2014
DOI: 10.1142/s0218863514500180
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Optical bistable switching in pyran dye-doped polymers

Abstract: In the present frame of work, optical bistability using a Fabry–Perot (FP) cavity containing 4-dicyanomethylene-2-methyl-6-p-dimethylaminostyryl-4H-pyran (DCM) dye entrapped in poly-methylmethacrylate (PMMA) matrix is experimentally investigated. Optical nonlinear behavior of solid-state samples is studied using a single-mode Q-switched nanosecond Nd:YAG laser operating at 532 nm. Various optical nonlinear parameters such as nonlinear refractive index (n2) and third-order susceptibility (χ3) of the material ar… Show more

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Cited by 3 publications
(1 citation statement)
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“…[1][2][3][4][5] Optical waveguide devices [6][7][8] have attracted a lot of research interest recently, not only because of their small device sizes, but also because of the possibility of achieving recon¯gurable functionality as well as large scale integration. Purnima and Mohan reported 9 the optical switching on the basis of optical bistability phenomenon with the change in input laser intensity. The nonlinear refraction coe±cient (n 2 Þ of order of 10 À9 cm 2 /W and third-order susceptibility ( 3 Þ of order of 10 À15 m 2 /V 2 could con¯rm the occurrence of strong third-order optical nonlinearity in dye-doped polymers.…”
Section: Introductionmentioning
confidence: 99%
“…[1][2][3][4][5] Optical waveguide devices [6][7][8] have attracted a lot of research interest recently, not only because of their small device sizes, but also because of the possibility of achieving recon¯gurable functionality as well as large scale integration. Purnima and Mohan reported 9 the optical switching on the basis of optical bistability phenomenon with the change in input laser intensity. The nonlinear refraction coe±cient (n 2 Þ of order of 10 À9 cm 2 /W and third-order susceptibility ( 3 Þ of order of 10 À15 m 2 /V 2 could con¯rm the occurrence of strong third-order optical nonlinearity in dye-doped polymers.…”
Section: Introductionmentioning
confidence: 99%