Formation of a Copper(II)–Tyrosyl Complex at the Active Site of Lytic Polysaccharide Monooxygenases Following Oxidation by H2O2

Hydrogen peroxide is a cosubstrate for the oxidative cleavage of saccharidic substrates by copper-containing lytic polysaccharide monooxygenases (LPMOs). The rate of reaction of LPMOs with hydrogen peroxide is high, but it is accompanied by rapid inactivation of the enzymes, presumably through protein oxidation. Herein, we use UV–vis, CD, XAS, EPR, VT/VH-MCD, and resonance Raman spectroscopies, augmented with mass spectrometry and DFT calculations, to show that the product of reaction of an AA9 LPMO with H2O2 at higher pHs is a singlet Cu(II)–tyrosyl radical species, which is inactive for the oxidation of saccharidic substrates. The Cu(II)–tyrosyl radical center entails the formation of significant Cu(II)–(●OTyr) overlap, which in turn requires that the plane of the d(x2–y2) SOMO of the Cu(II) is orientated toward the tyrosyl radical. We propose from the Marcus cross-relation that the active site tyrosine is part of a “hole-hopping” charge-transfer mechanism formed of a pathway of conserved tyrosine and tryptophan residues, which can protect the protein active site from inactivation during uncoupled turnover.


■ INTRODUCTION
Lytic polysaccharide monooxygenases (LPMOs, also known as PMOs) are copper-containing enzymes that catalyze the oxidative cleavage of polysaccharides by dioxygen or hydrogen peroxide. 1 The active site of LPMOs contains a single copper ion coordinated by an N-terminal histidine through the NH 2 of the amino terminus and the π-N of its imidazole side chain. 2 A T-shaped coordination geometry at the Cu is completed by the τ-N atom of a further histidine side chain. This structural unit is known as the histidine brace 3 (Scheme 1). There is interest in LPMOs, not only for their use in commercial bioethanol production 4 and bacterial/fungal virulence 5 but also for the as yet unknowndetails of their catalytic mechanism(s), 6 especially the means by which the enzyme oxidizes a C−H bond in the polysaccharide substrate, the bond dissociation energy (BDE) of which is calculated to be ca. 100 kcal/mol. 7 Studies of LPMOs have concentrated on the active site, with more recent attention focusing on the role of amino acid residues within the secondary coordination sphere of the Cu center. 8 Here the situation is complicated by the fact that LPMOs exist in at least seven distinct phylogenetic groups (listed as classes AA9, AA10, 1b AA11, 9 AA13, 10 AA14, 11 AA15, 12 and AA16 13 in the CAZy database). 14 Each class presents a subtly different active site structure, due to differences in the identities and positions of amino acid residues in the secondary coordination sphere of the copper (Scheme 2). 15 The secondary coordination sphere of the copper ion in proteins can have profound effects on the reactivity of any exogenous ligands bound to the copper. 16 Indeed, in the context of LPMOs, ongoing site-directed mutagenesis work coupled with activity studies and EPR spectroscopic measurements have highlighted the critical role, in terms of catalytic activity, of the glutamine in the active site of AA9 LPMOs and the important roles of a tyrosine and noncoordinating histidine that are also found in the secondary coordination sphere. 8,17 Also, the significance of an alanine side chain in AA10 LPMOs has recently been demonstrated, in which the methyl group of the alanine likely restricts coordination of exogenous ligands in the axial position of the copper coordination sphere. 18 Among these residues, however, the role of the tyrosine found in all LPMO classes (except some AA10 LPMOs) and which is always positioned in the axial coordination position of the copper ion has attracted the most attention, not least because it is not clear how this side chain is not oxidized in preference to the substrate during catalytic turnover; BDE(O−H), ca. 88 kcal/mol. 19 In this regard, various proposals exist for the role of the tyrosine in the mechanism of LPMOs. Principal among these is that the tyrosine forms part of an electron transfer chain that delivers electrons from an exogenous reducing agent to the copper while the LPMO is in contact with a substrate. 10a There have also been proposals where the tyrosine/tyrosyl radical redox couple stabilizes an intermediate Cu(II)−oxyl or Cu(III)−OH species, similar to the formation of the porphyrin radical cation seen in Compound I of P450 enzymes. 20 A further proposal is that the tyrosine protects LPMOs from selfoxidation during the nonsubstrate-coupled turnover of O 2 ; 21 this suggestion parallels a similar role for tyrosine(s) in P450 enzymes. 22 In delineating a role for the tyrosine in LPMOs, however, direct experimental evidence is scarce. There have been no spectroscopic determinations of any intermediates, save for a single report from Singh et al., who observe tyrosyl radical formation upon treatment of a Cu(II)−LPMO with hydrogen peroxide in the presence of excess reducing agent. Using perpendicular-mode EPR, resonance Raman, and UV− vis spectroscopies, the authors of this study proposed the formation of a S = 1 Cu(II)−( • OTyr) ferromagnetically coupled pair, which was further suggested to be part of the catalytic cycle of LPMOs. 21,23 In addition to experimental work, DFT and QM/MM calculations have also been undertaken on several different LPMO systems in the presence of substrate. None of the preferred pathways from these calculations invokes a role for the tyrosine residue within the catalytic mechanism. 24 It is in this context that we report a multispectroscopic (EPR, VT/VH-MCD, CD, UV−vis, XAS, resonance Raman), mass spectrometry, and DFT study into a purple-colored species that arises during the uncoupled turnover 24c, 25 of an Scheme 2. Known Active Site Structures of LPMO, Classified According to the CAZy Database, Showing Conserved Residues in the Active Site a a L refers to exogenous ligands, usually H 2 O/OH − or Cl − . Wild-type AA11 and AA14 LPMOs may contain a methylated N-terminal histidine side chain (depicted as '?'), like AA9, but this is unknown as the production systems (E. coli or Pichia pastoris) used to produce these enzymes lack the necessary enzymatic methylation apparatus (the AA16 class is not included in the scheme, as no structure is yet available).

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Article AA9 LPMO with hydrogen peroxide at raised pHs. We show that this species is a stable Cu(II)−tyrosyl radical, akin to those seen in other copper oxidases like galactose oxidase. 26 In contrast to galactose oxidases, this tyrosine radical is not covalently modified nor is it part of the catalytic cycle of LPMOs. Moreover, at physiological pHs (<7) the purple species does not form to any significant extent, leading to the proposal that the active site tyrosine in LPMOs, along with a nearby tryptophan residue, is part of a hole-hopping pathway which protects LPMOs from oxidation during uncoupled turnover. 18a,27 This study also points to the challenges which highly oxidizing intermediates present to enzymatic systems and the means by which the potentially deleterious effects of these intermediates are mitigated by the protein, not only through the use of hole-hopping residues like tyrosine but also through glycosylation substitutions on the enzyme, a feature also revealed in our current study.

■ RESULTS AND ANALYSIS
Formation of a Purple-Colored LPMO Species, Its pH/ Substrate/Peroxide/Glycosylation Dependence, and Its Activity on (Oligo)saccharide Substrates. LPMOs catalyze the oxidation of poly(oligo)saccharide substrates with O 2 and reducing agent cosubstrates (e.g., ascorbate). In addition to O 2 acting as a cosubstrate, it has also recently been reported that hydrogen peroxide acts as a cosubstrate for LPMOs, replacing the combination of O 2 and reducing agent, albeit in a reaction which is accompanied by significant protein degradation. 1c, 28 Despite the fact that the reaction with peroxide is deleterious to the enzyme, the addition of peroxide to LPMOs provides for a potential laboratory "shunt" that avoids the complicating use of reducing agents within spectroscopic and activity studies. 24c Thus, taking advantage of the peroxide shunt reaction with LPMOs, we added various concentrations of hydrogen peroxide (from 0 to 2 mM) to ∼1 mM solutions of an AA9 LPMO from Lentinus similis (LsAA9) which had previously been spectroscopically and structurally characterized. 2,29 This AA9 LPMO is active on soluble oligosaccharide substrates, affording the opportunity to be able to perform spectroscopic studies on optically transparent solutions. The addition of hydrogen peroxide to LsAA9 was performed at room temperature (∼290 K) over a range of pHs and peroxide concentrations ( Figure 1). The reaction was also separately performed on both naturally glycosylated LsAA9 (the enzyme was produced using Aspergillus oryzae and Pichia pastoris as expression systems, which maintain glycosylation patterns on the protein and, in the former expression system, the N ε -methylation on His1) and its de-N-glycosylated variant, which were prepared using previously reported methods (Supporting Information). 2 The resulting solutions were monitored over time by UV− vis and EPR spectroscopies. In the absence of substrate and at raised pHs (>7), following an initial burst of bubbling (presumably O 2 gas), a strongly colored purple solution formed over a period of minutes, which then appeared to be stable over a period of days. The UV−vis and CD spectra of this solution exhibit several intense bands in the visible region ( Figure 1, see later for analysis). The addition of peroxide under anaerobic conditions to the Cu(I) form of LsAA9 generated the same purple species but without the initial burst of bubbling observed for the addition of hydrogen peroxide to the Cu(II) form of LsAA9. These observations suggest that the appearance of bubbles following the addition of hydrogen peroxide to the Cu(II) form of LsAA9 was associated with the reduction of the Cu(II) form by hydrogen peroxide and the concomitant formation of superoxide that disproportionated into O 2 and hydrogen peroxide. 30 The rate of formation of the purple species and its final concentration depended on the pH and the initial concentration of hydrogen peroxide, with high pHs exhibiting the highest rate of formation (>0.1 mM min −1 ) and highest final concentrations (Figure 1).
Once formed, the UV−vis spectrum of the purple species remained invariant across a pH range of 3.0−10.0 ( Figure S1). At pHs lower than 3.0, the solution turned colorless with concomitant loss of the main bands (11 790, 17 100, 20 400 cm −1 ) in the visible part of the spectrum. Addition of H 2 O 2 in the presence of cellohexaose (a known oligosaccharide substrate 25 for LsAA9) gave the same purple species but at a much lower rate (ca. 200 times slower, Figure S2).
To show that the formation of the chromophore, although not necessarily its location within the protein, is associated with the copper ion, the purple species was treated with a combination of reducing agent and EDTA at pH 10.0 as follows: the addition of sodium dithionite solution to the purple species gave a colorless and EPR-silent solution, which was then incubated with EDTA and passed through a size exclusion filter to remove the [Cu(EDTA)] 2− complex. The amount of Cu leftover in the sample was measured by CW-EPR spectroscopy and determined by spin quantification to be less than 5% Cu content with respect to the resting state enzyme at the same concentration, as shown in Figure S3 (see Methods section). Readdition of a Cu(II) solution to the protein solution in aerobic conditions immediately gave a purple-colored solution with the same visible spectrum as the original purple species (see Discussion for explanation of this effect). In the absence of a reducing agent it was not possible to decolorize the solution with the addition of EDTA alone,

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Article suggesting that the copper active site in the purple species is highly stable. In addition, we report that the same purple species could be formed under aerobic conditions at high pH by addition of ascorbic acid as reducing agent to the enzyme solution but at a much slower rate than the reaction with peroxide.
The ability of the purple species to catalyze the oxidation of polysaccharides with either O 2 (and sodium ascorbate as the reducing agent) or hydrogen peroxide was assessed using cellohexaose as substrate. To perform these experiments it was important to remove the small amounts of LsAA9 that had not been converted to the purple species (see EPR discussion and Methods). Therefore, excess cellohexaose was added to a solution of the purple species that had previously been treated with Na 2 EDTA and any [Cu(EDTA)] 2− removed (i.e., retaining the purple species and removing any Cu(II) from unreacted Cu(II)−LsAA9). The products of the reaction, i.e., any oxidized oligosaccharides, were then analyzed by MALDI-TOF MS. In both cases (hydrogen peroxide or O 2 /ascorbate) the purple species did not generate any oxidized oligosaccharides under standard oxidation conditions after 24 h, and thus, the purple species appears to be catalytically inactive for the oxidation of polysaccharides ( Figure S4). As a positive control, under the same conditions, LsAA9 was shown by MALDI-TOF MS to generate C4 oxidized oligosaccharide products, as already demonstrated by Frandsen et al. ( Figure S4). 2 SDS-PAGE gel analyses of the purple-colored solutions were performed ( Figure 2) to determine whether the lack of activity of the purple species was due to indiscriminate oxidation of the protein by the peroxide. The gels show that the purple species generated from LsAA9 that had been de-N-glycosylated indeed underwent extensive proteolytic degradation at pHs 7.0−8.0, even upon addition of low concentrations of hydrogen peroxide (0.15 mM) or in the presence of substrate (cellohexaose). Such degradation is not surprising given the potent oxidizing power of hydrogen peroxide solutions. In contrast to the deglycosylated sample, LsAA9 left in its glycosylated form following its expression in Aspergillus or Pichia showed no signs of denaturation even upon treatment with a 20-fold molar excess of hydrogen peroxide with respect to the enzyme concentration ( Figure 2). The protective effect of the glycosylated side chains is evident from this experiment. Following treatment with hydrogen peroxide, glycosylated LsAA9 remained essentially intact, save for some evidence from the SDS-PAGE gels (Figure 2) of the formation of a small amount (<1%) of a higher molecular weight species at ca. 60− 65 kDa. The same experiment was repeated on LsAA9 produced in Pichia pastoris as an expression system. Pichia can glycosylate but not methylate LPMOs with different glycosylation patterns/sites to Aspergillus. 31 Even in this case, no peptide fragments were generated upon incubation with hydrogen peroxide ( Figure S5). The finding that glycosylation protects eukaryotic LPMOs from oxidative damage by hydrogen peroxide serves as a useful reminder of the functional importance of glycosylated side chains in proteins and the need to be aware that the absence of glycosylation in AA9 LPMOs which have been expressed in prokaryotic hosts can significantly affect the stability of these proteins. Accordingly, in the studies reported below, the Aspergillus-produced, glycosylated LsAA9 was used in all spectroscopic investigations.
Sites of Oxidative Damage to the Protein Following Addition of Peroxide. The SDS-PAGE analysis described above does not provide detailed information about the sites of oxidative damage within the protein. In this regard, there is evidence from earlier studies that hydrogen peroxide treatment of LPMOs leads to significant oxidative damage of residues close to the copper active site. 1c Therefore, to determine the sites of oxidative damage and also to trace any potential redoxactive pathways in LsAA9, 32 we performed LC-MS/MS analysis of the peroxide-treated glycosylated purple species protein post protease digestion to determine the sites of oxidative modification ( Figures S6 and S7). 33 Figures S5 and S6). The use of isotopically labeled hydrogen peroxide allowed for differentiation of peroxide treatment-induced oxidation ( 18 O) from oxidation which occurred during the protein purification procedure or sample preparation for LC-MS/MS analysis The analysis shows that the oxidative modification of amino acids by hydrogen peroxide occurred at several different sites across the protein, with measurable oxidation of some tryptophan, tyrosine, and methionine residues ( Figure 3). Oxidation was also detected at other amino acid residues adjacent to the copper active site; as previously reported, 1c oxidation of the histidine 1 side chain was observed. Additional oxidative damage was seen on the active site residues His-79 and His-147, commensurate with the copper−histidine brace in LPMOs being a site that generates oxidizing species. Distant from the active site, oxidative modification of Tyr-65 (12.6 Å from Cu) and Trp-5 (17.6 Å) was observed (see Discussion). Also, several other aromatic residues (Tyr-137, Tyr-153, Trp-98) were oxidized; most of them are close to the enzyme surface. There was additional oxidative modification of Tyr-85 (18.8 Å away from active site), which is notable as it forms one-half of a conserved tyrosine-dyad (Tyr-85, Tyr-191 in LsAA9) that appears in all AA9 LPMOs and, furthermore, is not surface exposed. 27 Against expectations however, over all conditions there was no evidence for covalent modification of the active site tyrosine (Tyr-164). This is an important finding insofar as some copper-containing oxidases, including copper amine oxidases, are known to undergo oxidative maturation of nearby tyrosine residues into redox-active cofactors; this appears not to be the case in AA9 LPMOs. 34 Spectroscopic Characterization of the Purple Species. X-ray Absorption Spectroscopy of the Purple Species.
To determine the oxidation state of the copper ion in the purple species, X-ray absorption studies at 77 K were performed. For reference, X-ray absorption spectra were also collected on the dithionite-reduced, EPR-silent Cu(I)−LsAA9 and the Cu(II) resting state of LsAA9 (spin-Hamiltonian parameters as previously reported). 2 The combination of the XAS spectra of the purple species with those of the Cu(I) and Cu(II) forms of LsAA9 reports on the changes at a single copper site over three oxidation levels ( Figure 4).
The X-ray absorption spectrum of Cu(I)−LsAA9 exhibits a characteristic XAS feature at 8982.4 eV on the rising edge, which we assign as a Cu 1s to nonbonding 4p transition. 35 This peak is ca. 0.8−1.1 eV lower in energy than those reported for other three-coordinate Cu(I) complexes (8983.2−8983.8 eV). 35 The spectral profile is consistent with a Cu(I) oxidation state in which the coordination geometry at the copper is Tshaped N 3 . For Cu(II)−LsAA9, care was taken not to overexpose the sample to X-rays, which are known to photoreduce the copper from Cu(II) to Cu(I) in LPMOs; this was achieved by creating a raster pattern with the X-ray beam across the sample during collection. 18b,36 Under these conditions, the subsequent XAS exhibits a weak pre-edge peak around 8977.4 eV which results from the dipole-disallowed, quadrupole-allowed Cu 1s to 3d(x 2 −y 2 ) transition. Again, as for the Cu(I) spectrum, this transition is ca. 1−1.5 eV lower in energy than equivalent absorptions in XAS spectra of other Cu(II) complexes, save those of Cu zeolites (8977.5 eV) used as methane oxidation catalysts 37 and of distorted [CuCl 4 ] 2− 38 (8977.8 eV). At higher energies a more intense band is observed on the rising edge at 8985.9 eV, which is assigned to a three-state Cu 1s to 4p+LMCT "shakedown" transition, often reported in the XAS of Cu(II) species and which typically appear in the range 8986−8988 eV. 35 (Aside: it was recently proposed that the energy at which the "shakedown" transitions of Cu(II) complexes occur may be associated with ligand charge donation to the Cu and the amount of ligand orbital overlap with the Cu 4p orbitals. 39 ) The pre-edge peak at 8977.4 eV is slightly lower in energy than those reported for other Cu(II) complexes, indicative of some charge transfer to the Cu(II) center in LsAA9. This observation is in accord with the high reduction potentials (>250 mV vs SHE) 18b which are known for Cu(II) LPMOs. The position of the rising edge band at 8985.9 eV is also commensurate with a Cu(II) oxidation state. 35,40 Both the Cu(I) and the Cu(II) XAS closely match those found in the analogous oxidation state of another AA9 LPMO and the Cu(I) state of a AA10 LPMO reported in earlier studies. 18b, 30 Overall, the spectral features are consistent with Cu(I) and Cu(II) oxidation states of the dithionite-reduced and resting states of LsAA9 LPMO, respectively.
The XAS spectrum of the purple species in the pre-edge and rising edge regions is almost identical (peaks at 8977.8 and 8986.0 eV) to that of Cu(II)−LsAA9. Notwithstanding the similarity, an additional weak pre-edge feature at 8982.8 eV of similar intensity to the 8977.8 eV Cu 1s to 3d(x 2 −y 2 ) transition is also resolved. In the difference spectrum between the purple species spectrum and Cu(II)−LsAA9 (inset, Figure  4), this extra peak could be cleanly fit with a single Gaussian.

Article
The difference spectrum contains no other significant features in the pre-edge and rising edge regions, showing that the preedge 1s to 3d(x 2 −y 2 ) transition and the 1s to 4p+MLCT shakedown transition are essentially unaffected in intensity and energy between the two different species. Thus, given the similarity in the XAS spectra the formal oxidation state of the Cu center in the purple species can be assigned as Cu(II). A higher oxidation state assignment would require that the preedge peak is upshifted by the order of 1−2 eV. 40 The new peak at 8982.8 eV in the purple species falls outside the usual window (8986−8988 eV) of rising edge transitions, and it is also significantly shifted (+5.0 eV) from the Cu(II) 1s to 3d(x 2 −y 2 ) transition, showing that it is not due to a Cu(III) 1s to 3d(x 2 −y 2 ) transition. We can also rule out the possibility that this peak is due to a small amount of photoreduction, since the transition is at the wrong position (+ 0.4 eV) for the Cu(I) 1s-4p transition and there is also no apparent drop in the intensity of the Cu(II) 1s to 3d(x 2 −y 2 ) peak at 8977 eV between the purple species and Cu(II) LsAA9.
In summary, the positions of the shakedown transition and principal edge along with the position of the 1s to Cu 3d(x 2 − y 2 ) pre-edge feature are commensurate with a Cu(II) oxidation state (see Discussion) for both Cu(II)−LsAA9 and the purple species. In addition, the appearance of a new pre-edge peak at 8982.8 eV is indicative of the formation of a new interaction between copper and a ligand (see Discussion). 39,40 Optical and Magnetic Spectroscopies. Simultaneous fitting of the UV−vis and CD spectra of the purple species ( Figure  S8) revealed the presence of six different absorption bands at 11 790 (1400 M −1 cm −1 ), 17 100 (1800 M −1 cm −1 ), 20 400 (3600 M −1 cm −1 ), 24 560 (860 M −1 cm −1 ), 28 000 (2100 M −1 cm −1 ), and 30 810 cm −1 (3700 M −1 cm −1 ). These bands all grew into the UV−vis and CD spectra at the same rate during the purple species formation, suggesting that they are all associated with a single species. This spectrum is quite different from the UV−vis absorption spectrum of LsAA9 in its resting Cu(II) state, which is characterized by a weak and broad absorption band around 16 600 cm −1 , typical for dipoleforbidden Cu(II) d−d transitions (Figure 1). All of the visible absorption bands of the purple species disappeared upon treatment with an aqueous solution of sodium dithionite.
In generating the purple species, perpendicular-mode Xband CW-EPR spectroscopy showed that the axial type 2 copper signal of the Cu(II)−LsAA9 slowly disappeared following treatment with hydrogen peroxide to a new EPRsilent species ( Figure 5). EPR spectroscopy also demonstrated that the conversion of the resting state to the purple species was not complete, even at pH 10.0, as 15−20% of Cu(II) signal (as estimated by double integration of the EPR spectrum) remained following treatment of the Cu(II)− LsAA9 form with hydrogen peroxide.
The EPR-silent nature of the purple species demonstrates that it is not a Kramers' spin doublet, although it is not possible to determine from this single observation whether it is a non-Kramers' singlet or triplet state. Therefore, to determine the spin state, variable-temperature, variable-field magnetic circular dichroism (MCD) spectroscopy was carried out at pH 10. The MCD spectrum contained bands at 14 300 and 17 000 cm −1 and shoulders at 18 000, 14 300, 25 700, and 28 400 cm −1 , all of which showed little/no field or temperature dependence across the full temperature (5−55 K) and full magnetic field ranges (3−7 T) employed in the study (Figures 5 and S9). Thus, all of the bands in the MCD spectra (<55 K) arise from straightforward CD transitions. This observation establishes a singlet S = 0 ground state for the purple species ≤55 K, where the small variation recorded (<15% of band intensity) can be assigned to the 15−20% fraction of Cu(II)−LsAA9 resting state that remained in the sample ( Figure S9), consistent with the EPR studies described above. In regions of the spectrum that did not contain bands from the C-term transitions of Cu(II)−LsAA9 (21 000−23 000 cm −1 ) there was no change in signal intensity over the full temperature range ( Figure S9). Therefore, assuming that the lack of temperature variation seen in the MCD spectra requires a Boltzmann distribution of any higher spin state which is less than 2% (approximate signal-tonoise ratio) of the singlet species, an estimation of an upper limit of the exchange constant between singlet and higher order spin states of 2J ≈ −200 cm −1 may be made (the negative sign indicates antiferromagnetic coupling). In practice, 2J is likely to be much more negative than −200 cm −1 since the low-temperature (5 K) CD spectrum is similar to the room-temperature CD spectrum, indicating that even at ∼300 K there is no spectroscopically distinct higher spin state. The CD spectrum is not directly sensitive to the magnetic properties of the sample as there is no dependence on the magnetic field, but in switching from a singlet to a triplet electronic configuration, a change in the UV−vis electronic transitions is expected, which would be reflected in the CD spectrum as well. Resonance

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Article Under all of these different conditions identical resonance Raman spectra were obtained and no bands were observed to be isotopically sensitive ( Figure S10). This overall observation rules out the possibility of the spectroscopic features arising from a Cu−peroxide or Cu−superoxide unit. The resonance Raman spectra were obtained with 532 and 785 nm laser excitations, which are associated with the absorptions appearing at 11 790, 17 100, and 20 400 cm −1 in the visible spectrum ( Figure S11). With 785 nm excitation, Raman bands in the spectrum appeared below 700 cm −1 with a prominent band appearing at 352 cm −1 (Figure 6, top). Using 532 nm laser excitation, a similar resonance Raman spectrum in the low-energy region was obtained, although the Raman band at 344 cm −1 was comparatively weaker. Conspicuously, excitation at 532 nm generated a rich Raman spectrum in the high-energy region (1300−1600 cm −1 ), which is typical for ligand-based vibrational modes. Together, these results are consistent with the electronic transition at 20 400 cm −1 being mostly ligand in character, whereas the transition at 11 790 cm −1 is significantly metal in character.
A comparison of the resonance Raman spectra of the purple species with those of the oxidized form of galactose oxidase, which contains a Cu(II)−(modified)tyrosyl radical in the active site (Table 1), shows that bands at 1596, 1482, and 1386 cm −1 have a direct correspondence with bands in the resonance Raman spectra of galactose oxidase. 41 The similarity in the positions between the two proteins suggests that a Cu(II)−tyrosyl species is also the source of the these bands in the resonance Raman spectrum of the purple species. Bands at ∼1330 and 1515 cm −1 in the spectrum of the purple species are unassigned, but we note that the 7a′ (C−O) mode of a noncoordinated tyrosyl is reported at 1516 cm −1 . 42  In order to test this hypothesis and to provide a framework within which to interpret the spectroscopic results, we undertook DFT and TD-DFT calculations on models of LsAA9. The models were based on the coordinates of the X-ray crystal structure of LsAA9. We used a cluster model of the active site, which is known from comparison with our previous QM/MM and DFT studies to model faithfully the active site structure of Cu(II)− LsAA9. 24a,c A Cu(II)−tyrosyl electronic state was optimized for both the triplet and the broken symmetry (BS) singlet electronic configurations using the BP86 functional. As the full coordination sphere of the copper in the purple species is unknown, we explored several different models that differed in the type of exogenous ligands (H 2 O/HO − ) which coordinate to the copper and their cis or trans position with respect to the tyrosyl radical ( Figure S12). The optimization on the BS singlet surface of these models showed differences with respect to those calculated on the triplet surfaces, most notably for Model3-OH trans (Table S1), where the principal difference between the two structures was the length of the Cu···OTyr contact (ca. 2.0 Å in the singlet-optimized structure and ca. 2.4 Å in the triplet-optimized structure). Therefore, given the large differences in structures between singlet and triplet states, the exchange coupling constants were calculated for both the broken-symmetry (BS) singlet and the triplet-optimized geometries. In all cases, as expected, a single-point BS calculation using B3LYP as functional from the triplet optimized geometry gave the lowest energy state with a positive J value (i.e., ferromagnetic coupling). In contrast, performing the single-point calculation with the singletoptimized geometry resulted in two structures with a modest (Model2-H 2 O trans , J = −132 cm −1 ) and strong (Model3-OH trans , J = −1004 cm −1 ) antiferromagnetic coupling (Table S2, Figure 7). Both of these structures had a short Cu−OTyr bond, 2.19 and 2.01 Å, respectively, albeit slightly longer than the equivalent bond observed in Cu(II)−phenoxyl radical complexes (1.94 Å). 43 Mindful of the well-known issues associated with the accuracy of BS calculations with transition metals and in particular their sensitivity to the degree of Hartree−Fock   (Table  S2). The same functionals predicted small exchange constants for the cis configuration, incommensurate with experimental measurements. Thus, all functionals predict a large singlet− triplet energy gap for the trans hydroxide configuration. Time-dependent DFT calculations of the UV−vis spectra and Cu K-edge XAS were performed on Model2-H 2 O trans and Model3-OH trans in their singlet electronic configuration using the B3LYP functional. For the UV−vis electronic transitions, at least one intense band was predicted in the visible region for both models, together with lower intensity bands ( Figure S13). In Model2-H 2 O trans the most intense band was calculated to appear at 24 800 cm −1 and arose from a MLCT transition (Cu to Tyr-radical) according to its transition difference density ( Figure S14). A second, less intense, transition at 15 500 cm −1 came from a LMCT (Tyr-radical to Cu) transition. For Model3-OH trans an intense MLCT (and with significant HO − character) was predicted at 12 390 cm −1 , together with a set of LLCT (histidine to tyrosine) and LMCT (histidine to Cu) transitions at higher energy (21 800 and 25 500 cm −1 ). These results assigned opposite character to the low-energy transition (∼11 800 cm −1 ) in the UV−vis spectrum of the purple species, LMCT for Model2-H 2 O trans , and MLCT for Model3-OH trans . Similarly, the nature of the higher energy transition (20 400 cm −1 ) between the two models was predicted to be different in nature: MLCT for Model2-H 2 O trans , His to Tyr (LLCT) and His to Cu (LMCT) for Model3-OH trans . These results are in partial agreement with the experimental spectrum as the relative intensities of the experimental transitions are not modeled accurately. The discrepancy between experimental and calculated intensities likely arises from significant multi-configurational character of the copper(II)−tyrosyl species. In this case, multireference calculations would be needed to model the UV−vis spectrum; these calculations will be considered in a future study.
The TD-DFT-calculated K-pre-edge XAS of both Model2-H2O trans and Model3-OH trans exhibit two weak features, the first at ∼8977 eV (for both models) and another at higher energy 8981.5 and 8980.0 eV, respectively ( Figure S15). The first feature is assigned to a standard Cu 1s → 3d transition (8977 eV), while the second corresponds to a MLCT from Cu 1s to the tyrosyl radical. The calculated energy separation (4.3 and 2.3 eV, respectively) between the two features is smaller than that determined experimentally (5.0 eV); however, the exact energy of the calculated transitions is known to be heavily dependent on the functional chosen for the calculation and is therefore not generally predictive. On the other hand, the number and intensities of the calculated peaks are more reliably predicted from calculations, and from this perspective, the match between experiment and theory is excellent. 44 Vibrational frequencies were calculated at the same level of theory used for geometry optimization (BP86, Def2-TZVP/ Def2-SVP, see DFT methods section) and gave Raman active vibrations for both Model3-OH trans and Model2-H 2 O trans at similar frequencies to those observed experimentally (Table  S5). The C−O tyrosyl stretch (Tyr 7a′) is calculated at 1455 and 1451 cm −1 , respectively (cf. ∼1482−1486 cm −1 ), and a Cu−OTyr stretch at 375 and 320 cm −1 , respectively (cf. 344− 352 cm −1 ). On the basis of the calculated J value, TD-DFT, and vibrational calculations, the most plausible structure for the purple species possesses a hydroxide ligand that lies trans to the tyrosyl ligand (Model3-OH trans in Figure 7), although we cannot rule out the model where a water molecule lies trans to the tyrosyl, Model2-H 2 O trans .
From the DFT and TD-DFT studies it is not possible to make a definitive conclusion on which model (Model2-H 2 O trans or Model3-OH trans ) best represents the structure of the purple species. Both are consistent with the experimental and calculated data. However, the lack of pH sensitivity of the purple species might argue more for Model3-OH trans being the representative species.

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Article ■ DISCUSSION Assignment of Spectroscopic Features. The addition of hydrogen peroxide to a ∼ 1 mM solution of LsAA9 LPMO (in either the Cu(II) or Cu(I) form) at pHs > 7.0 affords a purplecolored species. The dependence of the absorptions within the visible spectrum on the presence of copper shows that they arise from transitions associated with the copper active site. The combined XAS, EPR, and MCD spectroscopic data establish the species as an open-shell singlet in which one unpaired electron is associated with the Cu(II) center (from XAS) and the other with a coordinating ligand. This ligand cannot be a peroxide or a coordinated water molecule, since the resonance Raman spectra are insensitive to the isotopic substitution of peroxide. The observation also rules out the formation of an antiferromagnetically coupled Cu 2 −μ-peroxo dimer. Of the remaining ligands that could harbor an unpaired electron, the active site tyrosine offers the most reasonable possibility, and indeed, resonance Raman data of the purple species are best assigned by comparison to the oxidized form of galactose oxidase, which is known to contain a Cu(II)− (modified)tyrosyl radical pair. 34 We further considered the potential formation of an N-oxide at the amino terminus, but this species would be expected to have a prominent N−O vibration in the resonance Raman spectrum at 800 cm −1 , which is not observed. Also, while the spectroscopic data do not completely rule out a potential Cu(II)−semiquinone species which could arise from the covalent oxidative modification of the tyrosine, the possibility is very much reduced by the lack of any observable modification of the tyrosine in the mass spectrum of the purple species and by the absence of isotopic shifts in the resonance Raman spectra. 45 To secure the assignment of the purple species as a Cu(II)− tyrosyl center, we note the appearance of a weak pre-edge feature in the XAS (8982 eV) which is not present in the Cu(II)−LsAA9 spectrum. On the basis of previous examples of similar features in the XAS spectra of Cu(II) complexes and the TD-DFT calculations, this pre-edge feature is assigned to a 1s to SOMO transition where the SOMO has significant tyrosyl character. 39,40 The fact that this XAS transition has some intensity, along with the observed CT transition at 11790 cm −1 in the visible spectrum of the purple species, demonstrates that there is an appreciable overlap between the SOMOs of the tyrosyl and the Cu center. While unusual, the occurrence of second pre-edge peaks in the XAS spectra of metal complexes is not unprecedented, having been observed in complexes where strongly coordinated ligands which have low-lying empty π* orbitals gain σ-overlap with the Cu orbitals through distortion of the ligand. 39,40,45 Such an interaction could arise in LsAA9 where structures show that the conformation of the tyrosine with respect to the Cu admits some overlap of the π-manifold orbitals of the tyrosyl with the Cu 3d(x 2 −y 2 ) orbital ( Figure 8). Notably, this orbital pathway can only exist if the 3d(x 2 −y 2 ) orbital plane of the Cu is rotated out of the plane of the histidine brace toward the tyrosine O atom. This rotation further requires the presence of an exogenous ligand in the trans position to the tyrosyl ( Figure  8), matching the best-fit models from DFT calculations. Previous structural studies have shown this exogenous ligand is displaced on the binding of substrate, thus linking the formation of the purple species with the absence of substrate, as also observed experimentally herein.
Further evidence that the purple species is a Cu(II)−tyrosyl pair is gained from comparison with known small-molecule complexes, where experimental determination of the value of the exchange constant J as a function of the Cu−O−C angle (Figure 8) shows that a singlet ground state is only observed when this angle is near 130°(and the Cu−O−C−C dihedral angle ≈ 90°). 46 In LsAA9 the equivalent angles are 124°and 87°, respectively. Finally, we note here that careful inspection of the K-edge XAS spectrum of oxidized Cu(II) in galactose oxidase shows a similar pre-edge feature at ∼8985 eV, which was assigned at the time to small differences in coordination geometry between the oxidized and the reduced versions of the enzyme but now we would suggest represents the transition described above. 47 Thus, the data presented herein are commensurate with the formation of an intensely colored, stable Cu(II)−tyrosyl complex, which is formed during the noncoupled turnover of an AA9 LPMO with hydrogen peroxide. This species has an open-shell singlet ground state, in accord with the formation of a strong Cu(II)−O bond, leading to intense charge-transfer bands in its visible spectrum.

Journal of the American Chemical Society
Article Hydrogen Peroxide as a Cosubstrate for LPMOs. Formation of the tyrosyl radical at the active site of LsAA9 provides evidence that this is the site of generation of the oxidizing species in LPMOs, following addition of hydrogen peroxide. Hydrogen peroxide is a powerful oxidant, and its use as a cosubstrate in the reactions of LPMOs has been the center of much recent debate. 4c,48 This debate concerns itself with whether hydrogen peroxide or O 2 /reducing agent are the in vivo cosubstrates for LPMOs. While acknowledging that the peroxide/O 2 debate is not settled, our own working hypothesis for the work described herein is that hydrogen peroxide is a useful laboratory shunt for AA9 LPMOs for both coupled and uncoupled activities. In the former role it acts to simplify mechanistic studies, while in the latter it gives insight into the structural apparatus which LPMOs employ to deal with oxidizing intermediates generated at the active site in the absence of substrate. From this perspective we have shown herein that AA9 LPMOs are significantly protected from oxidative damage by their own glycosylation patterns. We also observe that some amino acid side chains (both at the surface and buried within the protein structure) are covalently modified after treatment with hydrogen peroxide (Figure 3), suggesting that these amino acids are redox active. This last aspect directs us toward the possibility that LPMOs are equipped with specific internal charge-transfer mechanisms for dealing with the oxidizing species which are generated during its catalytic cyclea proposal already made by others, 22a particularly given the parallels to P450 and also to the fact that the active site in LPMOs is surrounded by amino acid residues (e.g., tryptophans and tyrosines) that are in principle capable of translating a positive hole away from the active site. 49 Role for the Active Site Tyrosine in LPMOs. Mass spectrometry analysis shows that challenging LsAA9 with hydrogen peroxide during uncoupled turnover does not lead to covalent oxidative modification of the active site tyrosine (Tyr-164). Not only does this observation take this LPMO away from the class of other copper-containing enzymes that possess tyrosine-derived redox-active cofactors (e.g., quinones), it also provides evidence that the tyrosyl is converted to a tyrosine by an efficient charge-transfer mechanism within the protein.
Inspection of the LsAA9 structure shows that such mechanism could exist whereby the tyrosyl radical at the active site is quickly reduced to a tyrosine by a combination of rapid hole hopping from Trp-64 (8.1 Å away, Figure 9) and back proton transfer from water. The tryptophan cation is subsequently reduced by other amino acid side chains along a chargetransfer pathway (see below).
Taking the above discussion as a basis for the role of the tyrosine in the active site of LPMOs, any potential holehopping pathways and the rates at which charge transfer occurs through these pathways can be examined using Marcus theory. The rate constant for any donor−acceptor pairwise interaction along a hole-hopping pathway can be estimated using a chargetransfer rate expression as follows 50 Elements of the equation can be calculated/estimated from the known self-exchange reorganization energies of the donor (λ DD ) and acceptor (λ AA ), the reduction potentials of the donor and acceptor, and the distances between the donor and the acceptor, the last of which is obtained from structural information. The effective electronic coupling (V DA ) can be estimated using Hopfield's equation. 51 On the basis of the charge-transfer rate expression, a protein structure can then be searched for potential hole-hopping pathways and their rates calculated. To this end, a computer program, EHPath, is available to perform this search rapidly. 52 Accordingly, we applied EHPath to all of the potential holehopping residues (tyrosine, tryptophan, cysteine) within the known structure of LsAA9 2 using reduction potentials and reorganization energies at pH 7 and where the tyrosine at the active site (Tyr-164) acts as the hole donor. From this analysis a single and clear hole-hopping pathway in LsAA9 emerges, which transfers a hole away from the tyrosyl radical (Tyr-164) to a surface residue (Trp-5) through Trp-64 and Tyr-65 with a Figure 9. Depiction of LsAA9 structure (gray ribbons) and amino acid side chains (cylinder bonds in green) involved in putative hole-hopping pathway. Cu ion is represented as an orange sphere, and distances are given in Angstroms.

Journal of the American Chemical Society
Article mean-residence time of 6 ms ( Figure 9). All other pathways in the protein have residence times of >1 s ( Table 2). The rapid rate of the Tyr-164···Trp-5 pathway parallels similar holehopping pathways seen in the enzymes P450 (37 ms), BSS (4.5 ms), and CCP1 (2.5 ms). 52 In a further parallel to these enzymes, the calculated activation energy of H-atom abstraction from substrate in coupled turnover by LsAA9 is low (ΔG ‡ = 5.5 kcal mol −1 from QM/MM calculations) such that the rate of H-atom abstraction can be expected to be faster than the rate of hole hopping. As such, it is evident that the active-site tyrosine in LsAA9 along with adjacent Trp-64 could form part of an efficient charge-transfer pathway through LPMOs at pH 7, which is active during uncoupled turnover of the LPMO. It should be noted here that the network of aromatic residues connecting the Cu active site to the outside of the protein is largely conserved in the AA9 family. 20 The formation of the Cu(II)−tyrosyl species at pHs > 7 observed in our experiments is likely to be due to a combination of three factors. The first is, straightforwardly, that the active site tyrosine is easier to oxidize at higher pHs (reduction potential of tyrosyl is ∼0.7 V at pH 10 and 0.93 V at pH 7). 53 The second is that our MS results show that several redox-active residues, including those in the hole-hopping pathway, are covalently modified in the experiment, thereby compromising the protein's capacity to transfer charge away from the active site tyrosine. In such circumstances it may be that there is an effective buildup of tyrosyl radical at the active site, whichunder the conditions employed in our studyis eventually "extinguished" by the formation of a stable Cu(II)− tyrosyl bond (i.e., purple species). Third, the formation of the bond occurs through a process which involves a pH-dependent reorganization of the Cu coordination sphere as described above.
Roles of Substrate in the Turnover of LPMOs. The Cu(II)−tyrosyl radical species does not form in the presence of substrate. This finding highlights two factors in AA9 LPMO (bio)chemistry. The first is that the presence of a bound substrate changes the mechanistic pathways available to AA9 LPMOs, ostensibly by locking the copper equatorial coordination sites into the plane of the histidine brace ligands. The locking is achieved by displacement of the axial water molecule in the Cu coordination sphere and increasing the σdonation capacity of the NH 2 ligand, as previously demonstrated by EPR studies on LsAA9. 2 Second, the presence of an efficient hole-hopping pathway in LPMOs confounds kinetic comparisons between the relative reactivity of H 2 O 2 and O 2 /reducing agent as cosubstrates. The complication arises since the presence of a soluble reducing agent in the latter allows the hole-hopping mechanism to operate repeatedly to extinguish oxidizing equivalents generated at the active site. This pathway will compete against any weakly coupled pathway with substrate and thereby ostensibly lower the observed rate of reaction of substrate oxidation. Critical aspects in this regard are the availability (concentration) of substrate, its match to the LPMO under study, the presence of a carbohydrate-binding module, and the concentration and oxidation potential of the reducing agent, all of which are factors known to affect the rate of substrate oxidation by LPMOs. 25,48,54 ■ CONCLUSIONS The addition of hydrogen peroxide to an AA9 LPMO at high pHs in the absence of substrate results in the formation of a highly stable, purple-colored Cu(II)−tyrosyl complex that has been characterized using spectroscopic methods (UV−vis, CD, MCD, resonance Raman, EPR). The copper(II)−tyrosyl bond forms after the slow time scale "rotation" of the copper equatorial plane out of the plane of the histidine brace coordinating atoms. The redox activity of the active site tyrosine is indicative of its role in LPMOs, which is to act as part of an efficient charge-transfer pathway between the active site and the protein surface. Such a pathway, consisting of tyrosine and tryptophan residues and spanning ∼15 Å, has been identified in the LPMO used in our studies.

■ METHODS
Preparation of LsAA9 LPMO. LsAA9 LPMO was purified as reported previously. 9,25 Formation of the LsAA9 Purple Species. The reduced Cu(I) state of LsAA9 was generated by reaction of the enzyme with excess ascorbic acid inside a N 2 atmosphere glovebox. The excess ascorbic acid was then removed via buffer exchange with a 10 kDa MWCO VivaSpin centrifuge concentrator. All of the solutions used inside the N 2 atmosphere glovebox were degassed by freeze−pump−thawing on a Schlenk line (water, buffers) or by purging the solution with N 2 for 30 min (protein and H 2 O 2 solutions). H 2 O 2 in an appropriate amount was then added to the Cu(I)−LsAA9 solution to initiate the reaction. When starting from the Cu(II) resting state, H 2 O 2 was simply added to the protein solution without degassing.
LsAA9 Deglycosylation. LsAA9 was incubated with a His-tagged Endoglycosidase H (Endo H) in a 10:1 molar ratio in 20 mM Na− phosphate at pH 7.2 for 2 days at room temperature. NaCl and imidazole were added to the solution up to a final concentration of 500 and 25 mM, respectively; then the solution was applied to a 1 mL HisTrap FF column to remove the Endo H from the sample. EDTA was added to the flow through to a final concentration of 2 mM, and then it was incubated for 2 h at room temperature. The flow through was then applied to a Superdex 75 16/600 column, pre-equilibrated with 20 mM Na−phosphate, 250 mM NaCl at pH 7.2. The eluted fractions corresponding to the deglycosylated LsAA9 were then concentrated, copper loaded with 1 equiv of CuSO 4 ·5H 2 O, and buffer exchanged in 20 mM Na−phosphate at pH 6.0 with a 3 kDa MWCO VivaSpin centrifuge concentrator.
UV−vis, CD, and MCD Spectroscopies. The UV−vis absorption spectra were acquired on a Shimadzu UV-1800 spectrometer or on a PerkinElmer Lambda 465 diode array spectrophotometer. For the kinetics, the Cu(I)−LsAA9 and H 2 O 2 solutions were prepared as described above. The sample was then transferred to the spectrometer in a sealed cuvette, and an appropriate amount of deoxygenated H 2 O 2 was quickly added to initiate the reaction.
CD spectra were recorded on a Jasco J810 spectropolarimeter at room temperature. MCD spectra were recorded on a Jasco J-810 spectropolarimeter adapted to incorporate an Oxford Instruments Spectromag SM4000 magnetocryostat. The sample solutions were loaded into cells of ca. 2 mm path length constructed from quartz discs separated by a rubber ring spacer and frozen in liquid nitrogen.

Article
The spectra were collected at 3, 5, and 7 T with temperatures between 5 and 55 K. EPR Spectroscopy. Continuous-wave X-band frozen solution EPR spectra were acquired on a Bruker micro EMX spectrometer operating at ∼9.30 GHz with a modulation amplitude of 4 G, modulation frequency of 100 kHz, and microwave power of 10.02 mW. The spectra are the summation of 3 scans and were recorded at 170 K. The purple-colored species samples were generated in the same way as for the UV−vis experiments. EPR spin quantitation, via double integration of the spectra, of the paramagnetic Cu concentration was performed using a 0.200 mM CuSO 4 , 10 mM HCl, 2 M NaClO 4 standard solution.
The conversion of the Cu(II)−LsAA9 resting state to the purple species was estimated via EPR spin quantitation. It was assumed that the Cu(II) signal reduction was only due to conversion in the purple species. At pH 10.0, after the reaction with H 2 O 2 , the final Cu(II) concentration was 75−80% less than the Cu(II) resting state at the same protein concentration (i.e., 75−80% conversion into the purple species). To determine the Cu(II) concentration of the apoprotein after the purple species reduction and treatment with EDTA, the sample was buffer exchanged, under anaerobic conditions, to remove the excess of reducing agent and the [Cu(EDTA)] 2− complex. The sample was then taken to pH 2.0 by adding HCl to denature fully the enzyme. The Cu(II) concentration was then measured by EPR via spin quantitation.
XAS. XAS spectra were collected on a 1.0 mM solution of enzyme LsAA9 at pH 10.0, which had been flash frozen to 77 K. Data were acquired on the sample at 90 K at the B18 Core Spectroscopy beamline at Diamond Light Source, Oxfordshire, UK. At the time of the measurement the Diamond synchrotron was operating at a ring energy of 3 GeV. The beamline was equipped with a Si(111) doublecrystal monochromator, and harmonic rejection was achieved through the use of two Pt-coated mirrors operating at an incidence angle of 9 mrad. The monochromator was calibrated using the first maximum in the derivative in the edge region of the XAS spectra of a copper foil placed between the second and the third ion chambers at 8979 eV. Data were collected in fluorescence mode from 8770 to 9020 eV using a nine-channel Ge solid-state detector at the copper K absorption edge (∼8980 eV) in 1 eV steps. The measurements were collected at 77 K.
Resonance Raman Spectroscopy. Samples were prepared in the same way as the UV−vis samples but using H 2 18 O 2 , D 2 O, or H 2 18 O for the isotopically substituted samples. Spectra were collected using a HORIBA XploRA Raman microscope at room temperature using 532 and 785 nm laser wavelength excitations. The spectrometer gratings used were 2400 and 1200 gr/mm, respectively, together with a confocal pinhole size of 500 μm and slit width of 200 μm. The laser power was ∼7 mW. Samples were measured in the liquid state using a 63×/1.0 dipping objective (Zeiss). To test for heating effects, measurements were also made on the samples in the frozen state facilitated by using a LN 2 cooling stage and 100×/0.9 lens with the rest of the acquisition parameters remaining the same as those used for the liquid sample measurements. The frozen sample results showed no significant spectral differences compared to the liquid state data. Real-time spectral acquisition was also performed to optimize the acquisition parameters (signal-to-noise) and to verify nondestructive testing. To ensure acceptable measurement statistics, ∼40 spectra were collected per sample tested. The spectra were processed (baseline corrected, normalized, averaged) and then analyzed using OriginPro (2018) software with processing and spectral analysis also independently checked using IGOR Pro (v.6.3.7). Accounting for the measurement statistics, the maximum uncertainty associated with the Raman band positions was found to be ca. ±2 cm −1 .
Analysis of the Reaction Products. Cellohexaose was used as substrate. One hundred microliter reactions were set up with 750 μM cellohexaose, 1 mM ascorbic acid, 100 μM H 2 O 2 (no H 2 O 2 added in the O 2 turnover reactions), and 1 μM LsAA9 or purple LsAA9 in 5 mM MES at pH 7.0 and were incubated at 40°C for 2 h. The reaction was then quenched by addition of 3 reaction volumes of ethanol (98% v/v). Reactions with H 2 O 2 were performed inside an N 2 atmosphere glovebox. A 1 μL amount of sample was then mixed with 2 μL of 10 mg/mL 2,5-dihydroxybenzoic acid in 50% acetonitrile, 0.1% trifluoroacetic acid on a Bruker SCOUT-MTP 384 target plate. The spotted samples were then dried in air under a lamp before being analyzed by mass spectrometry on a Ultraflex III matrix-assisted laser desorption ionization-time-of-flight/time-of-flight (MALDI-TOF/TOF) instrument (Bruker), as described previously. 9 The purple species LsAA9 sample used in the assay was incubated with EDTA overnight to remove Cu 2+ from any LsAA9 that had not been converted to the purple species. The resulting [Cu(EDTA)] 2− complex was then removed from the solution by ultracentrifugation through 10 kDa cutoff size-exclusion filters.
DFT. Spin-unrestricted density functional theory (DFT) calculations were performed using the ORCA 4.1 electronic structure package. 55 The different cluster models were derived from the X-ray crystal structure of LsAA9 (PDB 5ACG). 2 Geometry optimizations were performed with the BP86 56 functional (with RI approximation), Def2-TZVP basis set 57 on Cu and ligating atoms, and Def-2-SVP on all of the remaining atoms; empirical dispersion correction were accounted for using Grimme's D3 method with Becke−Johnson damping (D3BJ); 58 solvation effects were included with the conductor-like polarizable continuum model (CPCM, ε = 4.0). The broken symmetry (BS) approach was used to optimize the singlet spin state geometry in each model. Single-point energies were calculated using the B3LYP functional 59  UV−vis and Cu K-edge absorption spectra were calculated with the time-dependent density functional theory (TD-DFT) approach applying the Tamm−Dancoff approximation. 61 The UV−vis absorption spectra were computed with the B3LYP functional, Def2-TZVP basis set on all atoms, and RIJCOSX 62 approximation with a dense integration grid (ORCA Grid5). The K-edge calculations were performed on the B3LYP functional together with the ZORA scalar relativistic approximation; 63 the CP(PPP) basis set 64 was used on the Cu and the ZORA-Def2-TZVP basis set 65 on all other atoms. In the TD-DFT approach, the description of the core hole leads to a systematic error in the absolute energy transitions, which can be compensated by a constant energy shift (which is characteristic for each functional and basis set). 66 Here, the calculated 1s → 3d preedge transition of the Cu(II) resting state model was used to calibrate the method. An energy shift of −5.8 eV was applied to all calculated transitions. Full details on the cluster models and the coordinates of the optimized geometries can be found in the Supporting Information.
LC-MS/MS. Full details on the experimental procedure and data analysis for LC-MS/MS can be found in the Supporting Information.