1. Random Lasing at Localization Transition in a Colloidal Suspension (TiO2@Silica)
- Author
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Fundação de Apoio à Pesquisa do Estado da Paraíba, Ministerio de Economía y Competitividad (España), Comunidad de Madrid, Conselho Nacional de Desenvolvimento Científico e Tecnológico (Brasil), Fundação de Amparo à Ciência e Tecnologia do Estado de Pernambuco, Fundação de Amparo à Pesquisa do Estado de São Paulo, Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (Brasil), Jiménez-Villar, Ernesto, Silva, Iran F. da, Mestre, Valdeci, Wetter, Niklaus U., López, Cefe, Oliveira, Paulo C. de, Faustino, Wagner M., Sá, Gilberto F. de, Fundação de Apoio à Pesquisa do Estado da Paraíba, Ministerio de Economía y Competitividad (España), Comunidad de Madrid, Conselho Nacional de Desenvolvimento Científico e Tecnológico (Brasil), Fundação de Amparo à Ciência e Tecnologia do Estado de Pernambuco, Fundação de Amparo à Pesquisa do Estado de São Paulo, Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (Brasil), Jiménez-Villar, Ernesto, Silva, Iran F. da, Mestre, Valdeci, Wetter, Niklaus U., López, Cefe, Oliveira, Paulo C. de, Faustino, Wagner M., and Sá, Gilberto F. de
- Abstract
Anderson localization of light and random lasing in this critical regime is an open research frontier, which besides being a basic research topic could also lead to important applications. This article investigates the random laser action at the localization transition in a strongly disordered scattering medium composed of a colloidal suspension of core-shell nanoparticles (TiO@Silica) in ethanol solution of Rhodamine 6G. The classical superfluorescence band of the random laser was measured separately by collecting the emission at the back of the samples, showing a linear dependence with pumping fluence without gain depletion. However, frontal collection showed saturation of the absorption and emission. Narrow peaks of approximately equal intensity are observed on top of the classical superfluorescence band, indicating suppression of the interaction between the peaks modes. The linewidth of these peaks is lower than that of the passive modes of the scattering medium. A method called fraction of absorbed pumping allowed us to infer that this peak's mode (localized modes) is confined to a shallow region near the input-pumping border.
- Published
- 2017