4.6 Article

Triplet Exciton Diffusion and Quenching in Matrix-Free Solid Photon Upconversion Films

Journal

JOURNAL OF PHYSICAL CHEMISTRY C
Volume 125, Issue 7, Pages 3764-3775

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.jpcc.0c11048

Keywords

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Funding

  1. Research Council of Lithuania (LMTLT) [S-MIP-17-77]
  2. EU
  3. German Science Foundation (DFG) [GRK1640]

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In this study, the diffusion and quenching of triplet excitons in solid state upconversion films based on two different BFA emitters and PtOEP sensitizer were investigated. It was found that the BFA-Ph film exhibited faster triplet exciton quenching rate, leading to optimal UC performance at lower temperatures than the BFA-Me film.
Efficient triplet exciton hopping (diffusion) in amorphous solid films is essential for triplet-triplet annihilation (TTA) and TTA-mediated photon upconversion (UC) at low excitation power densities. However, enhanced triplet diffusion, particularly in high-emitter-content UC films, also facilitates their trapping and quenching at nonradiative decay sites, thus deteriorating UC efficiency. In this work, triplet exciton diffusion and quenching are studied in matrix-free solid UC films based on two novel bisfluorene-anthracene (BFA) emitters, i.e., one with methyl substitution (BFA-Me) and the other with a phenyl substitution (BFA-Ph), and a standard platinum octaethylporphyrin (PtOEP) sensitizer. By analyzing temperature-dependent TTA-UC dynamics and accounting for various singlet exciton-related processes, we are able to discern triplet exciton quenching occurring explicitly in the emitter and show that it is one of the dominating mechanisms impeding the UC performance of BFA/PtOEP films, particularly at elevated temperatures. Regardless of the lower density of quenchers present in the BFA-Ph film, twice as large triplet diffusivity estimated in this film (D = (2.13 +/- 0.64) x 10(-9) cm(2).s(-1)) at room temperature as compared to that in the BFA-Me film caused more rapid triplet quenching. This resulted in the shifting of the optimal UC performance of BFA-Ph to lower temperatures (T = 160 K) with respect to that of BFA-Me (T = 220 K). To obtain a high UC quantum yield, which for these materials can be estimated to reach >5% at room temperature and above, the excessive diffusion to the remaining quenching sites needs to be suppressed, e.g., by increasing the intermolecular distance through side groups.

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