The S2S_2 state of the oxygen-evolving complex (OEC), the Mn4_4CaO5_5 cluster that catalyzes photosynthetic water oxidation in photosystem II, remains the most intensively studied intermediate of the Kok cycle, yet a single electronic-structural model that quantitatively reproduces its complete spectroscopic fingerprint does not exist. A 2018 computational study of low-oxidation-paradigm (LOP) models found that Mn(II)-containing formulations fit the geometric constraints but fail the ligand (17^{17}O, 14^{14}N, 1^1H) hyperfine data, reproduce only part of the 55^{55}Mn ENDOR pattern, and cannot explain how the S=1/2S=1/2 multiline and S=5/2S=5/2 g≈4.1g\approx 4.1 EPR signals could arise from the same oxidation pattern if Mn(II) were present. Later experiments — flash-counting during photoassembly, Mn Kα\alpha X-ray emission spectroscopy, and high-energy-resolution fluorescence-detected X-ray absorption spectroscopy — strongly favor the high-oxidation assignment Mn(III)Mn(IV)3_3 for S2S_2, but the interpretation of the X-ray free-electron laser structures remains contested, a minority low-oxidation program is still active through 2025–2026, and the source paper's specific unresolved items (the two anomalously small 55^{55}Mn ENDOR couplings near 45 MHz and 7 MHz, the untested ENDOR-invisibility hypothesis, and EPR-parameter computation with explicit zero-field splitting and spin-orbit coupling) have not been taken up by any published study. The problem posed here is to determine the oxidation, protonation, and spin-coupling assignment of the S2S_2 state that quantitatively reproduces the full fingerprint, and thereby to adjudicate the residual low-oxidation claims.

Background

In oxygenic photosynthesis, photosystem II (PSII) oxidizes water to dioxygen at the oxygen-evolving complex (OEC), an inorganic Mn4_4CaO5_5 cluster ligated by amino acid residues and waters. The cluster advances through the five oxidation states S0S_0–S4S_4 of the Kok cycle, storing oxidizing equivalents until O2_2 is released on the S4→S0S_4\to S_0 transition. The one-electron-oxidized S2S_2 state is the best characterized intermediate and exhibits two EPR (electron paramagnetic resonance) signals: a multiline signal (MLS) of about 16–19 partially resolved 55^{55}Mn hyperfine lines centered at g≈2g\approx 2, assigned to a total spin S=1/2S=1/2 ground state, and a broad signal at g≈4.1g\approx 4.1 assigned to an S=5/2S=5/2 state; the two signals interconvert under near-infrared illumination, temperature, and chemical perturbations, indicating two forms of the same oxidation level in equilibrium.

Hyperfine couplings — the magnetic interactions between the electron spin and nearby nuclear spins — are the most site-specific observables available. Electron nuclear double resonance (ENDOR) resolves them for individual nuclei: the four 55^{55}Mn ions, the 14^{14}N of the histidine ligand His332, 17^{17}O-labeled oxo bridges and substrate waters, and exchangeable protons. The isotropic component AisoA_{iso} (Fermi contact) and the anisotropic dipolar part together constrain the oxidation state and spin density at each metal and ligand site.

Two competing paradigms assign the manganese oxidation states. The high-oxidation paradigm (HOP) assigns S2S_2 as one Mn(III) plus three Mn(IV) ions, and explains the two EPR signals by two interconvertible geometric isomers of this same oxidation level — the closed-cubane and open-cubane forms, differing in whether the dangling Mn approaches the cubane oxo O5 (Pantazis et al., 2012). The low-oxidation paradigm (LOP) posits two additional electrons on the cluster, lowering the mean Mn oxidation to 3.25 instead of 3.75 (for example the Mn(II)-free Mn(III)3_3Mn(IV) or the Mn(II)-containing Mn(II)Mn(III)Mn(IV)2_2); this program is grounded in computational chemistry and magnetic resonance analysis (Terrett et al., 2016; Jin et al., 2014). The 55^{55}Mn Davies ENDOR (a pulsed ENDOR sequence) study at 2.5 K by Jin et al. (2014) reported a hyperfine pattern including two anomalously small couplings (approximately 45 MHz and 7 MHz) alongside larger couplings — a feature that any candidate electronic structure must explain.

Chen, Case, and Dismukes (2018) performed the most detailed computational test of LOP S2S_2 models, using broken-symmetry density functional theory (BS-DFT — DFT solutions with spin-localized, antiferromagnetically coupled metal centers) combined with spin-projection techniques to compute EPR and ENDOR parameters. They found LOP geometries consistent with X-ray diffraction and EXAFS (extended X-ray absorption fine structure) at accessible energies, but severe spectroscopic failures: all LOP models gave overly large 17^{17}O AisoA_{iso} for the oxo bridges O5/O4 (up to −221.4-221.4 MHz) and large 14^{14}N AisoA_{iso} for His332 (−10.4-10.4 to −17.4-17.4 MHz versus the experimental ∣6.95∣|6.95| MHz); the Mn(II)-containing isomer reproduced the large and intermediate 55^{55}Mn couplings but not the two small ones, which the authors speculated might arise from a Mn(IV) ion rendered ENDOR-invisible at 2.5 K by very slow nuclear relaxation — an untested hypothesis. The computed hyperfine projections relied on the strong-exchange limit, in which the cluster's local spins are rigidly projected onto the total spin; this neglects the zero-field splitting (ZFS, the splitting of a spin multiplet in zero field caused by spin-orbit coupling and anisotropic exchange) and is invalid when exchange couplings JJ are small (∣J∣<75|J|<75 cm−1^{-1}). A large empirical scaling factor (1.53) applied to the Mn isotropic hyperfine couplings added systematic uncertainty. The paper thus left open whether any low-oxidation formulation can be reconciled with the complete spectroscopic fingerprint, and what electronic structure actually produces it.

After 2018, three independent experimental lines bore directly on the oxidation inventory: flash-counting during photoactivation (light-driven assembly of the cluster from Mn2+^{2+}) required nine flashes for the first O2_2, supporting the HOP inventory (Cheah et al., 2020); room-temperature Mn Kα\alpha X-ray emission spectroscopy showed Mn-centered oxidation in the observable S-state transitions up to S3S_3, excluding Mn reduction at the cluster (Schuth et al., 2018); and high-energy-resolution fluorescence-detected X-ray absorption spectroscopy of all S-states established Mn-centered storage of oxidative equivalents in every observable transition (Chrysina et al., 2023). Meanwhile, however, the interpretation of the X-ray free-electron laser (XFEL) crystallographic models nominally depicting S2S_2 was shown to be problematic (Drosou et al., 2023), and the low-oxidation program continues to publish supportive analyses through 2025–2026 (Ariafard et al., 2026; Gates et al., 2024). Within the HOP consensus, the structure and protonation of the S=5/2S=5/2 isomer and the protonation state behind the MLS continue to be actively refined (Corry and O'Malley, 2019; Taguchi et al., 2020; Kosaki and Mino, 2023; Saito et al., 2023; Flesher et al., 2022; Lampert et al., 2026), and synthetic [MnIIIMn3IVO4][\mathrm{Mn}^{III}\mathrm{Mn}^{IV}_3\mathrm{O}_4] cubanes reproduce both signal types (Shiau et al., 2023). What no study has delivered is a single model that quantitatively reproduces the complete fingerprint — both EPR signals, the full 55^{55}Mn tensor set including the small couplings, and the ligand hyperfine data — under an explicit ZFS/spin-orbit treatment, which is the problem stated here.

Problem Statement

Determine the electronic structure of the S2S_2 state of the photosystem II oxygen-evolving complex — its manganese oxidation-state pattern, ligand and water protonation pattern, and exchange-coupling scheme — that quantitatively reproduces, to within the experimental uncertainty of the cited EPR and ENDOR values, the complete spectroscopic fingerprint of this state within a single model. Specifically, the model must account for: (i) the simultaneous presence and interconversion of the S=1/2S=1/2 multiline EPR signal and the S=5/2S=5/2 g≈4.1g\approx 4.1 signal arising from the same oxidation pattern; (ii) the full set of 55^{55}Mn hyperfine couplings measured by ENDOR, including the two anomalously small couplings of approximately 45 MHz and 7 MHz reported in the 2.5 K Davies ENDOR study; and (iii) the ligand hyperfine couplings, namely the 14^{14}N coupling of His332, the 17^{17}O couplings of the oxo bridges and substrate waters, and the exchangeable 1^1H couplings — with zero-field splitting and spin-orbit coupling treated explicitly, beyond the strong-exchange limit, wherever exchange couplings are small. Resolving the statement requires both the fingerprint-reproducing model and the low-oxidation adjudication: establish whether any Mn(II)-containing low-oxidation formulation of S2S_2 in the mean-oxidation-3.25 class defined in the Background (including via the proposed mechanism in which a Mn(IV) ion becomes ENDOR-invisible at 2.5 K through very slow nuclear relaxation) can be reconciled with this complete fingerprint, or demonstrate that the fingerprint requires the Mn(III)Mn(IV)3_3 assignment with its two spin isomers, thereby settling the residual low-oxidation claims against the X-ray-structural and electron-counting evidence on which they rest.

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