{"title":"Improving the stopband of the UWB bandpass filter with a novel compact 1-cell CRLHTL geometry with additional nulls","authors":"S. Kahng, J. Ju","doi":"10.1109/IWAT.2009.4906943","DOIUrl":null,"url":null,"abstract":"Previously, we suggested the unprecedented design of a very compact UWB bandpass filter, which is based on the 1-cell microstrip Composite Right- and Left-Handed Transmission-line(CRLH-TL)[1]. Though the design result turned out satisfactory in terms of Bandwidth, Insertion Loss, Return Loss, Group Delay variation and so on, it had a narrow stopband beyond the upper passband edge. Therefore, we present the improved design to widen the stopband from ‘10.6 GHz∼12.6 GHz’ to ‘10.6 GHz∼14.6 GHz’ by modifying the original structure to create additional nulls(or poles), and the resultant structure is still as small as ‘guided wavelength( λg )/9.4’.","PeriodicalId":166472,"journal":{"name":"2009 IEEE International Workshop on Antenna Technology","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2009-03-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2009 IEEE International Workshop on Antenna Technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IWAT.2009.4906943","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
Previously, we suggested the unprecedented design of a very compact UWB bandpass filter, which is based on the 1-cell microstrip Composite Right- and Left-Handed Transmission-line(CRLH-TL)[1]. Though the design result turned out satisfactory in terms of Bandwidth, Insertion Loss, Return Loss, Group Delay variation and so on, it had a narrow stopband beyond the upper passband edge. Therefore, we present the improved design to widen the stopband from ‘10.6 GHz∼12.6 GHz’ to ‘10.6 GHz∼14.6 GHz’ by modifying the original structure to create additional nulls(or poles), and the resultant structure is still as small as ‘guided wavelength( λg )/9.4’.