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. 2020 Feb 26;142(8):3753-3761.
doi: 10.1021/jacs.9b10371. Epub 2020 Feb 18.

S = 3 Ground State for a Tetranuclear MnIV4O4 Complex Mimicking the S3 State of the Oxygen-Evolving Complex

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S = 3 Ground State for a Tetranuclear MnIV4O4 Complex Mimicking the S3 State of the Oxygen-Evolving Complex

Heui Beom Lee et al. J Am Chem Soc. .

Abstract

The S3 state is currently the last observable intermediate prior to O-O bond formation at the oxygen-evolving complex (OEC) of Photosystem II, and its electronic structure has been assigned to a homovalent MnIV4 core with an S = 3 ground state. While structural interpretations based on the EPR spectroscopic features of the S3 state provide valuable mechanistic insight, corresponding synthetic and spectroscopic studies on tetranuclear complexes mirroring the Mn oxidation states of the S3 state remain rare. Herein, we report the synthesis and characterization by XAS and multifrequency EPR spectroscopy of a MnIV4O4 cuboidal complex as a spectroscopic model of the S3 state. Results show that this MnIV4O4 complex has an S = 3 ground state with isotropic 55Mn hyperfine coupling constants of -75, -88, -91, and 66 MHz. These parameters are consistent with an αααβ spin topology approaching the trimer-monomer magnetic coupling model of pseudo-octahedral MnIV centers. Importantly, the spin ground state changes from S = 1/2 to S = 3 as the OEC is oxidized from the S2 state to the S3 state. This same spin state change is observed following oxidation of the previously reported MnIIIMnIV3O4 cuboidal complex to the MnIV4O4 complex described here. This sets a synthetic precedent for the observed low-spin to high-spin conversion in the OEC.

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Conflict of interest statement

The authors declare no competing financial interest.

Figures

Figure 1.
Figure 1.
a) Proposed isomers S3A and S3B of the inorganic CaMn4O5(OH) core of the S3 state of the OEC. b) Representative examples of MnIV4 complexes and their corresponding spin ground states.
Figure 2.
Figure 2.
Mn K-edge XAS spectra for complexes 2 (black lines) and 3 (red dotted lines). a) Normalized XANES data, b) k3-weighted EXAFS data, and c) Fourier transforms of k3-weighted EXAFS data.
Figure 3.
Figure 3.
D-band EPR spectrum of complex 3 collected at 1.6 K. Spectral data are shown in black and the simulated spectrum is represented by the dashed red line and other colored traces. The simulated Mn(II) contribution is shown in light blue and the mS transitions that contribute to the complex 3 simulation are shown in blue, purple, and orange. Simulation parameters: S = 3, g = 1.97, D = 0.4 cm−1, E/D = 0.1. (Inset) Electron-spin nutation curves of complex 3 (blue) collected at 7 T and BDPA (black).
Figure 4.
Figure 4.
Parallel mode X-band CW-EPR of complex 3. Spectral data are shown in black and the simulated spectrum is represented by the dashed red line. Simulation parameters: S = 3, g = 1.97, D = 0.4 cm−1, E/D = 0.1.
Figure 5.
Figure 5.
(Left) EPR spectrum of 3 showing the field positions (*) where EDNMR spectra were collected. (Right) Field dependent EDNMR of 3. Experimental data are shown in black traces. Spectral simulations are shown in the colored traces. The simulated hyperfine values are listed in Table 1.
Scheme 1.
Scheme 1.
Synthesis of complexes 1~3 studied in this work.

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