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Amplified spontaneous emission and lasing in conducting polymers and fluorescent dyes in opals as photonic crystals

K. YoshinoDepartment of Electronic Engineering, Graduate School of Engineering, Osaka University, Yamada-Oka, Suita, Osaka 565-0871, JapanSatoshi TatsuharaDepartment of Electronic Engineering, Graduate School of Engineering, Osaka University, Yamada-Oka, Suita, Osaka 565-0871, JapanY. KawagishiDepartment of Electronic Engineering, Graduate School of Engineering, Osaka University, Yamada-Oka, Suita, Osaka 565-0871, JapanMasanori OzakiDepartment of Electronic Engineering, Graduate School of Engineering, Osaka University, Yamada-Oka, Suita, Osaka 565-0871, JapanAnvar ZakhidovDepartment of Thermophysics, Uzbek Academy of Sciences, Katartal 28, Chilernzar C, Tashkent 700135, UzbekistanZ. Valy VardenyPhysics Department, University of Utah, Salt Lake City, Utah 84112
Applied Physics Lettersjournal1999en
ABI

Аннотация

Spectral narrowing of photoluminescence (PL) and evolution of sharp emission lines upon optical excitation have been observed in opals made of SiO2 spheres infiltrated with conducting polymers such as OOPPV and MDDOPPV and also fluorescent dyes such as rhodamine 6G, NK-3483, and coumarin 120. Their emission properties are dependent on the sort of the opal and the solvents used for infiltration. With increasing optical excitation intensity, spectral narrowing and evolution of sharp lines have been observed in the green opal infiltrated with OOPPV, MDDOPPV, or rhodamine 6G but not in the infiltrated red and purple opals. With a solvent having a refractive index similar to that of SiO2, the evolution of the sharp emission lines is greatly suppressed and the lines exhibit a blueshift with decreasing refractive index. In NK-3483 and coumarin 120 which show red and purple PL, respectively, evolution of sharp lines is observed when they were infiltrated in red and purple opals, respectively, but not in other opals. These results are discussed in terms of amplified spontaneous emission and multimode lasing due to optical feedback in the opal matrix with a periodic structure.

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