Can ΔSCFand ROKS DFT-Based Methods Predictthe Inversion of the Singlet–Triplet Gap in Organic Molecules?

Inverted singlet–triplet gap systems (INVEST) have emerged as an intriguing class of materials with potential applications as emitters in Organic Light Emitting Diodes (OLEDs). Indeed, this type of material exhibits a negative singlet–triplet energy gap (Δ<i>E</i><sub>ST</sub>), i.e., an inversion of the lowest singlet (S<sub>1</sub>) and triplet (T<sub>1</sub>) excited states, that goes against Hund’s rule. In this study, the Δ<i>E</i><sub>ST</sub> of a set of 15 INVEST molecules has been computed within the framework of Restricted Open-Shell Kohn–Sham (ROKS) and Delta Self-Consistent Field (ΔSCF) methods and the results were benchmarked against wavefunction-based calculations performed at the EOM-CCSD, NEVPT2, and SCS-CC2 levels. We find that ROKS always (and wrongly) predicts a positive Δ<i>E</i><sub>ST</sub> with global hybrid, meta-GGA, and long-range corrected functionals and that this is almost functional-independent. We also show that the only way to obtain an inverted gap was to resort to double hybrid functionals. In contrast, using the above-mentioned functionals, ΔSCF usually gives a negative Δ<i>E</i><sub>ST</sub>, although the results are largely functional-dependent. Overall, applying a ΔSCF method based on the PBE0 functional provides the lowest MSD and MAD with respect to the EOM-CCSD results. We further show that the singlet–triplet inversion is driven by different degrees of orbital relaxation in the singlet versus triplet state and that this is well captured by ΔSCF calculations. As a matter of fact, this orbital relaxation in ΔSCF somehow mimics the involvement of double and higher-order excitations in EOM-CCSD, which leads to a difference in spatial localization of the α and β spins, and thus introduces (local) spin polarization effects sourcing the negative Δ<i>E</i><sub>ST</sub>. However, care should be taken when using the ΔSCF method to screen materials with potential INVEST behavior in view of their limited quantitative correlation with reference EOM-CCSD results on the molecular data basis used here.

Publication Details

Journal
Figshare
Published
2025-03-01
DOI
https://doi.org/10.1021/acs.jctc.4c01600.s001
Primary Topic
Synthesis and Properties of Aromatic Compounds
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article
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article

Can ΔSCFand ROKS DFT-Based Methods Predictthe Inversion of the Singlet–Triplet Gap in Organic Molecules?

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Synthesis and Properties of Aromatic Compounds
article

Can ΔSCFand ROKS DFT-Based Methods Predictthe Inversion of the Singlet–Triplet Gap in Organic Molecules?

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Abstract

Inverted singlet–triplet gap systems (INVEST) have emerged as an intriguing class of materials with potential applications as emitters in Organic Light Emitting Diodes (OLEDs). Indeed, this type of material exhibits a negative singlet–triplet energy gap (Δ<i>E</i><sub>ST</sub>), i.e., an inversion of the lowest singlet (S<sub>1</sub>) and triplet (T<sub>1</sub>) excited states, that goes against Hund’s rule. In this study, the Δ<i>E</i><sub>ST</sub> of a set of 15 INVEST molecules has been computed within the framework of Restricted Open-Shell Kohn–Sham (ROKS) and Delta Self-Consistent Field (ΔSCF) methods and the results were benchmarked against wavefunction-based calculations performed at the EOM-CCSD, NEVPT2, and SCS-CC2 levels. We find that ROKS always (and wrongly) predicts a positive Δ<i>E</i><sub>ST</sub> with global hybrid, meta-GGA, and long-range corrected functionals and that this is almost functional-independent. We also show that the only way to obtain an inverted gap was to resort to double hybrid functionals. In contrast, using the above-mentioned functionals, ΔSCF usually gives a negative Δ<i>E</i><sub>ST</sub>, although the results are largely functional-dependent. Overall, applying a ΔSCF method based on the PBE0 functional provides the lowest MSD and MAD with respect to the EOM-CCSD results. We further show that the singlet–triplet inversion is driven by different degrees of orbital relaxation in the singlet versus triplet state and that this is well captured by ΔSCF calculations. As a matter of fact, this orbital relaxation in ΔSCF somehow mimics the involvement of double and higher-order excitations in EOM-CCSD, which leads to a difference in spatial localization of the α and β spins, and thus introduces (local) spin polarization effects sourcing the negative Δ<i>E</i><sub>ST</sub>. However, care should be taken when using the ΔSCF method to screen materials with potential INVEST behavior in view of their limited quantitative correlation with reference EOM-CCSD results on the molecular data basis used here.

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Synthesis and Properties of Aromatic Compounds
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