2016
DOI: 10.1063/1.4942010
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Role of the sample thickness on the performance of cholesteric liquid crystal lasers: Experimental, numerical, and analytical results

Abstract: We have studied the performance characteristics of a dye-doped cholesteric liquid crystal (CLC) laser as a function of the sample thickness. The study has been carried out both from the experimental and theoretical points of view. The theoretical model is based on the kinetic equations for the population of the excited states of the dye and for the power of light generated within the laser cavity. From the equations, the threshold pump radiation energy Eth and the slope efficiency η are numerically calculated.… Show more

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Cited by 17 publications
(8 citation statements)
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“…We finish this section by giving a link between and the threshold energy per pulse E th in order to compare the previous theoretical analysis with experimentally measurable quantities. In the case of nanosecond or picosecond pump pulses, an approximate analytical expression for E th was obtained by Sanz-Enguita et al [ 10 ] where h is Planck’s constant. This equation was deduced from the kinetic equations of the excited state populations of dyes and emitted light developed by Shtykov and Palto [ 40 ].…”
Section: Theoretical Analysis Of Different Cell Architecturesmentioning
confidence: 99%
See 1 more Smart Citation
“…We finish this section by giving a link between and the threshold energy per pulse E th in order to compare the previous theoretical analysis with experimentally measurable quantities. In the case of nanosecond or picosecond pump pulses, an approximate analytical expression for E th was obtained by Sanz-Enguita et al [ 10 ] where h is Planck’s constant. This equation was deduced from the kinetic equations of the excited state populations of dyes and emitted light developed by Shtykov and Palto [ 40 ].…”
Section: Theoretical Analysis Of Different Cell Architecturesmentioning
confidence: 99%
“…In fact, when CLCs are doped with fluorescent dyes, mirrorless laser generation can be obtained at the edges of the PBG. Since the discovery of laser emission in CLCs by Kopp et al in 1998 [ 1 ], many efforts have been made to build up CLC lasers with increasing performance and durability [ 2 , 3 , 4 , 5 , 6 , 7 , 8 , 9 , 10 , 11 , 12 , 13 , 14 , 15 , 16 ].…”
Section: Introductionmentioning
confidence: 99%
“…The dependence of lasing threshold on particle size can be attributed to changes in the resonant strength of the CLC cavity and the amount of nonquenched dye available for stimulated emission. 40,41 Analytical forms for lasing threshold originate from the laser rate equations 42 and/or density of state considerations, 41 but result in the following dependence on particle diameter: 40…”
Section: Resultsmentioning
confidence: 99%
“…The dependence of lasing threshold on particle size can be attributed to changes in the resonant strength of the CLC cavity and the amount of nonquenched dye available for stimulated emission. , Analytical forms for lasing threshold originate from the laser rate equations and/or density of state considerations, but result in the following dependence on particle diameter: E th = Ad + B / d 2 , where E th is lasing threshold, d is particle diameter, and A and B are constants. Increasing the particle size increases the number of periods of the molecular helix within the droplet, thereby enhancing coherent scattering and increasing both the amplitude of the Bragg reflectance and the efficiency of the resonant cavity, Q .…”
Section: Resultsmentioning
confidence: 99%
“…The gap region is located between pn e and pn o , where p is the pitch and n e and n o the extraordinary and ordinary refractive indices, respectively. The photonic character of CLCs is the basis for their application to build distributed feedback (DFB) lasers. These lasers are made of CLC materials doped with fluorescent dyes whose emission spectra are significantly altered by the photonic structure. , …”
mentioning
confidence: 99%