县4700207,日本;3名古屋工业大学,名古屋市4668555,日本)摘要提出了一种同时具有圆极化和线极化的双频新型开槽微带天线的设计方法。天线双频工作是通过分别在靠近方形微带天线的两个辐射边处各开一个平行的窄槽来实现的。在较低的谐振频率处圆极化的可以通过在天线辐射单元上适当地设置摄动元素,并将馈电点移到辐射单元的对角线上。一个设计天线的测试结果给出了该天线在两个谐振频率上具有很好的圆极化和线极化的天线性能。关键词双频;开槽微带天线;线性极化;圆极化在雷达和通信系统中,经常需要双频工作。特别是在现代的移动全球定位系统中,通常要求双频之一为圆极化。因为平面天线在低成本、重量轻和稳定性方面的优点,已经被广泛研究并较好的应用于多频带系统中。早期的双频平面天线是多层栈式贴片结构,它的辐射单元习惯上为圆形、环形、矩形和三角形。最近,提出了一种双频天线,这种天线的结构是单层贴片,且有两个槽靠近辐射边缘,并且在两个谐振频率上既实现阻抗匹配又具有好的增益性能。然而,常规的研究仅仅针对线性极化的天线,拥有圆极化的双频天线却还没有被实现。本文中,在双频线极化天线传统研究的基础上,我们提出一种设计双频天线的方法,可设计出同时具有圆极化和线性极化特性的双频天线。两个谐振频率取决于调节贴片单元、槽的大小以、及槽在天线单元上的位置。一个天线获得圆形极化的关键是满足激励圆形极化的条件,例如通过设置摄动元素在贴片单元合适的位置上,并将馈点设置于对角轴线上,这样圆极化就可以被激励。我们已经用实验的方法在高低频率上获得了圆极化和线极化,并且将会展示一些关于天线输入端反射损失和辐射形式的实验性结果。1传统双频微带贴片天线的结构图1显示了传统线极化双频天线的结构。通过在辐射边缘蚀刻两个紧密平行的槽,两个谐振频率就被表现了出来,并且较低的谐振频率取决于贴片单元轮廓的大小,而较高的谐振频率取决于在贴片单元内的两个槽的大小和位置。因为两个槽设计在辐射边缘很近,所以在TM10模式下,应该得到较小的摄动单元。对于无摄动单元的TM30模式来说,由于两个槽位于对电流很重要的位置,所以电流将会发生很大的变化,而且将会得到一个与TM10相似的有干扰的TM30辐射图。我们的研究目的是获得一个具有圆极化和线极化的双频微带天线,这个天线具有如下特点对于低频来说是圆极化的,对于高频来说是线极化的。对于一个端口反馈面积为S的正方形贴片天线来说,一种激励圆极化的方法就是延长贴片单元平行边的长度,设置一个摄动单元S,并且将馈点设置在对角线上。当选择了一个合适的摄动单元时,将会获得一个具有很好轴比的圆极化天线。图1传统双频天线的结构2双频双极化开槽贴片天线的设计在双频线极化天线的传统研究中,为确保在双频上都具有好的辐射效率,贴片两边的纵横比取值范围是(1)078LW并且低频取决于(2)“2/,LRRCFLT其中C为自由空间的光速,为有效的介电常数,通常R(3)1210,2RYXX(4)54WLWL(5)“,RGT这里(6)10361,28074LN25185XYGYX高频取决于(7)2/,HRRCFLLDWT上述表达式中,参数W,L,T,W,D,L参阅图2,是基底的介电常数。然R而,在本文研究中,为在低频端获得一个圆极化,贴片轮廓的纵横比将会改变,因此,上述公式将不会完全得到满足。图2双频天线的结构我们提出了一种双频开槽双极化天线的设计方法,如下所述第一步用传统方法设计符合要求的低频的方形贴片天线。第二步应用方程(7),刻蚀两个与辐射边缘很近的平行槽来实现双频工作。然而,由于两槽改变了TM10的电流分布,较低的谐振频率F10将会改变。第三步校正天线单元的大小来获得所想要的低频。第四步校正两槽的长宽来获得较高的谐振频率F30。第五步设置天线的摄动单元和馈点来获得在低谐振频率下的圆极化。3实验结果与讨论我们用实验的方法设计了一个双频双极化贴片天线。图2展示了天线的结构,天线的详细说明如表1所示。在这个天线结构中,我们延长贴片天线的L边来来调节摄动元素,而将馈点设置在对角线上以便获得圆极化特性。表1具有双极化的双皮贴片天线的详细说明GPSVICSFREQUENCY/GHZ157525POLARIZATIONCIRCULARLINEARRETURNLOSS1515GAIN3DB5DB图3显示了测量到的所设计双频天线的反射损失,天线是由50同轴电缆反馈的。由这幅图可见,两个谐振频率均在所需的1575GHZ和250GHZ两个频点附近,这两个频率将被应用于GPS和VICS,并同时实现了较好的阻抗匹配在1575GHZ附近的反射损失值为17DB,在25GHZ附近的反射损失值为27DB。图3反射损失的频率特征图4显示了这个天线的轴比随频率变化而变化的关系。可以看出在1575GHZ时的最佳轴比为1DB。图4轴比的频率特性与图3相比,图5显示了测量到的天线阻抗特性。这说明在低频1575GHZ出为实现圆极化而留有摄动余量。图5输入阻抗的频率特性图6显示了在较低谐振频率1575GHZ上设计的圆极化天线的辐射图。图中,我们使用单位DBIC来表示增益大小

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