{"title":"Microwave photonic signal processing exploiting coherent interactions between Brillouin Stokes and anti-Stokes resonances","authors":"R. Pant, S. A.","doi":"10.23919/URSIAP-RASC.2019.8738430","DOIUrl":null,"url":null,"abstract":"Generation and processing of RF signals using photonic technologies enable electromagnetic interference (EMI) free low loss, light weight microwave photonic processor [1]. Generation of RF signals is typically achieved by beating multiple optical frequencies, which are created by exploiting nonlinear optical phenomenon in high-Q resonators [2]. RF photonic signal processing, on the other hand, is performed by modulating a laser with the incoming RF signal and processing one of the modulation side bands using active or passive optical resonance to achieve microwave photonic notch filter, RF switch, etc. [3]. Many of these photonics based RF signal processors use a phase modulator or a dual-parallel Mach-Zehnder modulator and a passive filter to create out-of-phase side bands with unequal amplitude. An active or passive resonance is then used to equalize the amplitude of the two out-of-phase sidebands [3, 4]. The resulting destructive interference between the beat signals, which are obtained by beating of the carrier with upper and lower sidebands, results in creation of a rejection band centered at the frequency of equal amplitude. Since the two sidebands are out-of-phase, the induced insertion loss is high because of cancellation in the pass band.","PeriodicalId":344386,"journal":{"name":"2019 URSI Asia-Pacific Radio Science Conference (AP-RASC)","volume":"49 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-03-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2019 URSI Asia-Pacific Radio Science Conference (AP-RASC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.23919/URSIAP-RASC.2019.8738430","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Generation and processing of RF signals using photonic technologies enable electromagnetic interference (EMI) free low loss, light weight microwave photonic processor [1]. Generation of RF signals is typically achieved by beating multiple optical frequencies, which are created by exploiting nonlinear optical phenomenon in high-Q resonators [2]. RF photonic signal processing, on the other hand, is performed by modulating a laser with the incoming RF signal and processing one of the modulation side bands using active or passive optical resonance to achieve microwave photonic notch filter, RF switch, etc. [3]. Many of these photonics based RF signal processors use a phase modulator or a dual-parallel Mach-Zehnder modulator and a passive filter to create out-of-phase side bands with unequal amplitude. An active or passive resonance is then used to equalize the amplitude of the two out-of-phase sidebands [3, 4]. The resulting destructive interference between the beat signals, which are obtained by beating of the carrier with upper and lower sidebands, results in creation of a rejection band centered at the frequency of equal amplitude. Since the two sidebands are out-of-phase, the induced insertion loss is high because of cancellation in the pass band.