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Organic lasers use an organic material as the gain medium. The first organic laser was the liquid dye laser.〔P. P. Sorokin and J. R. Lankard, Stimulated emission observed from an organic dye, chloro-aluminum phthalocyanine, ''IBM J. Res. Dev.'' 10, 162-163 (1966).〕〔F. P. Schäfer, W. Schmidt, and J. Volze, Organic dye solution laser, ''Appl. Phys. Lett.'' 9, 306-309 (1966).〕 These lasers use laser dye solutions as their gain media. Solid-state dye lasers are organic tunable lasers that use laser dye-doped polymers (DDP),〔B. H. Soffer and B. B. McFarland, Continuously tunable narrow-band organic dye lasers, ''Appl. Phys. Lett.'' 10, 266-267 (1967).〕 dye-doped ormosil (DDO),〔B. S. Dunn, J. D. Mackenzie, J. I. Zink, and O. M. Stafsudd, Solid-state tunable lasers based on dye-doped sol-gel materials, ''Proc. SPIE'' 1328, 174-182 (1990).〕 and dye-doped polymer-nanoparticle (DDPN)〔F. J. Duarte and R. O. James, Tunable solid-state lasers incorporating dye-doped polymer-nanoparticle gain media, ''Opt. Lett.'' 28, 2088-2090 (2003).〕 gain media. DDO and DDPN gain media are subsets of a larger class of organic-inorganic hybrid materials used as laser matrices.〔A. Costela, I. Garcia-Moreno, R. Sastre, Solid-state dye lasers, in ''Tunable Laser Applications'', 2nd Edition, F. J. Duarte, Ed. (CRC, New York, 2009) Chapter 3.〕〔A. Costela, L. Cerdan, I. García-Moreno, Solid-state dye lasers with scattering feedback, ''Prog. Quantum Electron.'' 37, 348-382 (2013).〕 Other types of solid-state organic lasers include the organic semiconductor lasers that use conjugated polymers as gain media.〔I. D. W. Samuel and G. A. Turnbull, Organic semiconductor lasers, ''Chem. Rev.'' 107, 1272-1295 (2007).〕〔C. Karnutsch, ''Low Threshold Organic Thin Film Laser Devices'' (Cuvillier, Göttingen, 2007).〕 These semiconductor materials can also be configured as "neat films."〔A. K. Bansal and A. Penzkofer, Linear and nonlinear optical spectroscopic characterization of 1,2,3-tris(3-methylphenylphenylamino) benzene, ''Chem. Phys.'' 352, 48-56 (2008).〕 Organic lasers are inherently tunable and when configured as optimized multiple-prism grating laser oscillators can yield efficient single-transverse mode, and single-longitudinal-mode, emission with laser linewidths as narrow as 350 MHz (approximately 0.0004 nm at a wavelength of 590 nm), in the high-power pulsed regime.〔F. J. Duarte, Multiple-prism grating solid-state dye laser oscillator: optimized architecture, ''Appl. Opt.'' 38, 6347-6349 (1999).〕 Organic lasers are also available in distributed feedback configurations〔W. J. Wadsworth, I. T. McKinnie, A. D. Woolhouse, T. G. Haskell, Efficient distributed feedback solid state dye laser with a dynamic grating, ''Appl. Phys. B'' 69, 163–169 (1999).〕 〔X-L. Zhu, S-K. Lam, D. Lo, Distributed-feedback dye-doped solgel silica lasers, ''Appl. Opt.'' 39, 3104–3107 (2000).〕 and distributed feedback waveguides.〔Y. Oki, S. Miyamoto, M. Tanaka, D. Zuo, M. Maeda, Long lifetime and high repetition rate operation from distributed feedback plastic waveguided dye lasers, ''Opt. Commun.'' 214, 277–283 (2002).〕 ==See also== *Dye lasers *Organic photonics *Organic semiconductors *Polymers *Nanoparticle *Solid-state dye lasers 抄文引用元・出典: フリー百科事典『 ウィキペディア（Wikipedia）』 ■ウィキペディアで「Organic laser」の詳細全文を読む スポンサード リンク
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