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The Role of the Lowest Excited Triplet State in Defining the Rate of Photoaquation of Hexacyanometalates.

ABSTRACT: Photosolvation is a type of ligand substitution reaction started by irradiation of a solution with light, triggering the replacement of a ligand with a molecule from the solvent. The excited state is created through many possible pathways. For the class of hexacyanides of groups 8 and 9 of the periodic table, irradiation in the ligand field band is followed by intersystem crossing to the lowest excited triplet state, which we propose to mediate the photoaquation reaction in this class of complexes. In this study, we present time-resolved X-ray absorption data showing indications of the triplet intermediate state in the cobalt(III) hexacyanide complex and we discuss general aspects of the photoaquation reaction in comparison with reported data on the isoelectronic iron(II) hexacyanide. Quantum chemical calculations are analyzed and suggest that the nature of the lowest excited triplet state in each complex can explain the drastically different rate of reactions observed.

SUBMITTER: Mascarenhas EJ

PROVIDER: S-EPMC10788954 | biostudies-literature | 2024 Jan

REPOSITORIES: biostudies-literature

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The Role of the Lowest Excited Triplet State in Defining the Rate of Photoaquation of Hexacyanometalates.

Mascarenhas Eric J EJ Fondell Mattis M Büchner Robby R Eckert Sebastian S Vaz da Cruz Vinicius V Föhlisch Alexander A

The journal of physical chemistry letters 20240102 1

Photosolvation is a type of ligand substitution reaction started by irradiation of a solution with light, triggering the replacement of a ligand with a molecule from the solvent. The excited state is created through many possible pathways. For the class of hexacyanides of groups 8 and 9 of the periodic table, irradiation in the ligand field band is followed by intersystem crossing to the lowest excited triplet state, which we propose to mediate the photoaquation reaction in this class of complex ...[more]

PMID: 38164541

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Project description:A family of complexes of the type [Ru(tpbn)(IP-R)(4-pic)]Cl2 (tbpn=2,2'-(4-(tert-butyl)pyridine-2,6-diyl)bis(1,8-napthyridine); 4-pic=4-picoline; IP-R=imidazo[4,5-f][1,10]phenanthroline attached to an aromatic group R for 2-8 and H for 1) were prepared as near-infrared (NIR) absorbing coordination complexes to test whether triplet intraligand excited states (3IL) of higher energy than the lowest-lying triplet metal-to-ligand charge transfer excited states (3MLCT) could effectively generate cytotoxic singlet oxygen (1O2) and elicit in vitro photodynamic therapy (PDT) effects. Aromatic groups ranged from benzene to anthracene, with corresponding triplet state energies that were all significantly higher (approximately 3.7-1.8 eV) than the 3MLCT state estimated at 1.5 eV. Complexes 1-8 absorbed NIR light, with their longest-wavelength peak maxima occurring near 725 nm that extended out to 800 nm. The 1O2 quantum yields for the aromatic-containing compounds were extremely small (ΦΔ=0.07), with correspondingly modest in vitro photocytotoxicities. All compounds were nontoxic without a light trigger, with dark EC50 values >60 μM and most values closer to 100 or greater. EC50 values with visible light were 5-6 (PI=15-20), 7-10 (PI=8-11), and 10-15 μM (PI=6-8) in SKMEL28, A375, and B16F10 cancer cell lines, respectively. With NIR light, these values were even less: 11-16 (PI=5-9), 16-50 (PI=2-6), and 15-19 μM (PI=4-6) in SKMEL28, A375, and B16F10 cancer cell lines, respectively. While measurable, the modest activities and absence of any trend between the 3IL energies and values for ΦΔ or PI demonstrate that 3IL states with energies above the lowest-lying 3MLCT states do not contribute to the overall excited state dynamics responsible for potent PDT effects in previous studies. Lowest-lying 3MLCT states in this family of NIR-absorbing photosensitizers do not produce the requisite 1O2 for effective in vitro photocytotoxic effects, underscoring the need to install 3IL states that are lower in energy than the lowest-lying 3MLCT states in order the create potent NIR-activatable Ru(II) complexes for PDT.

Project description:The structure of 30 monosubstituted benzenes in the first excited triplet T1 state was optimized with both unrestricted (U) and restricted open shell (RO) approximations combined with the ωB97XD/aug-cc-pVTZ basis method. The substituents exhibited diverse σ- and π-electron-donating and/or -withdrawing groups. Two different positions of the substituents are observed in the studied compounds in the T1 state: one distorted from the plane and the other coplanar with a quinoidal ring. The majority of the substituents are π-electron donating in the first group while π-electron withdrawing in the second one. Basically, U- and RO-ωB97XD approximations yield concordant results except for the B-substituents and a few of the planar groups. In the T1 state, the studied molecules are not aromatic, yet aromaticity estimated using the HOMA (harmonic oscillator model of aromaticity) index increases from ca. -0.2 to ca. 0.4 with substituent distortion, while in the S1 state, they are only slightly less aromatic than in the ground state (HOMA ≈0.8 vs ≈1.0, respectively). Unexpectedly, the sEDA(T1) and pEDA(T1) substituent effect descriptors do not correlate with analogous parameters for the ground and first excited singlet states. This is because in the T1 state, the geometry of the ring changes dramatically and the sEDA(T1) and pEDA(T1) descriptors do not characterize only the functional group but the entire molecule. Thus, they cannot provide useful scales for the substituents in the T1 states. We found that the spin density in the T1 states is accumulated at the Cipso and Cp atoms, and with the substituent deformation angle, it nonlinearly increases at the former while decreases at the latter. It appeared that the gap between singly unoccupied molecular orbital and singly occupied molecular orbital (SUMO-SOMO) is determined by the change of the SOMO energy because the former is essentially constant. For the nonplanar structures, SOMO correlates with the torsion angle of the substituent and the ground-state pEDA(S0) descriptor of the π-electron-donating substituents ranging from 0.02 to 0.2 e. Finally, shapes of the SOMO-1 instead of SOMO frontier orbitals in the T1 state somehow resemble the highest occupied molecular orbital ones of the S0 and S1 states. For several planar systems, the shape of the U- and RO-density functional theory-calculated SOMO-1 orbitals differs substantially.

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The Role of the Lowest Excited Triplet State in Defining the Rate of Photoaquation of Hexacyanometalates.

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The Role of the Lowest Excited Triplet State in Defining the Rate of Photoaquation of Hexacyanometalates.

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