Modeling MR-TADF Emitters: Excited-State Decay Rate Constants and Wave Function Descriptors
Mariana T. do Casal, Youssef Badawy, Daniel Escudero
Abstract
Multiresonance thermally activated delayed fluorescence (MR-TADF) emitters have gained popularity given their potential of attaining negligible singlet–triplet energy gaps, i.e., Δ E ST, without hindering emission, thus increasing the reverse and direct intersystem crossing rates without affecting fluorescence. This is achieved due to the singlet and triplet states’ short-range charge transfer character (SRCT). Thus, obtaining quantitative information about SRCT would help develop new MR-TADF emitters. This work studies three different families of MR-TADF emitters: DOBOA, DiKTa, and OQAO. First, we compute their adiabatic Δ E ST with four different methods (TDA-CAM-B3LYP, STEOM-DLPNO-CCSD, ADC(2), and SCS-CC2). Then, we compute fluorescence ( k r ), direct ( k ISC ), and reverse intersystem crossing rate constants. For k r, we assessed the effect of different levels of approximations on the rate calculations. We show that k r does not depend significantly on the different harmonic models (adiabatic Hessian or vertical Hessian), coordinate systems, and broadening widths. Moreover, Herzberg–Teller effects are negligible for k r but are the main contribution for k ISC and k RISC . The computed rate constants agree well with the experimental results. Moreover, we propose the use of two wave function descriptors, Q a t and LOC a, based on the 1-particle transition density matrix, which assigns the amount of charge centered on the atoms. We compute these descriptors for three transitions: S 0 → S 1, S 0 → T 1, and S 1 → T 1 . For the studied cases, these descriptors are independent of the choice of the electronic structure method and optimal geometry. We show that the adiabatic Δ E ST decreases with the increase of S 1 → T 1 Q a t, while Δ E ST increases with an increase of the S 0 → T 1 Q a t . These trends showcase how the Q a t values can act as guiding descriptors to design new MR-TADF emitters with small Δ E ST values.