{"title":"Simulation performance of ASE-XGM wavelength converter for spectrum-sliced WDM system","authors":"S. Baruh, M. Martinez, M. R. Rocco Giraldi","doi":"10.1117/12.511050","DOIUrl":null,"url":null,"abstract":"We evaluate the performance of a wavelength conversion technique based on the modulation of the amplified spontaneous emission of semiconductor optical amplifiers through simulation software. Unlike conventional conversion technique the ASE-XGM does not require a CW probe signal. The converted wavelength is determined by an optical filter, which slices the modulated ASE spectrum. We focus on bit error rate (BER)conversion performance of a 2.5 Gbit/s non-return to zero, pseudo-random sequence of order 11. BER values better than 10-9 are achieved for signal input power ranging from -6 dBm to 0 dBm, and for a slicing filter centered around 0.4 nm red shifted from signal wavelength.","PeriodicalId":282161,"journal":{"name":"SPIE ITCom","volume":"17 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2003-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"SPIE ITCom","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1117/12.511050","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
We evaluate the performance of a wavelength conversion technique based on the modulation of the amplified spontaneous emission of semiconductor optical amplifiers through simulation software. Unlike conventional conversion technique the ASE-XGM does not require a CW probe signal. The converted wavelength is determined by an optical filter, which slices the modulated ASE spectrum. We focus on bit error rate (BER)conversion performance of a 2.5 Gbit/s non-return to zero, pseudo-random sequence of order 11. BER values better than 10-9 are achieved for signal input power ranging from -6 dBm to 0 dBm, and for a slicing filter centered around 0.4 nm red shifted from signal wavelength.