Berghuis Anton Matthijs, Tichauer Ruth H, de Jong Lianne M A, Sokolovskii Ilia, Bai Ping, Ramezani Mohammad, Murai Shunsuke, Groenhof Gerrit, Gómez Rivas Jaime
Department of Applied Physics and Eindhoven Hendrik Casimir Institute, Eindhoven University of Technology, P.O. Box 513, 5600 MB Eindhoven, The Netherlands.
Nanoscience Center and Department of Chemistry, University of Jyväskylä, P.O. Box 35, 40014 Jyväskylä, Finland.
ACS Photonics. 2022 Jul 20;9(7):2263-2272. doi: 10.1021/acsphotonics.2c00007. Epub 2022 Jun 9.
Exciton transport in most organic materials is based on an incoherent hopping process between neighboring molecules. This process is very slow, setting a limit to the performance of organic optoelectronic devices. In this Article, we overcome the incoherent exciton transport by strongly coupling localized singlet excitations in a tetracene crystal to confined light modes in an array of plasmonic nanoparticles. We image the transport of the resulting exciton-polaritons in Fourier space at various distances from the excitation to directly probe their propagation length as a function of the exciton to photon fraction. Exciton-polaritons with an exciton fraction of 50% show a propagation length of 4.4 μm, which is an increase by 2 orders of magnitude compared to the singlet exciton diffusion length. This remarkable increase has been qualitatively confirmed with both finite-difference time-domain simulations and atomistic multiscale molecular dynamics simulations. Furthermore, we observe that the propagation length is modified when the dipole moment of the exciton transition is either parallel or perpendicular to the cavity field, which opens a new avenue for controlling the anisotropy of the exciton flow in organic crystals. The enhanced exciton-polariton transport reported here may contribute to the development of organic devices with lower recombination losses and improved performance.
大多数有机材料中的激子传输是基于相邻分子之间的非相干跳跃过程。这个过程非常缓慢,限制了有机光电器件的性能。在本文中,我们通过将并四苯晶体中的局域单重态激子与等离子体纳米颗粒阵列中的受限光模式强耦合,克服了非相干激子传输。我们在傅里叶空间中对从激发点起不同距离处产生的激子极化激元的传输进行成像,以直接探测它们作为激子与光子分数函数的传播长度。激子分数为50%的激子极化激元显示出4.4μm的传播长度,与单重态激子扩散长度相比增加了2个数量级。这种显著的增加已通过时域有限差分模拟和原子多尺度分子动力学模拟得到定性证实。此外,我们观察到当激子跃迁的偶极矩与腔场平行或垂直时,传播长度会发生改变,这为控制有机晶体中激子流的各向异性开辟了一条新途径。本文报道的增强的激子极化激元传输可能有助于开发具有更低复合损耗和更高性能的有机器件。