Robust structural analysis of native biological macromolecules from multi-crystal anomalous diffraction data
aNew York Structural Biology Center, NSLS X4, Building 725, Brookhaven National Laboratory, Upton, NY 11973, USA,bDepartment of Physiology and Biophysics, Virginia Commonwealth University, Richmond, VA 23298, USA,cHoward Hughes Medical Institute, Columbia University, New York, NY 10032, USA,dBiochemistry and Molecular Biophysics, Columbia University, New York, NY 10032, USA, and eDepartment of Physiology and Cellular Biophysics, Columbia University, New York, NY 10032, USA
*Correspondence e-mail: email@example.com
Structure determinations for biological macromolecules that have no known structural antecedents typically involve the incorporation of heavier atoms than those found natively in biological molecules. Currently, selenomethionyl proteins analyzed using single- or multi-wavelength anomalous diffraction (SAD or MAD) data predominate for such de novo analyses. Naturally occurring metal ions such as zinc or iron often suffice in MAD or SAD experiments, and sulfur SAD has been an option since it was first demonstrated using crambin 30 years ago; however, SAD analyses of structures containing only light atoms (Zmax ≤ 20) have not been common. Here, robust procedures for enhancing the signal to noise in measurements of anomalous diffraction by combining data collected from several crystals at a lower than usual X-ray energy are described. This multi-crystal native SAD method was applied in five structure determinations, using between five and 13 crystals to determine substructures of between four and 52 anomalous scatterers (Z ≤ 20) and then the full structures ranging from 127 to 1200 ordered residues per asymmetric unit at resolutions from 2.3 to 2.8 Å. Tests were devised to assure that all of the crystals used were statistically equivalent. Elemental identities for Ca, Cl, S, P and Mg were proven by f′′ scattering-factor refinements. The procedures are robust, indicating that truly routine structure determination of typical native macromolecules is realised. Synchrotron beamlines that are optimized for low-energy X-ray diffraction measurements will facilitate such direct structural analysis.
The generation of images of macromolecules from X-ray diffraction of crystals requires the retrieval of phases, which are lost in the recording of X-ray diffraction patterns. When structures of sufficient similarity are already known for molecular relatives, the method of molecular replacement very often provides adequate initial approximations for full structural analysis. Otherwise, phases must be evaluated de novo either by direct methods or by experimental phase evaluation. Until now, the dominant means of de novo phase evaluation has entailed derivatization with heavy atoms such as Hg (Z = 80) for phase evaluation by multiple or single isomorphous replacement (MIR or SIR) or by multi- or single-wavelength anomalous diffraction (MAD or SAD) (Hendrickson, 1991, 1999). Reliable incorporation of selenomethionine (Z = 34) into proteins (Hendrickson et al., 1990) provides particularly efficient de novo structure determination by Se MAD/SAD phasing. For proteins that naturally contain metals, such as Fe (Z = 26), structure determination by native SAD or MAD is often straightforward. Typical anomalous diffraction signals are only a few percent of the normal diffraction signals, and experimental noise from various sources (counting statistics, diffuse scattering, absorption, radiation damage etc.) can obscure the detection of the anomalous differences needed to place the dozens of atomic positions in a typical substructure and then to obtain phases for full structure analysis.
Complications from experimental noise can adversely affect even SAD/MAD analyses of selenomethionyl (SeMet) proteins, and they can be devastating for the feebler anomalous signals from lighter atoms such as sulfur (Z = 16). The problems are exacerbated for crystals that diffract poorly owing to high atomic mobilities. These difficulties are evident in the struggles with SeMet phasing at relatively low resolution and with sulfur SAD phasing even at medium resolution. Such struggles are mostly known only by anecdote, but the effects are evident in the holdings of the Protein Data Bank. As of this writing, more than 5200 de novo SAD structures have been reported in the Protein Data Bank; however, structures determined at relatively higher resolution and with stronger anomalous scatterers (Z > 20) predominate at the 98% level. We can identify only 32 SAD structures at low resolution (dmin ≥ 3.5 Å) and we find only 58 SAD structures based on light-atom (Z ≤ 20) anomalous scatterers (Table 1). This underrepresentation of low-resolution and low-Z SAD structures poses a challenge for crystallographic methods.
Biological macromolecules generically contain low-Z elements that are potentially adequate for effective native SAD experiments: sulfur in proteins and phosphorus in nucleic acids. Proteins on average have methionine and cysteine residues at frequencies of 1.42 and 0.68%, respectively, corresponding to one S atom every 30 residues. Nucleic acids have one P atom per base. Routinely effective native SAD analysis could greatly reduce the uncertainties and complications that arise from heavy-atom derivatization and incorporation. The concept of native SAD phasing was first demonstrated three decades ago by the resolved anomalous phasing of crambin (Hendrickson & Teeter, 1981). SAD as we now know it emerged as density-modification procedures (Wang, 1985; Cowtan & Main, 1993) became effective for breaking the phase ambiguity intrinsic to single-source phase evaluation, as in an application to neurophysin (Chen et al., 1991). Its extension to sulfur-SAD phasing evolved with feasibility tests on lysozyme (Dauter et al., 1999) and the de novo analysis of obelin (Liu et al., 2000). Substantial advances have been made during the past 30 years; among these are the inverse-beam mode of data collection (Hendrickson et al., 1989), the use of highly redundant data collection (Dauter & Adamiak, 2001; Weiss et al., 2001), the use of longer wavelengths (Yang et al., 2003), the use of special crystal mounts (Kitago et al., 2010; Sugahara, 2012), the use of a fine-slicing low-noise detector (Mueller et al., 2012) and other developments (as reviewed in Dodson, 2003; Dauter, 2006a). Nevertheless, as shown in Table 1, the output of light-atom-only native SAD structures has been low and largely restricted to crystals that diffract very well. It appears that difficulties in making accurate measurements of the weak anomalous signals from native biological macromolecules adversely affect the outcomes.
In attempting to enhance the signal-to-noise ratio for anomalous diffraction experiments, one can contemplate increasing the anomalous signal strength and also reducing the noise. For resonant-edge experiments, such as those used for SeMet proteins, anomalous signals might be strengthened through enhanced energy resolution. For light-atom experiments, as for sulfur SAD, the signals might be enhanced through the increase in the f′′ scattering strength at lower X-ray energy. In either case, noise that obscures weak signals might be reduced through the averaging of diffraction data. To increase the multiplicity within the constraints of radiation damage, we have adopted the approach of measuring data from several statistically equivalent crystals. In previously addressing difficult phasing problems at low resolution, we were able to solve a relatively large and poorly diffracting SeMet protein structure by merging data sets from eight crystals at 3.5 Å resolution (Liu, Zhang et al., 2011). We showed that various measures of anomalous signal accuracy were improved substantially with multi-crystal data and that averaged data robustly supported both substructure determination and phasing.
Here, we have devised robust procedures for multi-crystal native SAD experiments at lower than usual X-ray energy. We used these procedures to solve five protein structures varying in size (127–1200 ordered residues) and the number of anomalous scatterers (4–52) at modest resolutions (2.3–2.8 Å). The five applications are diverse. HK9S is an example that could not be labeled with SeMet owing to nonexpression or expression in inclusion bodies. Netrin G2 is a human protein and various heavy-atom derivatizations did not yield satisfactory electron-density maps. CysZ is a novel membrane transporter. TorT–TorSS is a heteromeric protein–protein complex at a relatively low resolution of 2.8 Å. DnaK–ATP is the largest de novo native SAD structure, with 1200 ordered residues in the asymmetric unit. The structure determinations are summarized in Table 2. Results from the analysis of four of them have recently been published separately (Liu et al., 2012). Here, we use the application to DnaK–ATP to illustrate the process of multi-crystal native SAD phasing. We also use the combined experience from the five applications to characterize features of solvability, radiation damage and identification of light-element ions (Na+, Mg+, Cl−, K+ and Ca2+) from the refinement of f′′ scattering factors. We conclude that robust structure analysis of native biological macromolecules is feasible when SAD data from multiple statistically equivalent crystals are combined appropriately.
Details of the production of proteins and crystals for the HK9S, netrin G2, CysZ and TorT–TorSS analyses are described in the supplementary material of our previous paper (Liu et al., 2012) and in the associated structure reports (Brasch et al., 2011; Moore & Hendrickson, 2012; Qi et al., 2013). Many of the procedures used for data collection, data reduction and structural analysis have also been described previously. Here, we use the specific application to DnaK in complex with ATP (DnaK–ATP) in order to demonstrate the procedures that are employed.
For this study, we used a nearly full-length construct from the bacterial Hsp70 chaperone DnaK from Escherichia coli with two mutations. Detailed protein-construct description and protein production will be published separately (Qi et al., 2013). Briefly, a DnaK construct encoding residues 1–610 was affinity-purified and concentrated to 10–20 mg ml−1 in a buffer consisting of 5 mM HEPES pH 7.5, 10 mM KCl and then brought to 5 mM magnesium acetate, 2 mM ATP just before being set up for crystallization. DnaK–ATP crystals were grown at 277 K by the hanging-drop vapor-diffusion method. An equal volume of protein solution was mixed with well solution consisting of 1.8–2.0 M ammonium sulfate, 0.1 M HEPES pH 7.5, 2–3% PEG 400. For cryocrystallography, the crystals were briefly soaked in well solution supplemented with 15% glycerol and were then flash-cooled in liquid nitrogen for data collection at 100 K. Standard Hampton loops were used for crystal mounting and, since the crystals were relatively large, no special precautions were taken to remove cryo-solution around the crystals.
X-ray diffraction data were collected from the five best-diffracting crystals using an ADSC Q4R CCD detector on beamline X4A at the National Synchrotron Light Source (NSLS). The X-ray wavelength was tuned to the Fe K edge (λ = 1.743 Å) as verified by fluorescence scans. The inverse-beam mode of data collection was used; the crystals were rotated 180° every ten frames to measure Friedel mates. Each frame had a rotation angle of 0.5°. A total of 400 × 2 frames were collected from each of the five crystals, with an exposure time of 12 s per frame.
Single-crystal data sets were processed using the XDS (Kabsch, 2010a,b) and CCP4 (Winn et al., 2011) programs POINTLESS and SCALA (Evans, 2011). Frames for a single crystal were indexed and integrated by XDS. The same crystal orientation matrix was used for both sides of the inverse-beam sweeps. Integrated intensities were then corrected by XDS for detector modulation, radiation damage and absorption. Bijvoet pairs were treated differently during all corrections and were kept separate after XDS. The CCP4 programs POINTLESS and SCALA were then used for further data combination, scaling and merging. Ambiguities in multi-crystal data sets owing to random indexing among crystals were resolved by re-indexing in POINTLESS before combining. Reduction of single-crystal as well as multi-crystal data was carried out using SCALA. During data reduction, Bijvoet pairs were treated as equivalent reflections during scaling but were treated separately during merging. Rotational scale and B-factor restraints were used with corrections for secondary beam and absorption. After processing of single-crystal data sets, unit-cell parameters and diffraction intensities were used for outlier crystal detection and rejection by clustering analyses (Liu et al., 2012). Compatible data sets were then scaled and merged together by SCALA. Relative anomalous correlation coefficients (RACCs) of individual data sets to the merged data set were calculated for further outlier crystal rejection. For RACC calculations, data were truncated at 3.5 Å resolution. Data sets with RACC values below 35% were rejected from further analyses. After outlier crystal rejection, the remaining data sets were reordered according to their RACC values and were progressively merged either from the best to the worst or from the worst to the best for structure-determination attempts. The program CTRUNCATE (French & Wilson, 1978; Padilla & Yeates, 2003) was used to convert merged intensities to structural amplitudes with Bijvoet pairs separated. Data-collection and reduction statistics for single-crystal and multiple-crystal data sets are listed in Table 3.
‡Rp.i.m. is the precision-indicating (multiplicity-weighted) Rmerge as reported from SCALA.
§I/σ(I) = 〈〈I(hkl)〉/σ[〈I(hkl)〉]〉, where 〈I(hkl)〉 is the weighted mean of all measurements for reflection hkl and σ[〈I(hkl)〉] is the standard deviation of the weighted mean. The values are as reported from SCALA as Mn(I/sd).
¶Rank of the anomalous correlation coefficient of individual data sets to the merged data.
††ΔF/σ(ΔF) is the average anomalous signal from data truncated to dmin = 3.5 Å. The values are derived using CCP4 programs and are computed by SFTOOLS as 〈|ΔF|/σ(ΔF)〉, where ΔF = |F(h)| − |F(−h)|.
‡‡Anomalous correlation coefficient evaluated from data truncated to dmin = 3.5 Å.
Anomalous center substructures were found by SHELXD (Sheldrick, 2010). SHELXD first derives E-values from Bijvoet-difference amplitudes, |ΔF±h| = ||F(h)| − |F(−h)||, and excludes the weak Eobs data, defined by Emin, from the substructure searches as being ineffective and unreliable. The program uses correlation coefficients (CCs) between Eobs and Ecalc as criteria to evaluate the validity of substructure solutions. CCall is the correlation coefficient based on all data and CCweak is that from the 30% of the weak data which, akin to Rfree, is not used in substructure searches and provides a sensitive measure of validity (Schneider & Sheldrick, 2002). For SHELXD searches, we tried various high-resolution cutoffs from 2.5 to 5 Å in steps of 0.1 Å. Based on these attempts, we used a high-resolution cutoff at 3.8 Å for substructure determination with an Emin value of 1.6 to search for 32 protein sulfur sites by assuming the presence of two DnaK–ATP molecules in the crystallographic asymmetric unit. Attempts were also made using single-crystal data sets as well as their merged data. For each data set, 1000 or 10 000 attempts were made.
The substructures found by SHELXD were refined and completed using Phaser (Read & McCoy, 2011). The log-likelihood gradient maps produced by Phaser were used for substructure completion. This is implemented in Phaser by the LLG complete keywords `COMPLETE ON' and `SIGMA 5.5'. For phasing experiments, initial SAD phases to the data limit were calculated by Phaser. Phases for both enantiomorphs were generated and these phases were then subjected to automatic density modification with solvent flattening and histogram matching as implemented in the CCP4 program DM (Cowtan & Zhang, 1999). Although the crystallographic asymmetric unit contained two DnaK–ATP molecules related by twofold noncrystallographic symmetry (NCS), such NCS was not used for density modification. The estimated solvent content of 68% was used for solvent flattening and no additional treatments were made. After density modifications, the resulting electron-density maps were visually checked to identify the correct hand by looking for more interpretable molecular boundaries and structural features.
For those single-crystal and multi-crystal data sets that did not support successful substructure determinations by SHELXD, the substructures obtained from the merged five-crystal data were used for SAD phasing. Similarly, SAD phases to the data limit were calculated by Phaser and initial phases were density-modified for further analyses.
2.4. Structure refinement and analyses
Initial automatic model building was carried out using ARP/wARP (Langer et al., 2008) starting with experimental electron densities after density modification. Manual model building was carried out using Coot (Emsley et al., 2010) and refinements were performed using phenix.refine (Adams et al., 2011; Afonine et al., 2012). TLS parameters and isotropic B factors were refined without NCS restraints. Friedel pairs were treated as two reflections in refinement. The refined model was validated by PROCHECK (Laskowski et al., 1993) and MolProbity (Chen et al., 2010) to ensure good geometry. To identify anomalous scatterers, Bijvoet-difference Fourier maps were visually inspected. The f′′ values of respective anomalous scatters were then refined against the merged data. The f′′ refinements were performed by phenix.refine with starting values of zero for all anomalous scatterers.
For native SAD experiments, there are various considerations for optimized anomalous signal measurement. Perhaps the most critical parameter of concern is the X-ray energy. Although anomalous signals from light elements increase steadily with decreasing energy, many other properties affect diffraction experiments increasingly adversely with decreasing energy. The advantages of low energy are readily apparent: f′′ for sulfur increases from 0.24 e at the Se K edge (12.7 keV) to 3.05 e at 3 keV, and the profile for phosphorus is similar (Fig. 1a). Factors that militate against this advantage include X-ray absorption, diffuse scattering and large Bragg angles. Absorption of X-rays by air, as in the path of diffracted rays, or by water, as in the crystal sample, diminishes the diffracted rays (Fig. 1b), incoherent scattering into the background increasingly obscures Bragg diffraction as absorption increases at lower energies (Fig. 1c) and, by Bragg's law, lower energy diffraction patterns extend to greater diffraction angles, making for challenging diffraction geometries (Fig. 1d).
There are solutions for many of the complicating low-energy factors. Importantly, both absorption and scattering in the beam paths can be mitigated by replacing air with an atmosphere of helium (Figs. 1b and 1c). With respect to detector geometry, we have already shown that it is possible to record a full 3.2 Å resolution data set at 3.7 keV (U MIV edge) on a flat detector (Liu et al., 2001); however, the preferred solution is to use a shaped (geodesic dome or cylindrical) detector. On the question of absorption in the diffracting sample, it obviously helps to use mounts that present the crystal cleanly (Kitago et al., 2010; Sugahara, 2012); however, the crystal itself is an unavoidable source of absorption, which of course depends on the crystal thickness. Approximating X-ray absorption by macromolecular crystals as that of water (macromolecular crystals are 30–80% water and the absorptivity of proteins and nucleic acids is not far off that of water), we can characterize the trade-off between crystal size and anomalous scattering signal by plotting the transmitted signal as a function of sample size (Fig. 2). Although other factors, including incoherent scattering, absorption in optical elements and windows, detector efficiency and radiation damage, will contribute to energy optimization, crystal size is an important determinant. As such, the optimum for a 200 µm sample is at ∼6 keV, whereas that for a 50 µm sample is at ∼4 keV. To aspire to lower energy and larger transmitted anomalous signals, true microcrystals and microbeams are needed for optimization.
The crystals used for the four initial tests of multi-crystal SAD phasing were in the size range 100–300 µm and we chose to set the energy to 7.112 keV (Fe K edge calibrated by iron-foil fluorescence). The crystals of DnaK–ATP were all 200–300 µm in thickness, where the predicted optimum is in the 6–7 keV range, so we also used the Fe K edge in DnaK–ATP experiments. The inverse-beam mode of data collection (Hendrickson et al., 1989; Clemons et al., 2001) was used, but a helium cone was not used since the DnaK–ATP crystals diffracted very strongly.
When combining diffraction data from multiple crystals, it is important to assure that the data sets to be merged are statistically compatible with one another. We did not find any incompatible data sets in our previous eight-crystal SeMet SAD phasing (Liu, Zhang et al., 2011), which was at relatively low resolution (dmin ≥ 3.5 Å); however, the current native SAD studies are based on weaker signals and are at higher resolutions. Thus, more stringent standards for crystal uniformity might be needed. We thus devised three tests for statistical equivalence and applied them for outlier rejection. The results of these tests for our four initial applications of multi-crystal SAD phasing have been described previously (Liu et al., 2012). Here, we show the comparisons for the DnaK–ATP crystals. Except for one CysZ crystal, all of the other crystals used in these five structure analyses are statistically compatible and contribute collectively.
Our first criterion for crystal compatibility is a unit-cell deviation analysis. In the particular case of DnaK–ATP crystals, which belong to space group I422, we first used the two variable unit-cell parameters a and c to calculate Euclidean distances between pairs (j, k) of crystals. These distances were then used to construct a distance matrix, normalized by population variances, which was used for a clustering analysis for the five crystals (Fig. 3a). Crystals 1 and 3 form one cluster and crystals 2, 4 and 5 form a second cluster, which appeared to be compatible for averaging at an inter-cluster distance just over 2σ. When a large number of crystals are available, structural analyses for individual clusters may be informative.
Our second criterion was a further check by diffraction dissimilarity analysis. We define diffraction dissimilarity as 1 − PICC, where the paired intensity correlation coefficient (PICC) is the correlation coefficient between intensities in a pair of diffraction patterns. Bijvoet pairs were averaged for PICC calculations, and for DnaK–ATP the high-angle data were truncated to 3.5 Å resolution. The 1 − PICC distances were used directly for clustering analysis by searching for the maximum distances between two clusters. From the diffraction dissimilarity clustering (Fig. 3b) the five crystals differ very little, all within 0.5%, indicating that these five crystals are compatible.
Our third criterion is a test on anomalous diffraction signals. Anomalous differences from our native SAD experiments proved to be too small for useful pairwise analysis, so we devised a relative anomalous correlation coefficient (RACC) whereby the merged Bijvoet differences |ΔF±h| in the data set from an individual crystal are compared with those in the merged data set averaged from all crystals. For DnaK–ATP, high-angle data were truncated to 3.5 Å resolution for RACC calculations and the results are shown with crystals ordered by RACC rank (Fig. 3c). The top two crystals have RACC values over 70% and the lowest still shows a significant contribution at 44%, again implying that all five crystals are compatible with one another. To optimize structure-determination efficiency, we reordered the crystals on the basis of their RACC values (Table 3).
Although each criterion may have its limitations and could falsely reject or retain crystals, we find that in general, as here for DnaK–ATP, these criteria are consistent with one another. Based on experience from these five native SAD structures, we suggest that a unit variation of <3σ, a diffraction dissimilarity of <5% and an RACC of >35% are acceptable values for including crystals. Meeting all three criteria reinforces the assurance that all merged crystals are statistically equivalent. While it seems advantageous to reject data from outlier crystals, the process is robust even to the inclusion of outliers. As long as the number of crystals is large, a few outlier crystals are unlikely to affect overall SAD phasing results.
In order to assess the strength of diffraction signals during the course of our native SAD phasing analyses, we followed three statistical measures: the anomalous correlation coefficient (ACC), which compares two randomly selected subsets from a data set, the average Bijvoet difference 〈|ΔF|〉 normalized by the normalized standard deviation σ(〈|ΔF|〉) of that averaged difference, which we denote simply as ΔF/σ(ΔF), and the average diffracted intensity 〈I〉 normalized by the standard deviation σ(〈I〉) of that averaged difference, which we denote simply as I/σ(I). Results from the progressions in adding of crystals in our first four applications of native SAD phasing have already been reported (Liu et al., 2012), and here we describe results from progressions in the DnaK–ATP analysis.
ACC values were used as reported by the CCP4 program SCALA and they are strongly resolution-dependent. For the single-crystal data sets, ACC values approach 45–60% at low scattering angles and then fall below 10% for Bragg spacings greater than 4.5 Å (Fig. 4a); however, the ACC values were substantially enhanced across all Bragg spacings upon merging of the five single data sets, with progressive enhancement as data were added crystal by crystal from the best to the worst (Fig. 4b). Even the worst crystal 5′ helped to increase the ACC. Overall, the ACC increased from 14.2% for the best single crystal 1′ to 41.8% for the merged data (Table 3).
Profiles of ΔF/σ(ΔF) with respect to Bragg spacings also demonstrated enhancements of anomalous signals from the inclusion of multiple crystals. As for ACC, there is a marked improvement in anomalous signal-to-noise ratios upon merging (Fig. 4c) and this is again progressive with crystal-by-crystal mergings (Fig. 4d). The best single-crystal data set, from crystal 1′, is appreciably stronger than all others; yet nevertheless the merged data set shows strongly enhanced signal to noise even relative to this best single set. Overall, ΔF/σ(ΔF) for the merged data to 3.5 Å spacings was enhanced by a factor of 1.52 over the 1′ data set (Table 3). Moreover, even the worst single-crystal data set, from crystal 5′, still boosts ΔF/σ(ΔF) by 12% over the 1′–4′ merging.
I/σ(I) values provide measures of signal to noise in overall diffraction and they thus define the limit of measureable diffraction. This limit is at 2.3 Å Bragg spacing for DnaK–ATP (except for crystal 5, which was truncated at 2.5 Å). As for ACC and ΔF/σ(ΔF), the I/σ(I) profiles also increased dramatically for merged over individual data sets (Fig. 4e) and progressively upon addition crystal by crystal (Fig. 4f). The notable difference is the extension to higher resolution for overall diffraction compared with the much weaker anomalous diffraction signals.
The first step in native SAD phasing is to determine the substructure of anomalous scatterers. For these studies, we have used the combined Patterson search and Shake-and-Bake dual-space refinement of SHELXD (Sheldrick, 2010). Details of substructure determinations for the first four native SAD phasing studies have been reported previously (Liu et al., 2012); thus, we concentrate here on the DnaK–ATP studies to illustrate the procedures. As in the other applications, optimized SHELXD parameters feature a resolution cutoff substantially reduced from the diffraction cutoff: to 3.8 from 2.3 Å for DnaK–ATP.
Compared with other cases, the DnaK–ATP crystals proved to be quite recalcitrant to substructure determination. We first performed tests with 1000 attempts for each data set in the crystal-by-crystal progression and found no solutions until data from all five crystals were merged. Subsequently, we increased the number of tries to 10 000 per data set. We found no solutions for any of the single-crystal data sets even at this level; however, we did then find solutions for the four-crystal cases both in the best-to-worst order (1′ to 4′) and in the reverse order (5′ to 2′), as well as the five-crystal case (Tables 4a and 4b). In all cases, the vast majority of attempts resulted in candidate solutions characterized by correlation coefficients CCall and CCweak clustered at 15 ± 1% and 2 ± 1%, respectively. True solutions have correlation coefficients that are significantly higher than this random background; in the four-crystal 1′ to 4′ case, 20 successful solutions emerged with CCall/CCweak values of up to 37.2/22.4% and adding the fifth crystal further improved the success rate and CC values (Table 4a).
‡Figure of merit.
§Correlation coefficient between experimental (no density modification) and model-phased maps.
¶Correlation coefficient between experimental (density-modified) and model-phased maps.
††The number of residues built by ARP/wARP versus ordered residues in the refined model.
‡‡Reported by ARP/wARP.
As an aside, it is worth noting that a single successful SHELXD solution suffices for substructure determination. Each of the successful candidates can produce a correct substructure, but identifying even one is a challenge when the success rate is low. The success rates for DnaK–ATP (0.4% for the five-crystal case) were significantly worse than in the other multi-crystal native SAD experiments (from 0.7% for TorT–TorSS to 35% for HK9S; Liu et al., 2012). The success rate is a function both of the signal-to-noise ratio, which is improved by the inclusion of additional crystals, and of substructure complexity, which is an intrinsic complication. Based on the protein composition and assuming two DnaK molecules per asymmetric unit, 32 S atoms were expected; however, the actual refined substructure included 52 atoms of varying strength (Table 2). Lower success rates can be expected as the substructure size increases.
To further check the robustness of substructure determination, we merged the data into eight successive wedges (Table 5a) and used the accumulative wedged data in substructure-determination trials (Table 5b), using the same parameters as for the crystal-by-crystal trials. Although each 50-frame wedge was at least 99.5% complete, none of the individual wedges supported substructure determination. Furthermore, there were no solutions from accumulative mergers through the first three wedges (frames 1–150); however, successful solutions were obtained from mergers of four or more wedges. In Fig. 5, we plot the CCall and CCweak distributions from accumulative wedged data sets wedge 1 to wedges 1–8, singling out the successful solutions. Comparing Tables 4(a), 4(b) and 5(b), it can be seen that with accumulative wedged data an overall multiplicity of 74.1 can suffice for substructure determination, whereas with crystal-by-crystal mergers a higher overall multiplicity of 123.3 seems to be needed. We presume that the improved performance from wedged data merging is a consequence of the reduced level of radiation damage in this approach.
Phase determination can proceed once a substructure is known, whether or not the particular data set supported substructure determination. The substructures found from various conditions are all essentially the same except for shifts of the origin and enantiomorphic changes. Therefore, the substructure from the five-crystal data set was used in each subsequent DnaK–ATP phasing test. Initial SAD phase calculations were performed by Phaser and phase improvement was performed by density modification with DM. Automatic model building into resulting DM-modified electron-density maps was performed with ARP/wARP. The structure based on the five-crystal data set was refined with PHENIX. Phasing effectiveness was evaluated by the figure of merit (FOM), by map correlation coefficients (MapCC) comparing experimental electron-density maps with the map produced from the ultimate refined atomic model and by the fraction of ordered structure that could be built by ARP/wARP.
SAD phasing tests were performed based on each data set described in Tables 4(a), 4(b), 5(a) and 5(b) using the five-crystal substructure for each. The final electron-density map from the five-crystal data set itself was excellent, giving a MapCC of 85.3% and automated building of 1117 of the 1200 residues (93%) for the DnaK–ATP structure. Even the SAD-phased map without DM modification gave a MapCC of 46.6%. We also found that data sets that did not support substructure determination on their own could support overall structure determination when given the substructure of anomalous scatterers. Thus, single data set 1′ gave a MapCC of 73.0% and an 88% autobuilt atomic model. Only data from single-crystal set 5′, the worst crystal, and the single-wedge data sets other than wedge 1 did not support automated structure determination efficiently (40% autobuilt for crystal 5′, 39–47% for wedges 2 through 8). With the addition of data, either crystal by crystal or wedge by wedge, progressive improvements followed in the monitors of phasing effectiveness.
There are complications in measuring the effectiveness of SAD phasing in that the quality of a resulting map is a function of the density-modification protocol as well as the anomalous phasing efficacy. Moreover, automated map interpretability depends on the fitting algorithm as well as the map quality. These complications are evident in the enhancement progressions of our tracking parameters. The overall enhancements from the single crystal to five-crystal determinations are 34% for FOM; 29% for MapCC before DM; 17% for MapCC after DM and 5% for residues built correctly for the RACC-ordered progression (Table 4a); 62, 91, 90 and 132%, respectively, in the reverse-ordered progression (Table 4b); and 46, 40, 31 and 5%, respectively, for the wedge-by-wedge progression (Table 5b). For the RACC-ordered progression, MapCC values after DM do not improve after the 1′ to 3′ merger and the number of autobuilt residues is already at 88% after the first crystal, 1′ to 1′. Provided that starting SAD phases are of sufficient quality, density modification can proceed to completion; similarly, automated model-building procedures can proceed to completion by injecting atomic refinement information. From these results, ARP/wARP succeeds at the 90% level when MapCC is above ∼35% before DM (∼70% after DM). FOM and MapCC before DM are purely dependent on the anomalous scattering, but they underestimate the SAD phasing efficacy since they are affected by phase ambiguity. Perhaps the intrinsic figure of merit from bimodal phase probability distributions (Hendrickson, 1971) could be used as a better measure. In any case, it is important to stress that the initial maps for 17 of the 26 tests represented in Tables 4 and 5 could not have been produced were it not for the substructure, which required a minimum of four crystals. Clearly, substructure determination was the most challenging aspect of native-SAD phasing for DnaK–ATP.
To visualize the phasing results, we plotted experimental electron densities from the five single-crystal data sets and from the merged five-crystal (1′ to 5′) data set (Fig. 6). Crystal 1′ shows reasonably continuous electron-density coverage for the main chain and for most side chains (Fig. 6a), while electron density for the worst crystal, 5′ (Fig. 6e), would be hard to interpret without being guided by the model. Other crystals showed intermediate density quality. In contrast, the merged five-crystal data set gave strikingly superior electron-density coverage of the model. Similarly, the five-crystal density for the Mg2+-ATP complex is better than for any single-crystal case, although even crystal 5′ is interpretable (Fig. 7). It must be emphasized again that the single-crystal maps depend on assuming a substructure determined from multiple crystals.
Native SAD phasing of proteins can be considered to be sulfur SAD phasing since the S atoms of methionine and cysteine residues are the predominant light atoms in proteins. In our present studies, however, we find that light atoms present in ligands and associated ions are also usually present (Table 2), and in the case of DnaK–ATP these comprise nearly 40% of the anomalous substructure. The additional sites appear unavoidably from the substructure determination, and their probable identity can often be assigned from the chemical environment. However, independent assurance is also possible. We show here that positive identifications are possible based solely on the anomalous scattering signals at a single X-ray energy remote from the absorption edges.
DnaK is an Hsp70 molecular chaperone and its ATPase activity is critical for its function in protein folding (Qi et al., 2013). For this study, a hydrolysis-deficient mutant protein was crystallized in the presence of 10 mM KCl, 5 mM magneisum acetate, 2 mM ATP and 1.8–2.0 M ammonium sulfate. The SHELXD analyses returned 45 sites, and the 32 strongest were used for substructure completion and initial SAD phasing by Phaser assuming an all-sulfur substructure. After model refinement by PHENIX, we generated Bijvoet-difference Fourier maps to cover the two DnaK molecules in the asymmetric unit and used the CCP4 program PEAKMAX to find the 60 strongest peaks above 3σ (Fig. 8). By comparing the peak-height profile from the five-crystal data set with the refined atomic model, we matched 32 peaks to protein S atoms, 12 peaks to 11 sulfate ions (one sulfate has two mutually exclusive positions), six peaks to the P atoms of two ATP molecules and two to ATP-associated Mg2+ ions. The weakest of these matches, at 5.2σ, is of peak 52 with the Mg2+ ion of molecule A. This peak coincides with a magnesium ion coordinated octahedrally by four water molecules and by the β and γ phosphate groups of this ATP molecule (Fig. 7); peak 45, at 8.4σ, corresponds to the Mg atom of molecule B (Fig. 8). Incidentally, the comparison of Bijvoet-difference peak profiles from the five-crystal merger versus those from the five single-crystal data sets (Fig. 8) provides yet another demonstration, beyond those of Fig. 4, of the power of multi-crystal averaging.
Conventionally, the positive identification of atomic elements from anomalous scattering has entailed measurements above and below an absorption edge or, for lighter elements where measurements at the edge are not readily feasible, the use of heavier same-group replacements such as Br− for Cl−, Rb+ for Na+ or K+, and Sr2+ or Yb3+ for Ca2+ or Mg2+ with measurements above the surrogate edge. Because of wide differences in atomic mobilities (B factors), element identifications from peak heights in Bijvoet-difference Fourier syntheses (Fig. 8 here and Fig. 2 in Liu et al., 2012) are fraught, and for ionic species the chemical environment may not be decisive for identification. Thus, we devised a highly effective alternative strategy for these studies. We first carried out refinements of models of the postulated elemental species with Friedel mates averaged; then, again using phenix.refine (Afonine et al., 2012), we followed this with refinements against Friedel-separated data but now including elemental f′′ values as variable parameters. Results of scattering-factor refinements for our five native SAD structures are presented in Table 6. The refinements converged to almost the same values whether started as here with all f′′ values set to zero or with initial values of 0.699 e, the theoretical f′′ for sulfur at the Fe K-edge energy. The process is robust because atomic positions, occupancies and B factors are largely determined by the normal scattering components, whereas the fitting of deviations from Friedel's law requires accurate anomalous scattering factors.
For many of the sites in these five structures, the identity of the anomalous element is not in question. Sulfur is such a case, of course. Thus, by comparing the refined sulfur f′′ values with the theoretical value calculated from first principles, one obtains a check of the refinement procedure. The five fitted f′′(Sprotein) values average 0.630 ± 0.025 e, which is within 3σ of the theoretical value of 0.699. It is low, however, by a factor of 0.90, which is similar to the average factor by which the other eight entries in Table 6 are low. Although its origins are unclear, this underestimation does not preclude clear-cut identification of anomalously scattering elements. Notably, the refined f′′ value clearly identifies the Mg2+ sites in DnaK–ATP, consistent with the Bijvoet-difference map (Fig. 7). In contrast, previous anomalous diffraction analyses of Hsp70 complexes with Mg2+-ADP did not show detectable signals for Mg (Wilbanks & McKay, 1995; Arakawa et al., 2011). Moreover, although K+ was expected in DnaK–ATP, being relevant for DnaK function and being found bound in complexes of Mg2+-ADP with Hsp70 (Wilbanks & McKay, 1995; Arakawa et al., 2011) and of Mg2+-ATP with Hsp110 (Liu & Hendrickson, 2007; Polier et al., 2008), the results from Fig. 8 and Table 6 definitively rule out its presence as an ordered component of DnaK–ATP.
The multi-crystal native SAD procedures described here were devised in the context of applications to five structure determinations (Table 2), and the resulting structures are shown as ribbon diagrams in Fig. 9. Structures from three of these analyses, and their associated biological implications, are described in full elsewhere (Brasch et al., 2011; Moore & Hendrickson, 2012; Qi et al., 2013) and descriptions for the other two are in preparation; the initial four structures were also shown in our previous account of this work (Liu et al., 2012). The five structures range from 127 to 1200 ordered residues, are in crystal lattices from monoclinic to trigonal to tetragonal, have resolution limits from medium at 2.3 Å to low at 2.8 Å and contain systems such as a molecular machine (DnaK), a membrane protein (CysZ) and a protein–protein complex (TorT–TorSs). The range of these applications indicates substantial generality and robustness.
Solving macromolecular structures without needing to incorporate any kind of non-native atom or having a known structural relative is an aspirational idea. Although the proof of concept was demonstrated over 30 years ago (Hendrickson & Teeter, 1981) and structure determination by SAD was already exploding ten years ago (Table 1) on the way to its current dominance for de novo structure determination, native SAD phasing has not been routinely feasible: witness the fewer than 60 light-atom-only SAD structures in the PDB. Several challenges have thwarted routine de novo structure determination and we discuss them here in the context of our approach to native SAD phasing from the merged data of multiple crystals.
Both because of relatively low signals from light-atom anomalous scatterers and also owing to noise contributions from incoherent scattering at lower X-ray energies, native SAD experiments present challenging signal-to-noise ratios. A protein of 250 residues has approximately eight S atoms on average, which will produce a Bijvoet-diffraction ratio (ΔF/F) of only ∼1% for data collected at the Fe K edge (E = 7.112 keV). These are very small signals and they require low noise levels for reliable detection. On average, since σ(ΔF) = 21/2σ(F), if ΔF = q|F| then ΔF/σ(ΔF) = (q/21/2) × [F/σ(F)], I/σ(I) = (1/2) × [F/σ(F)]; thus, to achieve ΔF/σ(ΔF) = a, one requires I/σ(I) = (21/2/2) × (a/q). Thus, at the 1% signal level, to achieve a signal-to-noise level of 1 in average Bijvoet difference, ΔF/σ(ΔF), requires that I/σ(I) be at the level of 70. Typical macromolecular diffraction experiments have overall I/σ(I) values in the range 10–30, well below the required accuracy. Signals can be enhanced by further lowering the X-ray energy (Fig. 1a); however, the background noise then increases owing to enhanced scattering from samples, mounts, windows and flight-path gases. Such noise can be reduced by experimental design, for example by using a helium beam path (Fig. 1b), and obfuscating systematic errors can be minimized by strategies such as inverse beam. Noise from random errors can be minimized by increasing the data multiplicity; however, radiation damage limits crystal lifetime and thus single-crystal multiplicity.
The use of multiple crystals seems to be effective for achieving high-multiplicity signal-to-noise enhancement without excessive radiation damage (Liu et al., 2011). The DnaK–ATP structure determination illustrates the advantages of native SAD experiments well. These crystals have 32 protein S atoms and we find 52 actual anomalous scatterer sites. The calculated Bijvoet-diffraction ratio is close to the value for an average protein: 0.9% and 1.1% at the Fe K edge for the respective alternatives, assuming fully occupied sulfur sites; thereby the overall I/σ(I) of individual data sets ranged between 29.1 (data set 5) and 37.0 (data set 4) (Table 3), which are all insufficient to provide a signal-to-noise ratio of 1 in ΔF/σ(ΔF); indeed, none of these data sets supported substructure determination by SHELXD. After assuring statistical equivalence among individual data sets (Fig. 3), we merged them into the five-crystal data set, which has an I/σ(I) of 64.5 overall and 16.2 in the outermost shell (Table 3). Bragg spacings for the five-crystal data set still extend beyond 3 Å when truncated at I/σ(I) > 70, our estimate for signal to noise above 1, and the merged data gave reliable substructure determinations for truncations anywhere between 3.5 and 4.5 Å, where I/σ(I) values are above 100 (Fig. 4e).
Another approach that has been proposed for improving accuracy in sulfur anomalous diffraction experiments is a multi-data-set merging procedure (Liu, Chen et al., 2011). Here, the averaging of N data sets exposed at a rate x/N is shown theoretically and in practice to improve upon results from a single data set exposed at a rate x. From theory (Liu, Chen et al., 2011), the impact of this multi-data-set procedure is expected to be greatest for intense reflections, which is consistent with an asymptotic I/σ(I) for intense reflections (Diederichs, 2010; Liebschner et al., 2012). We have not performed multi-data-set experiments in this study, but one can expect beneficial complementarity if used in multi-crystal experiments. Nevertheless, for radiation-sensitive samples a single crystal may not suffice, whereas data from multiple crystals can overcome radiation damage and improve phasing efficacy.
Native SAD phasing is a two-step process, requiring first determination of the substructure of anomalous scatterers and then the phasing procedure to define the full atomic model. Both steps need accurate anomalous signals and failure in either step normally prevents structure determination, although occasionally one can use initial phases from other sources for substructure determination, as in MR-SAD (Schuermann & Tanner, 2003; Panjikar et al., 2009; Read & McCoy, 2011). Thus, for a typical native SAD structure determination there are two possible bottlenecks. One is the substructure determination, especially if the anomalous substructure is large, and the other is phasing effectiveness if the anomalous substructure is relatively small.
The DnaK substructure has 52 anomalous scatterers, which is relatively high, and substructure determination was the bottleneck in this case. Fig. 10(a) plots the successful SHELXD CCweak values and model correctness for structure determination of data merged crystal-by-crystal as in Table 4(a). SHELXD could not find a substructure until data were merged from four or five crystals. Once the substructure had been determined, however, it could be used for successful phasing with all other data sets (1′ to 1′, 1′ to 2′, …, 1′ to 5′), resulting in similar model completeness and model correctness (Table 4a and Fig. 10a). This again demonstrates that the substructure determination is the rate-limiting factor of multi-crystal native SAD phasing for DnaK and the substructure solvability is four crystals, either when combined best to worst (Table 4a) or worst to best (Table 4b).
In contrast to DnaK, the bottleneck for solvability with HK9S was phasing efficacy instead of substructure determination. Fig. 10(b) plots the course of structure determination for HK9S with data merged crystal-by-crystal from best to worst. The four-atom substructure of HK9S could be found by SHELXD from as few as two data sets, although three or more data sets gave more reliable substructures and much higher SHELXD CCweak values. Moreover, success rates were much higher than for the DnaK analysis: 35% for the six-crystal HK9S experiment compared with 0.36% for the five-crystal DnaK experiment. On the other hand, this substructure could not support successful SAD phasing until five- or six-crystal data were used. The quality of maps improved only gradually with added crystals as measured by automatic building by ARP/wARP (Fig. 10b), remaining below 80% model correctness for fewer than five crystals, whereas with six crystals 98 out of 127 ordered residues could be built automatically with a model correctness close to 100%.
These contrasting examples illustrate differing kinds of barriers to structure solution from native SAD data. Although the sticking points for DnaK and HK9S structure determinations differed, it was the signal-to-noise enhancements from multi-crystal averaging that proved to be crucial for both. There is no apparent disadvantage in adding additional crystals to a merged data set; however, the strategy of successive wedge-by-wedge crystal-by-crystal additions until a structure solution appears to be an economical approach.
Radiation damage and high multiplicity have conflicting effects in single-crystal data collection: on the one hand, increasing multiplicity can benefit the measurement of weak anomalous signals; on the other hand, radiation damage increases with added X-ray exposure and affects data quality adversely. Radiation damage is a serious problem and is common for delicate samples, for example membrane proteins and large macromolecular complexes.
To detect radiation damage in single-crystal data sets, the Rd plot (Diederichs, 2006), anomalous correlation coefficient, scaling B factor and Rmerge may all be useful, as have been thoroughly reviewed (Dauter, 2006b; Garman & Nave, 2009; Garman, 2010; Borek et al., 2010). For multi-crystal native SAD experiments, these indicators are also effective to detect and reject seriously damaged frames. In addition, the merger of diffraction data by wedges is useful to detect and mitigate the effects of radiation damage (Liu, Zhang et al., 2011).
Relatively large crystals were available for these studies and complete data sets were collected from each of the crystals in each of the systems. We estimate based on RADDOSE simulations (Paithankar et al., 2009) that accumulated doses were well below the Henderson limit (20 MGy) for all five systems; for DnaK in particular the dose was ∼5 MGy per crystal for the 800 frames in each data set. Nevertheless, our wedge-by-wedge analyses (eight wedges of 50 + 50 inverse-beam wedges each) show clear indications of radiation damage. Although each wedged data set has similar multiplicity and all are essentially complete, the measures of data quality [I/σ(I), ACC, MapCC before and after DM] all worsen on average as exposure increases (Table 5a). Although I/σ(I), a measure of overall diffraction quality, deceased from 29.8 for wedges 1–3 to 23.9 for wedges 6–8 (20%), measures sensitive to anomalous signals (ACC and MapCC) suffered more. For example, MapCC after DM decreased from 62.2 to 42.3% over the same span (32%).
To test the effects of radiation damage on structure determination, we next merged the DnaK data accumulatively wedge by wedge (Table 5b) and used these merged data sets for substructure determination and SAD phasing. Measures of substructure determination (by SHELXD CCweak) and phasing efficacy (by MapCC) were plotted against multiplicity in Fig. 10(c). Similar wedge-by-wedge mergings had been performed before for the other four structures (Liu et al., 2012) and results from the HK9S study are shown in Fig. 10(d). The features described above with respect to structure solvability in crystal-by-crystal mergings (Figs. 10a and 10b) are also observed in wedge-by-wedge mergings (Figs. 10c and 10d, respectively); however, performance is better as a function of multiplicity by wedges than of multiplicity measured crystal by crystal, even when in the best-to-worst order. For example, DnaK data merged by accumulated wedges supported substructure determination at an overall multiplicity of 74.1 (frames 1–200), whereas determinations from the mergings of crystals best to worst required nearly double that multiplicity (123.3 for crystals 1′ to 4′). We attribute this improvement to reduced radiation damage at lower wedged multiplicity. For DnaK, the substructure success rate peaks on merging of just five wedges (frames 1–250) and then falls off, which may also reflect the effects of radiation damage (Table 5b). For HK9S, inclusion of the last two wedges even had a deleterious effect on substructure determination in that CCweak from SHELXD decreased and map quality as judged by MapCC was nearly flat beyond wedge 4. These effects are also consistent with radiation damage that is mitigated by restricting exposure.
For the radiation doses used in these studies, we find that the quality of the electron-density maps (MapCC) improves asymptotically with wedged multiplicity (Fig. 10; see also Fig. 3 of Liu et al., 2012), which implies that the damaged data contribute positively even if marginally. Nevertheless, there is a clear strategic advantage in limiting the radiation dose. This can be accomplished while still reaching adequate multiplicity for structure solution by combining measurements from many crystals with limited exposure for each. Since radiation damage is disordering as well as destructive, reducing high-angle diffraction first (Hendrickson, 1976), this limited-exposure approach is expected to improve resolution as well as the overall phasing statistics. In any case, it is evident from the results in Fig. 10 that wedge-by-wedge merging is advantageous, at least for analyzing the effects of radiation damage.
Many biologically relevant metal ions (Na+, Mg2+, K+ and Ca2+) and anions of interest (phosphate, sulfate and chloride) feature low-Z elements (Z ≤ 20). Although the chemical environments of such ions in crystal structures give important clues for identification, such sites can be ambiguous and especially so at low resolution. Anomalous scattering offers a means of direct identification, but the absorption edges for such light elements are far away from the X-ray energies commonly used in X-ray crystallography. Therefore, the direct identification of low-Z ions is challenging, especially for the lightest ions Na+ and Mg2+. Often, the indirect alternative of replacing a candidate ion with a chemical relative is used (Zhou & MacKinnon, 2003; Morth et al., 2007; Kazantsev et al., 2009). Examples include replacement of Na+ and K+ by Rb+ or Tl+; of Mg2+ and Ca2+ by Sr2+ or a lanthanide such as Yb3+; of Cl− by Br− or I− and of SO42− by SeO42−. Such replacements are never perfect, however, and direct in situ identification will certainly be advantageous. Others have used low-energy X-ray diffraction to show that diverse, and sometimes unexpected, ions are components of protein crystal structures (Mueller-Dieckmann et al., 2007; Raaf et al., 2008); however, previous studies have relied on chemical composition and environment for elemental identification.
The procedure that we have devised here for detecting and identifying low-Z ions directly from anomalous scattering signals is straightforward and robust. For site detection, we used Bijvoet-difference Fourier syntheses; for elemental identification, we used f′′ refinements against Bijvoet mates. The procedure worked effectively for all five native SAD structures in this study (Table 6 and Fig. 8; see also Fig. 2 of Liu et al., 2012). Once an atomic structure is known, the same procedure could be used with a single-crystal data set, of course; however, multi-crystal averaging clearly improves the signals (Fig. 8). We used 7.1 keV X-rays in the current studies, whereas a lower X-ray energy could be beneficial owing to the increased f′′ values. It is worth noting that variable site occupancy is a potential complication for f′′ refinement since occupancy and scattering strength are redundant parameters. Occupancy is usually fixed at 1.0 for protein atoms unless alternate conformations are present; however, ions may be present at less than unit occupancy. For refinements at moderate resolution, B factors and occupancy parameters are highly correlated; however, ions or other ligands tend to have B factors that are similar to those of the protein atoms to which they are coordinated. Therefore, we fixed the B factors of ions to be at the average of those for associated protein atoms; we next refined occupancy parameters in a conventional refinement and finally we refined the f′′ anomalous scattering factors with occupancies fixed at these values. Notice that positional and B-factor parameters are mainly determined by the predominant normal scattering contributions; Bijvoet differences depend uniquely on f′′ values. The refined f′′ value provides an orthogonal check that must be consistent with the normal scattering identity used for atomic refinement.
We show in these studies that native SAD phasing can be effective even with X-rays at the modestly low energy of the Fe K edge and even with bending-magnet radiation. Experiments at lower energy promise stronger anomalous signals (Fig. 1a), and with appropriate experimental designs the complications from absorption (Fig. 1b) and incoherent scattering (Fig. 1c) can be addressed very effectively. With the brightness of an undulator source, beam size and divergence can be reduced for better data quality. With noise-free readout over a wide dynamic range, pixel-array detectors can record diffraction data with improved accuracy (Mueller et al., 2012). With improved methods for sample handling and automation, improved data sets composed from many dozens or hundreds of crystals can be envisioned. Moreover, with an advanced microdiffraction beamline, the smaller samples needed to take full advantage of lower X-ray energies for improved anomalous signals (Fig. 2). With lower X-ray energy, more challenging native SAD experiments, such as larger structures at lower resolution, might become routinely feasible. For energies below ∼4 keV (λ > ∼3 Å), flat detectors become problematic because of high scattering angles even for modestly fine Bragg spacings (Fig. 1d) and detectors with quasi-spherical or quasi-cylindrical geometry are needed. Indeed, there is a strong case for synchrotron beamlines and instrumentation dedicated to low-energy diffraction experiments.
The data-processing procedures could also be optimized. For example, an improved local-scaling algorithm that takes better advantage of inverse-beam data could be used to reduce nonsystematic errors. A better weighting scheme could also be developed and used to enhance anomalous signals in merged data. Further optimization of crystal clustering and sorting procedures would be advantageous, especially when envisioning incomplete data sets from large numbers of microcrystals.
We believe that procedures of the kind described here can have very broad applicability, and especially so with optimizations of the kind described above. We devised our multi-crystal native SAD procedures in the course of applications to five crystal structures (Table 2, Fig. 9) that are not atypical of the range of contemporary structural problems. They include structures with up to 1200 amino-acid residues in the asymmetric unit and have resolution limits as low as 2.8 Å. As of 10 April 2012, 90% of PDB entries from X-ray crystallography (63 559 out of 70 739) were determined at 2.8 Å resolution or higher. For de novo structures solved by SAD, the fraction at 2.8 Å resolution or better increases to 96% (5077 out of 5286). Thus, we suggest a broad reach for the method.
Structure determination by multi-crystal native SAD phasing is distinguished from current practice in requiring a supply of equivalent crystals, and meeting this condition may be an obstacle in some cases; however, an abundance of crystals is quite common and such production is likely to increase should the new technology take hold. At present, SeMet SAD is the predominant method for solving crystal structures de novo and molecular replacement dominates overall. With anticipated advances in synchrotron instrumentation and automation, it is plausible to expect that multi-crystal native SAD phasing could come to predominate for de novo structure determination, perhaps incorporating molecular replacements to aid in substructure determination. As an added benefit, such analyses could routinely include the discovery and reliable identification of associated ions such as Na+, Mg2+, K+ and Cl−, often troublesome heretofore.
We thank Ruifeng Qi and Xinping Xu for their assistance in preparing crystals, and they as well as John Schwanof and Randy Abramowitz for help with synchrotron data collection. We also thank our collaborators in the previously published aspects of the current work, especially Zhen Zhang, Filippo Mancia and Lawrence Shapiro. This work was supported in part by NIH grants GM34102 and GM095315, and by start-up funds from the Virginia Commonwealth University School of Medicine, a New Scholar Award in Aging from the Ellison Medical Foundation and a Grant-In-Aid Award from the American Heart Association. Beamline X4A of the National Synchrotron Light Source (NSLS) at Brookhaven National Laboratory, a DOE facility, is supported by the New York Structural Biology Center.
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