首页> 外文期刊>Journal of the Optical Society of America, B. Optical Physics >Emission of R6G dye in Fabry-Perot cavities in weak and strong coupling regimes
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Emission of R6G dye in Fabry-Perot cavities in weak and strong coupling regimes

机译:在弱和强耦合制度中的法布里 - 珀罗腔中R6G染料的排放

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We have studied spectra and angular distribution of emission in Fabry-Perot cavities formed by two silver mirrors separated by a layer of poly (methyl methacrylate) polymer doped with rhodamine 6G (R6G) dye in low (20 g/l) and high (200 g/l) concentrations. The frequency of emission radiated to a cavity mode was larger at large outcoupling angles-the "rainbow" effect. At the same time, the angle of the strongest emission was also determined by the cavity size: the larger the cavity, the larger the angle. The angular distribution of emission is commonly dominated by two symmetrical lobes (located at the intersection of the three-dimensional emission cone with a horizontal plane) pointing to the left and to the right of the normal to the sample. Despite the strong Stokes shift in R6G dye, the branch of the cavity dispersion curve obtained in the emission experiment is positioned above the one obtained in the reflection (extinction) experiment. Some dye molecules are poorly coupled to cavity modes. Their emission has very broad angular distribution with the maximum at theta = 0 degrees. The signatures of strong cavity-exciton coupling were observed at high dye concentration (200 g/l) but not at low concentration (20 g/l). The evidence of the effect of strong coupling on emission is exemplified by a strong difference in the angular distribution of emission in two almost identical cavities, one with and another without strong coupling. Most importantly, we have demonstrated the possibility to control the ground state concentration, the coupling strength, and the dye emission spectra with Q-switched laser pulses. (C) 2020 Optical Society of America.
机译:我们研究了在低(20 g/l)和高(200 g/l)浓度下,由一层掺杂罗丹明6G(R6G)染料的聚甲基丙烯酸甲酯聚合物隔开的两个银镜形成的法布里-珀罗腔中的光谱和发射角分布。在较大的外耦合角下,辐射到腔模的发射频率更高,即“彩虹”效应。同时,发射最强的角度也取决于空腔的大小:空腔越大,发射角度越大。发射的角分布通常由两个对称的波瓣(位于三维发射锥与水平面的交点处)控制,指向样品法线的左侧和右侧。尽管R6G染料中存在强烈的斯托克斯位移,但在发射实验中获得的腔色散曲线的分支位于反射(消光)实验中获得的分支之上。一些染料分子与腔模耦合不良。它们的发射具有非常广泛的角分布,最大值为θ=0度。在高染料浓度(200 g/l)下观察到强腔激子耦合的特征,但在低浓度(20 g/l)下没有观察到。在两个几乎相同的腔体中,一个有强耦合,另一个没有强耦合,发射的角分布有很大的差异,这就证明了强耦合对发射的影响。最重要的是,我们已经证明了用调Q激光脉冲控制基态浓度、耦合强度和染料发射光谱的可能性。(C) 2020年美国光学学会。

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