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Intrachain Photoluminescence Dynamics of MEH-PPV in the Solid State

机译:固态MEH-PPV的链内光致发光动力学

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The photoluminescence(PL)dynamics of poly[2-methoxy-5-(2'-ethyl-hexyloxy)-1,4-phenylene vinylene](MEH-PPV)blended in host polymer(polypropylene,PP)matrix as well as that in the neat film has been studied.The concentration of MEH-PPV in the PP blend is designed to be fairly low(0.01 wt %)in order to observe the intrinsic intrachain PL property of MEH-PPV in the solid state.The steady-state 0-0 PL band of the blend sample shows a blue-shift of 0.12 eV with respect to that of the neat film of MEH-PPV.The PL-excitation(PLE)spectra of the blend sample exhibit definite vibronic structure,and hence we can determine the magnitude of the Stokes shift as 0.06 eV.The blend sample shows a single-exponential PL decay at 4 K with a time constant of 850 ps.We emphasize that this single-exponential-type PL decay is an intrinsic property of the intrachain PL species.Time-resolved PL measurements confirm dynamical red-shift of the PL band in the neat film,whereas this trend is not found in the case of the PP blend.These observations indicate that the energy transfer between finite segments,which can cause exciton migration,is much less efficient within the isolated MEH-PPV polymer chain compared to the case of the interchain transfer.The time-resolved measurements further demonstrate that the Stokes shift identified in the blend sample takes place at the early stage within 50 ps following photoexcitation.We attribute this Stokes shift to the rapid increase of the planarity of the MEH-PPV chain caused by the torsion of some constituent phenyl rings following photoexcitation.Finally,based on an argument on the different magnitudes of Stokes shift between the blend sample and the neat film,we conclude that the PL of MEH-PPV in the neat film predominantly occurs at the site of interchain excitations via the interchain migration of excitons.
机译:聚[2-甲氧基-5-(2'-乙基-己氧基)-1,4-亚苯基亚乙烯基](MEH-PPV)共混在主体聚合物(聚丙烯,PP)基质中的光致发光(PL)动力学为了观察MEH-PPV在固态下的固有链内PL特性,将PP共混物中的MEH-PPV浓度设计得相当低(0.01 wt%)。混合样品的0-0状态PL带相对于MEH-PPV纯膜的蓝移显示0.12 eV的蓝移。混合样品的PL激发(PLE)光谱表现出确定的振动结构,因此我们可以确定斯托克斯频移的大小为0.06 eV。混合样本显示了在4 K时的单指数PL衰减,时间常数为850 ps。我们强调这种单指数型PL衰减是时间分辨的PL测量结果证实了纯膜中PL带的动态红移,而在t的情况下没有发现这种趋势这些观察结果表明,与链间转移相比,在分离的MEH-PPV聚合物链中有限段之间的能量转移(可能引起激子迁移)效率低得多。时间分辨的测量结果进一步表明:共混样品中识别出的斯托克斯位移发生在光激发后的50 ps内的早期阶段。我们将此斯托克斯位移归因于光激发后某些组成苯环的扭曲引起的MEH-PPV链平面度的快速增加。最后,基于混合样品与纯膜之间斯托克斯位移的大小不同的观点,我们得出结论:纯膜中MEH-PPV的PL主要通过激子的链间迁移发生在链间激发的位置。

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