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解析多模卟啉腔极化激元样品中增强发光与吸收之间的差异。

Deciphering between enhanced light emission and absorption in multi-mode porphyrin cavity polariton samples.

作者信息

Odewale Elizabeth O, Avramenko Aleksandr G, Rury Aaron S

机构信息

Materials Structural Dynamics Laboratory, Department of Chemistry, Wayne State University, 48202, Detroit, MI, USA.

出版信息

Nanophotonics. 2024 Mar 15;13(14):2695-2706. doi: 10.1515/nanoph-2023-0748. eCollection 2024 Jun.

Abstract

It remains unclear how the collective strong coupling of cavity-confined photons to the electronic transitions of molecular chromophore leverages the distinct properties of the polaritonic constituents for future technologies. In this study, we design, fabricate, and characterize multiple types of Fabry-Pérot (FP) mirco-resonators containing copper(II) tetraphenyl porphyrin (CuTPP) to show how cavity polariton formation affects radiative relaxation processes in the presence of substantial non-Condon vibronic coupling between two of this molecule's excited electronic states. Unlike the prototypical enhancement of Q state radiative relaxation of CuTPP in a FP resonator incapable of forming polaritons, we find the light emission processes in multimode cavity polariton samples become enhanced for cavity-exciton energy differences near those of vibrations known to mediate non-Condon vibronic coupling. We propose the value of this detuning is consistent with radiative relaxation of Herzberg-Teller polaritons into collective molecular states coupled to the cavity photon coherently. We contrast the feature stemming from light emission from the HT polariton state with those that occur due to polariton-enhanced light absorption. Our results demonstrate the landscape of molecular and photonic interactions enabled by cavity polariton formation using complex chromophores and how researchers can design resonators to leverage these interactions to characterize and control polaritonic properties.

摘要

目前尚不清楚腔受限光子与分子发色团的电子跃迁之间的集体强耦合如何利用极化激元成分的独特性质来服务于未来技术。在本研究中,我们设计、制造并表征了多种包含四苯基卟啉铜(CuTPP)的法布里 - 珀罗(FP)微谐振器,以展示在该分子的两个激发电子态之间存在大量非康登振动耦合的情况下,腔极化激元的形成如何影响辐射弛豫过程。与在无法形成极化激元的FP谐振器中CuTPP的Q态辐射弛豫的典型增强不同,我们发现对于腔 - 激子能量差接近已知介导非康登振动耦合的振动能量差的多模腔极化激元样品,其发光过程会增强。我们提出这种失谐值与赫兹伯格 - 泰勒极化激元向与腔光子相干耦合的集体分子态的辐射弛豫是一致的。我们将来自HT极化激元态的发光特征与极化激元增强光吸收所产生的特征进行了对比。我们的结果展示了使用复杂发色团通过腔极化激元形成实现的分子与光子相互作用的全貌,以及研究人员如何设计谐振器来利用这些相互作用来表征和控制极化激元性质。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e06c/11636455/491d5e7d1c96/j_nanoph-2023-0748_fig_001.jpg

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