Latent and active abPPO4 mushroom tyrosinase cocrystallized with hexatungstotellurate(VI) in a single crystal

Mushroom tyrosinase isoform abPPO4 (Agaricus bisporus polyphenol oxidase 4) was crystallized by means of an Anderson-type polyoxometalate. The enzyme crystallized as a crystallographic heterodimer containing the zymogen (L-TYR; 64 kDa), the 21 kDa smaller activated form (A-TYR) and the polyoxometalate (POM) within one single crystal in a 1:1:1 ratio.

Tyrosinases, bifunctional metalloenzymes, catalyze the oxidation of monophenols and o-diphenols to o-quinones, the precursor compounds of the brown-coloured pigment melanin. In eukaryotic organisms, tyrosinases are expressed as latent zymogens that have to be proteolytically cleaved in order to form highly active enzymes. This activation mechanism, known as the tyrosinase maturation process, has scientific and industrial significance with respect to biochemical and technical applications of the enzyme. Here, not only the first crystal structure of the mushroom tyrosinase abPPO4 is presented in its active form (Ser2-Ser383) and in its 21 kDa heavier latent form (Ser2-Thr545), but furthermore the simultaneous presence of both forms within one single-crystal structure is shown. This allows for a simple approach to investigate the transition between these two forms. Isoform abPPO4 was isolated and extensively purified from the natural source (Agaricus bisporus), which contains a total of six polyphenol oxidases (PPOs). The enzyme formed crystals (diffracting to a resolution of 2.76 Å ) owing to the employment of the 6-tungstotellurate(VI) salt (Na 6 [TeW 6 O 24 ]Á22H 2 O) as a cocrystallization agent. Two of these disc-shaped Anderson-type polyoxoanions [TeW 6 O 24 ] 6À separate two asymmetric units comprising one crystallographic heterodimer of abPPO4, thus resulting in very interesting crystal packing.
Polyoxometalates (POMs), which are anionic metal-oxo clusters of early transition metals in high oxidation states, exhibit a unique structural and compositional variety (Pope, 1983;Pope & Kortz, 2012). POMs have interesting electronic, redox, catalytic, optical, thermal, magnetic and bioactive properties and are hence studied in many different fields of science and technology (Mü ller et al., 2001;Schnack et al., 2006;Kortz et al., 2009;Iqbal et al., 2013;Jahier et al., 2013). The high negative charge, large size, shape and water-solubility of POMs allows binding to proteins, which enables their utilization as effective protein-crystallization agents (Zhang et al., 2007). However, the employment of POMs in this regard has so far mostly been limited to crystal-soaking experiments, exploiting their potential for phasing by either isomorphous replacement or anomalous scattering (Corey et al., 1962;Ladenstein et al., 1987;O'Halloran et al., 1987;Thygesen et al., 1996;Rudenko et al., 2003;Zebisch et al., 2012;Dahms et al., 2013). Additionally, POMs have been implemented as contrast agents in protein crystallography in order to elucidate buried compound channels in larger proteins (Dauter, 2005). It is also worth noting the famous crystal structure of the 50S ribosome (Deinococcus radiodurans) where crystals were soaked with the Keggin-type POM salt K 5 H[PW 12 O 40 ]Á12H 2 O (Schluenzen et al., 2000;Harms et al., 2001;Pioletti et al., 2001).
Based on X-ray crystallographic studies, POMs (mostly of the Keggin, Lindqvist and Well-Dawson types) are part of the structure of around 25 PDB entries (Pioletti et al., 2001;Locher et al., 2002;Kowalewski et al., 2012;Zebisch et al., 2012Zebisch et al., , 2014. However, owing to mostly poorly defined electron densities at POM binding locations described in the literature or to a lack of interest in binding modes because POMs were only incorporated for phasing purposes, a detailed structural POM binding mode to proteins has so far rarely been defined. The exceptions are a self-assembled POM (PDB entries 4f6t and 2ogx) in a molybdenum-storage protein (Schemberg et al., 2007) and a very recent structure of NTPDase1 (PDB entries 4bvo, 4bvp and 4brh; Zebisch et al., 2014). The latter publication describes in detail the binding modes of soaked and cocrystallized POMs, namely dodecatungstate, decavanadate and octamolybdate/heptamolybdate. Interestingly, besides the predominantly electrostatic interactions and hydrogen bonds described in this study, covalently bonded POMs have also been identified (Zebisch et al., 2014).
The mushroom tyrosinase abPPO4 was extensively purified and crystallized using a method described elsewhere (Mauracher, Molitor, Al-Oweini et al., 2014;Mauracher, Molitor, Michael et al., 2014). In the present crystallographic study, the crystal structure of active abPPO4 (UniProt C7FF05 and K9I869) and its zymogen, simultaneously present in one structure, are described. Hence, the enzyme cocrystallized in its active (A-TYR) and latent (L-TYR) forms as a crystallographic heterodimer within the same asymmetric unit. The origin of A-TYR in the crystallization batch is unclear since to all intents and purposes only L-TYR was used to set up the crystallization trials. However, minor protease impurities combined with long storage times of the purified protein solution resulting in partial activation may offer an explanation. Owing to the peculiar heteromeric structure, a direct comparison between A-TYR and L-TYR is feasible and allows new insights into the tyrosinase-maturation process. The sodium salt of 6-tungstotellurate(VI) (Na 6 [TeW 6 O 24 ]Á22H 2 O; PDB ligand ID TEW) was crucial for the formation of single crystals and showed an exceptional assembly in this crystal structure. The polyoxoanion [TeW 6 O 24 ] 6À with the Anderson-Evans-type structure was deliberately used as a cocrystallization agent to obtain single research papers crystals suitable for X-ray diffraction. Hence, a detailed description of its binding mode and high-order arrangement is presented herein.

Protein purification and crystallization
Protein purification and crystallization was performed as described elsewhere (Mauracher, Molitor, Al-Oweini et al., 2014;Mauracher, Molitor, Michael et al., 2014). Briefly, the protein was extensively purified from the natural source (A. bisporus fruiting-body stipes) by an extraction method including detergent and aqueous polymer phase separations followed by a subsequent multi-step chromatographic purification procedure via FPLC (fast protein liquid chromatography). Protein purity was checked by SDS-PAGE and mass spectrometry (nano-ESI QTOF). The protein was crystallized by means of the hanging-drop vapour-diffusion technique with a protein concentration of 10 mg ml À1 , a drop volume of 1 ml (0.5 ml protein solution and 0.5 ml reservoir solution) and a reservoir volume of 500 ml. The crystallization conditions were 10% PEG 4000, 1 mM Na 6 [TeW 6 O 24 ]Á22H 2 O, 25 mM Tris-HCl pH 7.5 at 291 K. Crystals grew within 1-5 d to approximate dimensions of 300 Â 30 Â 10 mm.

Data collection and processing
Data collection was performed as described elsewhere (Mauracher, Molitor, Al-Oweini et al., 2014) at Diamond Light Source (DLS), Oxfordshire, England on the monochromatic (0.9173 Å ) MX beamline I04-1. The obtained diffraction data sets were processed with the XDS program package (version March 30, 2013;Kabsch, 2010). Datacollection statistics are given in Table 1.

Structure solution and refinement
Initial phase determinations using molecular replacement (MR) with Phaser from the PHENIX program suite (Adams et al., 2010) were performed using a model of the abPPO3 mushroom tyrosinase structure (PDB entry 2y9w, chain H; Ismaya et al., 2011) modified with the sequence of abPPO4 (UniProt K9I869) derived from a comparative protein structure modelling program (MODELLER; Š ali & Blundell, 1993). As predicted from the Matthews coefficient (phenix. xtriage; 46% solvent content), two molecules fitted in the asymmetric subunit. Notably, in the initial electron-density maps, two highly dense disc-shaped sites were visible, corresponding to the shape of the cocrystallized polyoxoanion [TeW 6 O 24 ] 6À . The rotated and translated model was employed to perform MR/SAD phasing applying AutoSol from the PHENIX program suite. This phase-determination operation was possible owing to the anomalous signal of the cocrystallized POM anion [TeW 6 O 24 ] 6À . The corresponding f 0 and f 00 values of tungsten at the corresponding wavelength (0.92 Å ) are À3.79 and 10.42 e, respectively. The electron density thus generated was used for initial model building. Moreover, the two polyoxoanions were incorporated into the model by placing the structural data of the respective POM and the corresponding restraint data in the PDB file (generated by phenix.reel and phenix.elbow from the crystal structure of TEW; Schmidt et al., 1986). Notably, owing to the positioning of the POMs on a twofold axis their occupancy was set to 50%.
Based on the lack of structural information for the C-terminal domain, the respective model ended with residue Gly379. No electron density was visible extending beyond residue Gly379 of chain A; however, this was not the case in chain B. Several tube-shaped electron-density convolutions were visible in the near-vicinity of Gly379 in a volume of approximately 10.000 Å 3 . Applying the automated modelbuilding and refinement program AutoBuild from the PHENIX program suite indicated two -strands corresponding to the sequence sections Phe428-Tyr447 and Phe482-Tyr498. However, no further reasonable solution was generated using automated modelling programs for the missing residues of the C-terminal domain of chain B. Therefore, we completed the missing chain by placing alanine residues in the vacant electron density and applying intermediate refinement steps (phenix.refine v.1.8.4_1496 from the PHENIX program suite and REFMAC from the CCP4 program suite; Murshudov et al., 2011;Winn et al., 2011). The alanine residues were then successively replaced by the respective amino-acid residues derived from the sequence (UniProt K9I869). While improving the model R values, we repeated phase determination by AutoSol (MR/SAD) with the respective optimized model. This was performed until all of the statistical parameters of the model were in an adequate range for deposition of the structure in the PDB.

Model validation and deposition
Structural models were assessed with respect to the experimental data using SFCHECK (Vaguine et al., 1999).   Table 1 Data collection and processing. 3. Results and discussion 3.1. Overall structure of the asymmetric unit of mushroom tyrosinase abPPO4 The crystal structure of mushroom tyrosinase abPPO4 was solved by combining molecular replacement (MR) and singlewavelength anomalous dispersion (SAD), benefiting from the anomalous scattering signal of the tungsten provided by the cocrystallized POM. In Fig. 1(a) an overall view of the asymmetric unit of abPPO4 is shown. The protein crystallized in space group C2 as a crystallographic heterodimer composed of one polypeptide chain of L-TYR (Ser2-Thr556) and one chain of A-TYR (Ser2-Ser383) as well as two half POM discs ([TeW 6 O 24 ] 6À ). Both POMs lie on a crystallographic twofold axis and show an occupancy of 1.00 generated by two superimposing POM disks (occupancy of 0.5) originating from two oppositely positioned asymmetric units. The final structure was refined to a resolution of 2.76 Å . The complete crystallographic data set is described in Table 2.

Overall structure of abPPO4 A-TYR
The A-TYR chain lacking the C-terminal domain (Ser2-Ser383) has an approximately conical shape tapered at the POM binding site, with a basal diameter of $50 Å and a height of $40 Å (Fig. 1b). The secondary-structure elements are Overall structure. Colour code: L-TYR main core, blue; C-terminal domain, turquoise; A-TYR, purple; sodium ions, yellow; copper ions, bronze; POM (TEW) oxygen, red; tellurium, grey; positive electrostatic potential of coulombic surface, blue; negative electrostatic potential of coulombic surface, red. (a) Overall structure of asymmetric unit; the crystallographic heterodimer of abPPO4. L-TYR is shown on the left and A-TYR is depicted on the right. (b) Illustration of the activation process. By the proteolytic removal of the C-terminal domain the active site becomes solvent-exposed and substrates (e.g. l-tyrosine) are able to approach. (c) Different viewing angle of the single monomer of L-TYR to illustrate the -barrel-shaped C-terminal domain, the proteolytic cleavage site and the putative CXXC motif-containing copper grappler. (d) Coulombic surface illustration of the L-TYR main core with the C-terminal domain (cartoon) attached. The solvent-accessible groove, exhibiting a strong negative electrostatic potential, is indicated by the dashed arrow. Phe454 is shown to protrude into the active site (transparent surface around the active site).
identified and are numbered sequentially ( for -helix, for 3 10 -helix, for -strand and TT for hydrogen-bonded turn; Fig. 2). The A-TYR chain consists of 382 continuous amino acids ending with a cleavage site after Ser383 as determined by mass spectrometry (MS; Mauracher, Molitor, Michael et al., 2014). There are a number of hydrogen bonds present that are not part of the secondary-structure elements. These hydrogen bonds connect the turnover region 4/5 to the -bundle 2/ 3 (Thr114 N to Tyr155 O, d = 2.7 Å ) and the N-terminal end to loop Ile56-Leu86 (Leu3 N to Ala65 O, d = 2.8 Å ), and several others are importantly involved in defining the struc- . In addition to the type-3 copper centre, another metal-binding site, occupied by sodium, is also present (Na1A; Gly55 O, Gly58 O, Pro60 O and H 2 O126/127; Figs. 1b and 4b).
3.2.1. Overall structure of abPPO4 L-TYR. The main core of L-TYR (Ser2-Ser383; Fig. 1c) exhibits a very similar shape to that of A-TYR (Fig. 1b). It has the same conical shape but has the C-terminal domain (Glu384-Gly558) placed on the 'flat bottom' side with approximate dimensions of 50 Â 40 Â 18 Å . A total of 555 continuous amino acids could be assigned to the respective well defined electron density for the L-TYR chain. Only the small disordered C-terminal ending loop is missing (Val559-Thr565). This terminal region has a ragged constitution in that the C-terminal amino acid differs amongst the variants, as demonstrated by MS measurements (Mauracher, Molitor, Michael et al., 2014). The secondary-structure elements on the L-TYR chain are identified and are numbered sequentially ( for -helix, for 3 10 -helix, for -helix, for -strand and TT for hydrogen-bonded turn; Fig. 2). Apart from the same hydrogen bonds as indicated in the main core of A-TYR, three hydrogen bonds between the L-TYR main core and the C-terminal domain are present (Ile380 N to Lys398 O, d = 2.7 Å ; Ala270 N to Arg455 O, d = 2.9 Å ; Glu238 N to Val472 O, d = 2.9 Å ). In addition to the type-3 copper centre, three metal-binding sites, occupied by sodium, were found (Na1A, Gly55 O, Gly58 O, Pro60 O and H 2 O126/127; Na2B, Gly237 O, Asn235 O and Glu331 O; Na3B, Leu348 O, Glu99 O "1 , Arg16 N 2 and Ser96 O ) (Fig. 1c).
3.2.2. Crystal-packing interfaces in A-TYR and L-TYR. PISA (Proteins, Interfaces, Structures and Assemblies; Krissinel & Henrick, 2007) studies have shown that an interface between A-TYR and L-TYR in the asymmetric unit has no probability of formation (complex-formation significance score of 0.00) in solution (Fig. 1a). No strong interactions were predicted for an interface area of 526.6 Å 2 (surface area: A-TYR, 15 388 Å 2 ; L-TYR, 21 827 Å 2 ) with a ÁG value of À0.9 kcal mol À1 and a ÁG P-value of 0.67. However, one hydrogen bond (A Gln149 N "2 to B Thr343 O 1 , d = 3.21 Å ) as well as three salt bridges .76 Å ) are present. In addition to the asymmetric unit interface, six other reasonable interfaces in the crystal packing between protein surfaces, none of which display any reasonable interaction for forming quaternary structures in solution, are described by PISA calculations. Thus, it is assumed that both A-TYR abPPO4 and L-TYR abPPO4 exist as monomers in solution.
The packing is best described as a stack of protein layers by defining the front surface of the layer as the POM-exposed side (Fig. 3a) and the back surface as the protein-exposed side (Fig. 3b). Consequently, two layers are stacked together in a back-to-back fashion oriented in opposing directions. Such a double layer is further stacked via its front side (protein-POM 'sandwich') with another double layer orientated in equivalent directions (Figs. 3c and 3d).
The protein layers are composed in such a way that when an L-TYR chain is viewed centrally and its C-terminal domain is considered to be the head then L-TYR is positioned unidirectionally (head to body; Figs. 3b and 3e). Furthermore, L-TYR is surrounded by five A-TYR chains, of which two are bilaterally positioned at the head (C-terminal domain), two are bilaterally positioned at the body (main core) and one is positioned atop the head (Fig. 3e).
Interestingly, the C-terminal domain of L-TYR is crucially involved in crystal packing. The main cores of A-TYR and L-TYR are not positioned equally. Moreover, as illustrated in Fig. 3(d), a hypothetical attachment of a C-terminal domain to A-TYR would result in a massive clash with the L-TYR main core of another asymmetric unit. Hence, a similar crystal packing for a crystal composed exclusively of L-TYR can be excluded and the present packing is only feasible owing to the heterogeneity provided by the presence of both forms.
3.2.3. Superimposition of A-TYR and L-TYR. The A-TYR and L-TYR chains were superimposed to analyze structural changes induced by the proteolytic removal of the C-terminal domain, which shields the active site (Fig. 4a). However, only small structural changes in the main core were perceivable
research papers Acta Cryst.   Superimpositions. Colour code: L-TYR main core, blue; L-TYR C-terminal domain, turquoise; A-TYR main core, purple; aoTYR main core, green; aoTYR C-terminal domain, lime green; abPPO3 main core, orange; abPPO3 light subunit, yellow; L-TYR abPPO4 copper ions, green; respective superimposed copper ions, red; sodium ions, yellow; water molecules, blue; tropolone, pink; POM oxygen spheres, red. In L-TYR, this loop region occupies a position sideways towards the 'flat bottom' side of the conical main core, which is flipped orthogonally in the A-TYR chain by the hypothetical removal of the C-terminal domain. Interestingly, a metal binding site (Na2B) is lost owing to this side turn. This loop is followed by the 9 helix, which contains two copper-coordinating histidines (His251 and His255); however, almost no conformational change is observed. Only a minor alteration of the side-chain posture is discernible at the two copper-binding histidine positions (Fig. 4c). Following the 9 helix, another loop (Gly259-His266) and a small 3 10 -helix (2) turn into the 10 helix in the antiparallel direction. The 10 helix is host to the HH motif (His282 and His283), which is conserved in tyrosinases and in which His283 coordinates the copper B ion (CuB; Fig. 4c). Apart from a different side-chain orientation (Arg260) and a side-chain flip of His282, no significant conformational change is apparent. Such a change might normally be expected in this region (  proteolytic removal of the C-terminal domain, which could explain the observed copper flexibility (outlined below) of the CuB site of A-TYR.

Active site
The active site of L-TYR exhibits the deoxy-state conformation with a Cu I -Cu I distance of 4.7 Å , and all coppercoordinating histidines (N "2 ) are found at the proper remote distances of around 2 Å (Fig. 5b). A water molecule is positioned on a line between the two coppers. The CuA-CuB distance of 4.2 Å in the A-TYR chain is slightly shorter and the water molecule (occupancy 0.9) is also present but in a triangular position to the two coppers (Fig. 5a). The active site of A-TYR therefore appears to be in the met state, which is defined as the resting state where the two cupric (CuII) ions are bridged via a hydroxide or a water ligand at a distance of approximate 3.4 Å (Solomon et al., 1996). However, as shown previously for a catechol oxidase from grapes (PDB entry 2p3x; Virador et al., 2009), the two coppers here may adopt rather distant (4.2 Å ) positions from each other.
Nonetheless, one distinct residue (Phe454) originating from the loop region right after 11 is clearly protruding towards the CuA site of L-TYR (Fig. 5b). This phenylalanine residue is supposed to act as a placeholder for a potential substrate, as described recently (Fujieda et al., 2013). This has similarly been described previously for a tyrosine residue of the attached caddie protein (ORF378) from S. castaneoglobisporus tyrosinase (scTYR) as well as for a phenylalanine residue from M. sexta pro-tyrosinase and several arthropod haemocyanins (Hazes et al., 1993;Matoba et al., 2006;Li et al., 2009). Therefore, an active-site blocking function of the C-terminal domain in a comparable manner can be supported by the data presented here.
In catechol oxidase structures a bulky residue (mostly Phe) positioned atop the CuA site has been described to be responsible for hindering the monophenolase activity (Klabunde et al., 1998;Matoba et al., 2006). A superimposition of the active sites of ibCO and L-TYR abPPO4 (Fig. 5c) shows that an alanine residue is located at this position in abPPO4, which endorses the aforementioned assumption.
The C "1 atom of His81 and the S atom of Cys79 exhibit a covalent thioether bond in both chains. This exceptional posttranslational modification is common in eukaryotic type-3 copper centres (Gielens et al., 1997). In a recent study of aoTYR, a mechanism for the formation of this thioether bridge owing to the incorporation of copper ions was depicted (Fujieda et al., 2013).
The crystal structure of abPPO4 described here with a crystallographic heterodimeric constitution allows a direct comparison between the two active sites of a latent (zymogen) tyrosinase (L-TYR) and its proteolytically activated form (A-TYR). In Fig. 4(c), a superimposition of the respective active sites is presented.
All three of the histidines coordinating copper A (CuA; His57, His82 and His91), the covalent thioether bridge linking Cys80 to His82, and the CuA sphere superimposed well.
Hence, the CuA site seems to be fixed irrespective of whether or not the C-terminal domain is present. However, the CuBcoordinating histidine side chains (His251, His255 and His283) as well as the CuB ion have only slightly shifted conformations. Interestingly, positive electron density (mF o À mF c ) is observed between CuB and His282 (HH motif) at a distance of 2.3 Å from CuB. Thus, an alternative conformation was assumed for the position of CuB ion in which it is coordinated in a trigonal-pyramidal fashion (nearly tetrahedrally) by four histidine ligands (His251, His255, His282 and His283). His282 is a residue originating from the 10 helix (Figs. 2, 4c and 5a) and is conserved throughout tyrosinases. Thus, a coordination of the CuB ion that includes this seventh His282 may be assumed to be an alternative conformation with a minor probability (CuB2; occupancy 0.09). This would result in a somewhat flexible CuB site. In the inset in Fig. 5(a) the anomalous electron density for the CuB site is shown. Here, a hump of the electron-density sphere around CuB is clearly expanding towards His282, indicating that the density is not caused by water but by an anomalous scatterer. Notably, a similar situation for copper flexibility in tyrosinases was observed for the CuA site in scTYR (Matoba et al., 2006). However, in this case no additional histidine is involved in cooper coordination but one of the involved histidines shows an alternative conformation, resulting in a second binding mode for CuA. Notably, in scTYR no thioether bridge was found for the CuA site.
The observed copper flexibility for the CuB site could contribute to elucidation of the tyrosinase mechanism, particularly the monophenolase activity, which is still not fully understood.

Proteolytic cleavage site
The latent precursor enzyme (L-TYR) is transformed to its active form (A-TYR) by removal of the C-terminal domain (Faccio et al., 2013;Fujieda et al., 2013). The proteolytic cleavage site (post-Ser383), which was precisely determined by mass spectrometry, is located on a loop (Ile380-Asn388) protruding into the surrounding solvent which follows the common tyrosinase YG motif (Mauracher, Molitor, Michael et al., 2014;Figs. 1c, 2 and 4g, inset). This accessible location can be easily approached by a protease of a still unknown origin and type. Similar to aoTYR, a hydrogen-bond interaction between Tyr279 of the conserved YG motif and Arg288 as well as Asp133 of the main core is present in both forms (A-TYR and L-TYR), thus forcing this region to associate with the main core. However, in contrast to the aoTYR crystal structure, the cleavage site is not located on a -helix but on a loop (Fig. 4g, inset). Notably, in contrast to the A-TYR abPPO3, which ends at the YG motif (in the crystal structure), the A-TYR abPPO4 chain continues for an additional four amino acids to Ser383.

C-terminal domain
The C-terminal domain consisting of 182 residues (Glu384-Thr565) contains four -helices, one 3 10 -helix and ten research papers -strands and is attached to the 'flat bottom' side of the main core in such a way that the active site is shielded (Fig. 1d). Curiously, the electron density assigned to the C-terminal domain (Glu384-Thr558) of the enzyme was solely located in the B chain. The electron density for all expected residues was found except for the last seven C-terminal residues (Val559-Thr565). Their absence might be explained by a disordered arrangement. Six long -strands (9-13 and 15) and two short -strands (17 and 18) form a -barrel structure (Fig. 1c). Crucial for the C-terminal shielding function is the region Ile448-Thr455 (starting with 11), which protrudes through the solvent-accessible groove of the active site (Fig. 1d). The residue Phe454 acts as the substrate placeholder, pointing directly towards CuB at a distance of 4.3 Å (C "2 -CuB). Interestingly, the following range of residues (Arg446-Leu471) forms a relatively long loop extending from the main core of the protein. This loop bends with a small angle halfway and integrates again into 12. The conserved tyrosinase CXXC motif of the protein (Cys462-Cys465), which is also a crucial motif in copper chaperones (Davis & O'Halloran, 2008;Robinson & Winge, 2010;Figs. 1c and 1d), is located at its turnover. No disulfide-bonded state of this motif is found, in contrast to the previously reported MS measurements (Mauracher, Molitor, Michael et al., 2014). This motif has been described to be responsible for the incorporation of copper ions into the active site. The proposed mechanism does work in a non-disulfide-bonded state (Fujieda et al., 2013). One can speculate that this part of the C-terminal domain acts as a grappler to supply the active site with copper ions.
A similar -barrel shape was observed for the related structures of aoTYR, the light subunit (UniProt G1K3P4) of abPPO3 (Ismaya et al., 2011;Fujieda et al., 2013) and the caddie protein in the scTRY crystal structure (Matoba et al., 2006). Only low sequence identities and structural similarities to these light subunits are found for the C-terminal domain of abPPO4 (aoTYR, sequence identity 16%, r.m.s.d. C = 4.3 Å ; abPPO3 light subunit, sequence identity 12%, r.m.s.d. C = 14.6 Å ; scTYR caddie, sequence identity 8%, r.m.s.d. C = 11.3 Å ). Apart from the active-site blocking and copperincorporation function, no further purposes of this peculiar domain, which constitutes one third of the whole protein, are known. A structural homology search for the C-terminal domain using the DALI server (Holm & Rosenströ m, 2010) gave structural similarities to lipoxygenases (PDB entries 2p0m and 1lox) and lectins (PDB entries 1ous and 2xr4) in addition to hits for obviously related proteins [aoTYR (PDB entry 3w6w) and haemocyanin (PDB entry 1js8)]. Interestingly, lipoxygenases are similarly constituted to tyrosinase precursors (Oliw, 2002), containing a large 'nonhaem iron centre' active-site domain and a smaller N-terminal -barrelshaped domain (Oliw, 2002). The -barrel domains exhibit a Ca 2+ -stimulated membrane-targeting function (Oldham et al., 2005). The full-length abPPO4 is known to possess a putative transmembrane anchor in the proteolytically removed C-tail region Ala569-Ala591 (Mauracher, Molitor, Michael et al., 2014; Fig. 2). Hence, a membrane-targeting function would be conceivable. Owing to the high similarity of the main core of the tyrosinases (abPPO3, abPPO4 and aoTYR), which preserves the functionality of the enzymes, the contrasting lower similarity of the C-terminal domain might explain a subcellular targeting function that differs between the isoforms. With regard to the structural similarity to lectins as indicated by DALI, it has to be outlined not only that the light subunit attached to abPPO3 has been described as possessing a lectin-like fold, but also that A. bisporus lectin (ABL) was copurified with active mushroom tyrosinase (Rescigno et al., 2007;Flurkey et al., 2008;Mauracher, Molitor, Michael et al., 2014). However, neither a membrane-targeting function nor a carbohydrate-binding function can be shown at this stage, but are indicated as conceivable additional purposes of the C-terminal domain.
3.6. Superimposition of L-TYR abPPO4 with A-TYR abPPO3 In Fig. 4(b), a superimposition of L-TYR abPPO4 with A-TYR abPPO3 (PDB entry 2y9x) is shown. Apart from the loop regions (Gly139-Gly149, Ala72-Cys80 and Leu327-Val332), the two main core structures match very well (r.m.s.d. C = 0.681 Å , r.m.s.d. total = 0.709 Å ). AbPPO3 was crystallized as a tetramer of two heavy subunits (abPPO3) and two light subunits (ORF239342; UniProt G1K3P4). The light subunit, for which no biological role is known to date, has a lectin-like folding and is supposed to attach to all six PPOs in A. bisporus (Weijn et al., 2013). Interestingly, the light subunits of abPPO3 could notionally attach to abPPO4 in such a way that the C-terminal domain of abPPO4 fits perfectly in a vicinal position (Fig. 4d). Thus, a similar attachment of the light subunit to abPPO4 cannot be excluded from a steric perspective. However, there is no evidence that such a quaternary structure would exist, since no light subunit was copurified or detected at any stage during the purification procedure (Mauracher, Molitor, Michael et al., 2014).

Superimposition of L-TYR abPPO4 with L-TYR aoTYR (UniProt B8NJ95)
Although aoTYR has a similar total number of amino acids (616) to abPPO4 (611), the main core consists of 458 amino acids and is significantly larger than A-TYR abPPO4 with 383 amino acids. However, even without the missing putative membrane-orientated C-tail (Ala566-Phe611), the C-terminal domain of L-TYR abPPO4, with 188 (of a total of 228) amino acids, is significantly larger than the C-terminal domain of aoTYR with 158 amino acids. Notably, in the crystal structure of L-TYR abPPO4 some C-terminal residues have no electron density (Val558-Thr565) but were confirmed to be present by MS measurements (Mauracher, Molitor, Michael et al., 2014).
Apart from some small -helices and loop regions, it is possible to superimpose the main cores of the homologous proteins very well ( Fig. 4g; r.m.s.d. C = 1.540 Å ; r.m.s.d. total = 1.411 Å ). Interestingly, the two loop regions (loopX and loopY; L-TYR abPPO4, Asn236-Ser246 and Gly259-His266; aoTYR, Ser299-Asn323 and Gly337-His355) are located before 9 and 10, respectively, representing the -helices where the CuB-coordinating histidines are located, and show similar 'pushed-aside' positions owing to the attachment of the C-terminal domain (Figs. 4g and 4h). As indicated for L-TYR abPPO4 (for loopX), the motion of those loops might have an influence on a conformational change in the active-site region.
The distance between the two copper ions (3.6 Å ) in aoTYR is smaller than in abPPO4 (A-TYR, 4.2 Å ; L-TYR, POM (TEW) binding site. Colour code: L-TYR, blue; A-TYR, purple; O atoms, red; Te atom, grey, W atoms, black; water molecules, cyan; hydrogen bonds, dashed black lines; positively charged coulombic surface, blue; negatively charged coulombic surface, red. (a) POM-binding (L-TYR) site B is located at the tip (start of -helix 5) of the conical-shaped main core. The polyoxoanion lies on a twofold axis (C 2 ) embedded by two opposing HKKE motifs (L-TYR and L-TYR C 2 ). (b) Image of two different views of the one-sided POM-binding site B with the respective electron density indicated by a grey mesh (2mF o ÀmF c , 0.40 e Å À3 , 1 r.m.s.d.) and all possible hydrogen bonds outlined. (c) Coulombic surface image of two opposing asymmetric units (heterodimer, A-TYR/L-TYR abPPO4) sharing two polyoxoanions on a twofold axis. This image illustrates how the POM acts as a conjunction linking two otherwise repulsive surfaces. (c) Image section of crystal packing displaying a sandwich-like constitution (protein layer-POM layer-protein layer). 4.7 Å ). While the full-length aoTYR is described as being in the met state, the L-TYR PPO4 is in the deoxy state (Fig. 4i).
The C-terminal domains of both homologous enzymes constitute a seven--strand barrel fold. However, following the primary chain, the secondary-structure elements and the turnover regions differ more significantly in position and length in comparison to the main core (Fig. 4h). The conserved CXXC motif, described as being involved in copper incorporation into the active site and lacking some electron density in the aoTYR structure, is also located on a loop that appears to be disordered (Arg454-Val472) and protrudes from the C-terminal domain in abPPO4 (Fig. 4g).

POM binding sites
In Fig. 6(c), the two POM binding sites in A-TYR abPPO4 and L-TYR abPPO4 are shown. In both cases, the HKKE motif is located at the beginning of the 5 helix right after a turnover from helix 4 and acts like a claw grabbing the discshaped polyoxoanion (TEW; Fig. 6a). At each POM binding site, one of these HKKE claws from the oppositely located asymmetric unit shares one polyoxoanion. Thus, each polyoxoanion is bound by a total of eight amino acids from two equivalent monomers (A-TYR abPPO4 or L-TYR abPPO4). Both polyoxoanions are positioned on a twofold axis by which two opposing asymmetric units, each providing one HKKE motif, are projected on each other (Fig. 6a). Therefore, it should be outlined that one asymmetric unit contains one heterodimer (A-TYR-L-TYR) and two halves of the nonchiral polyoxoanion (Fig. 6c).
For POM binding site A (A-TYR) the electron density is less defined compared with POM binding site B (L-TYR). In the latter, the POM is very distinctly located on the twofold axis directly between the two HKKE claws (Fig. 6b). Binding site A exhibits a broader electron density perpendicular to the twofold axis. The electron density would offer space for two polyoxoanions that are closely stacked together. However, such a constitution is not possible owing to electrostatic repulsion. Therefore, an alternative position for this polyoxoanion that is not resolved by the electron density is assumed. We refer in the following to POM binding site B since the electron density allows a more precise characterization of the binding situation (Fig. 6b).
Owing to the crystallization conditions at a pH value of 7.5, the lysines involved in POM binding are protonated and hence a hydrogen bond between a lysine N atom and a POM O atom is assumed. The distances of 2.7 Å (N -O22 TEW) and 3.19 Å (N -O23 TEW) for the laterally positioned Lys118 support this assumption. Lys117 is pointing away from the polyoxoanion (4.8 Å for N -O16 TEW); however, only weak electron density for the determination of its actual location is present. In contrast to the lysines involved, His116 is located atop the polyoxoanion with an N " position that is protonated at the given pH. However, a coordinative interaction between the side chain of His116 and the tellurium of the polyoxoanion is not indicated owing to its too distant positioning (5.3 Å ) (Fig. 6b). Distances of 2.7 Å from N " to O8 of the POM are favourable for a hydrogen-bonding interaction. Furthermore, a water-bridged interaction between O " of Glu119 over Wat12 (3.4 Å ) to O12 (2.2 Å ) and O18 (2.4 Å ) is visible (Fig. 6b). In addition to these side-chain interactions, the peptide-bond N atoms (His116, Lys117 and Lys118) are at suitable distances (2.7, 3.0 and 2.8 Å , respectively) to be involved in POM binding (Fig. 6b). No covalent bonds between the POM and the protein were observed as were described for the structure of NTPDase1 cocrystallized with POM (PDB entry 4bvp; Zebisch et al., 2014).
The detailed characterization assigned to the POM binding mode is appropriate owing to the fact that POM binding site B has well defined electron density and a rather low B factor (B TEW_A = 61.8 Å 2 , B TEW_B = 56.1 Å 2 ; Fig. 6b). However, an alternative characterization of the POM binding mode might be described as an electrostatic interaction of a highly negatively charged anion embedded between two oppositely located positively charged protein regions, resulting in a stable interface. In coulombic surface structures of two asymmetric units shown in Fig. 6(c), it is clearly visible that both polyoxoanions bind to regions of the protein with a positive electrostatic potential. Moreover, the POM, owing to its negative charge, connects otherwise repulsive surfaces. This feature comprising a high negative charge on a large rigid molecule makes the TEW polyoxoanion a very suitable agent for the crystallization of otherwise very difficult to crystallize proteins.
In the crystal-packing situation, shown in Figs. 3 and 6(d), it is illustrated how the POM forms a layer between two protein layers, resulting in a sandwich-like formation. Therefore, the situation might be pictured as follows: if a protein forms a stable crystallographic interface on equivalent monomeric sides but therefore exposes repulsive charged surfaces on the other sides, this would result in impossible interface formation for crystal packing. Owing to its unique structure and high negative charge, a polyoxoanion such as [TeW 6 O 24 ] 6À could act as a 'glue' to connect these otherwise electrostatically repulsive surfaces.
Using a large compound in a high charge state as a cocrystallization agent, one can query whether nonphysiological structural changes are implied in a set of respective crystal structures. In the case of the structure described here, we can entirely disprove a conformational change in the structure, in contrast to the POM-induced domain-orientation change in the structure of NTPDase1 cocrystallized with POM (Zebisch et al., 2014). This is owing to the mere fact that the respective POM binding domain (4 and 5 helices) superimposes very well with the comparable structure of mushroom tyrosinase isoform abPPO3 (Ismaya et al., 2011;Fig. 4f).
SGM and AR are grateful to the University of Vienna for financial support of the graduate training program entitled 'Functional Molecules' . Financial support from the 'Fonds zur Fö rderung der wissenschaftlichen Forschung' (FWF) under P25217-N28 is gratefully acknowledged. UK thanks Jacobs University and the German Science Foundation (DFG) for generous support over the years. RA research papers Acta Cryst. (2014). D70, 2301-2315 thanks the German Academic Exchange Council (DAAD) for a PhD fellowship allowing him to pursue doctoral studies at Jacobs University. The EU COST Action CM1203 PoCheMoN is acknowledged. We also thank Prof. Dr Georg Schmetterer, Dipl. Ing. Matthias Pretzler, Aleksandar Bijelic, MSc. and Mag. Gerlinde Grabmann for valuable discussions regarding this work. Special thanks to Dr Alice Douangamath, beamline (I04-1) scientist at Diamond Light Source, Oxfordshire, England, for very kind support during data collection (proposal No. MX8476).