{"title":"Dispersion-Engineered Super-Gain Parametric Amplification in Nanoscale Optical Cavities","authors":"Özüm Emre Aşırım","doi":"10.1002/adpr.202300247","DOIUrl":null,"url":null,"abstract":"<p>The gain factor of the optical parametric amplification (OPA) process is known to be negligible in the small scale due to low-interaction-medium length. Hence, in the nanoscale, OPA is deemed as infeasible. Therefore, in small-scale-integrated optical devices, stimulated-emission-based amplifiers (lasers) are employed instead of OPAs. In contrast, the major advantage of OPAs over lasers is that unlike lasers which only provide amplification over a narrow spectral band, OPAs provide high-gain amplification over a very large, user-controlled spectral band. In this article, it is shown that OPA can yield wideband high-gain amplification over a nanoscale beam propagation distance through dispersion engineering. This is achieved by a proper tuning of the pump (source) wave frequency, which can maximize the effective medium nonlinearity by a few orders of magnitude, while concurrently maximizing the intracavity energy density, thereby compensating for the small co-propagation distance for the input (signal) and pump beams. In this study, it is shown that an input wave can be amplified by a factor <span></span><math>\n <semantics>\n <mrow>\n <msup>\n <mrow>\n <mn>10</mn>\n </mrow>\n <mn>8</mn>\n </msup>\n </mrow>\n <annotation>$\\left(10\\right)^{8}$</annotation>\n </semantics></math> in a nanoscale cavity via precise dispersion engineering. Both empirical and computational formulations are used for the investigation, which display a reasonable agreement.</p>","PeriodicalId":7263,"journal":{"name":"Advanced Photonics Research","volume":"5 5","pages":""},"PeriodicalIF":3.7000,"publicationDate":"2024-03-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/adpr.202300247","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Photonics Research","FirstCategoryId":"1085","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/adpr.202300247","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
The gain factor of the optical parametric amplification (OPA) process is known to be negligible in the small scale due to low-interaction-medium length. Hence, in the nanoscale, OPA is deemed as infeasible. Therefore, in small-scale-integrated optical devices, stimulated-emission-based amplifiers (lasers) are employed instead of OPAs. In contrast, the major advantage of OPAs over lasers is that unlike lasers which only provide amplification over a narrow spectral band, OPAs provide high-gain amplification over a very large, user-controlled spectral band. In this article, it is shown that OPA can yield wideband high-gain amplification over a nanoscale beam propagation distance through dispersion engineering. This is achieved by a proper tuning of the pump (source) wave frequency, which can maximize the effective medium nonlinearity by a few orders of magnitude, while concurrently maximizing the intracavity energy density, thereby compensating for the small co-propagation distance for the input (signal) and pump beams. In this study, it is shown that an input wave can be amplified by a factor in a nanoscale cavity via precise dispersion engineering. Both empirical and computational formulations are used for the investigation, which display a reasonable agreement.