CCP4 study weekend
Twinned crystals and anomalous phasing
^{a}Synchrotron Radiation Research Section, National Cancer Institute, Brookhaven National Laboratory, Building 725AX9, Upton, NY 11973, USA
^{*}Correspondence email: dauter@bnl.gov
λ capsid protein, show that the singlewavelength anomalous diffraction (SAD) method can be used to solve its structure even if the data set corresponds to a perfectly twinned crystal with a twin fraction of 0.5.
or of crystals cannot be identified from inspection of the diffraction patterns. Several methods for the identification of and the estimation of the twin fraction are suitable for macromolecular crystals and all are based on the statistical properties of the measured diffraction intensities. If the crystal twin fraction is estimated and is not too close to 0.5, the diffraction data can be detwinned; that is, related to the individual crystal specimen. However, the detwinning procedure invariably introduces additional inaccuracies to the estimated intensities, which substantially increase when the twin fraction approaches 0.5. In some cases, a can be solved with the original twinned data by standard techniques such as multiple or multiwavelength anomalous diffraction. Test calculations on data collected from a twinned crystal of gpD, the bacteriophageKeywords: twinning; merohedral; pseudomerohedral; anomalous scattering; SAD.
1. Introduction
). The splitting or cracking of crystals often encountered by practicing crystallographers should not therefore be described as The size of the twin domains is large in comparison with the crystal cell dimensions, so that Xrays diffracted by the separate parts do not interfere and the total diffraction corresponds to the sum of intensities originating from individual domains. This is in contrast to disorder in a crystal, where there are differences in the location of the content of the neighbouring unit cells. In the case of disorder (either static or dynamic), diffracted Xrays represent the averaged (spatially or temporally) content of all unit cells.
occurs when a crystalline specimen consists of multiple domains which are mutually reoriented according to a specific transformation that does not belong to the symmetry operations of the crystal but is related in some way to the crystal (Koch, 1992Twins can be classified according to the mutual disposition of the individual domains. Various kinds of twins have different manifestations in ) differentiate between twins with twinlattice symmetry, characterized by a single with all reflections perfectly overlapped, and twins with twinlattice quasisymmetry, with some reflections originating from individual separated domains. According to the terminology introduced by Friedel (1928), they correspond to or nonmerohedral twins, respectively.
which has important consequences for the process of structure solution of twinned crystals. Donnay & Donnay (1974Merohedral twins reflect the possibility of different nonequivalent orientations of crystals within a e.g. with only a half (hemihedry) or a quarter (tetartohedry) of its symmetry elements, the of such a crystal transformed by a of the but not belonging to the will conform perfectly within the same but will not be equivalent to the initial orientation. In such a transformation will lead to the exchange of indices between nonequivalent reflections having different intensities, as in Fig. 1. In general, the relation between different twin domains may involve rotations, mirror reflections or point inversions, and all are observed in smallmolecule crystallography and mineralogy. Since proteins, and are chiral, in macromolecular crystallography the only possible twin operations are proper rotations and further discussion will be restricted to twins related by rotations. In Friedel's nomenclature, this corresponds to relations between holoaxial (maximum rotational symmetry of the lattice) and holoaxial (a half of the previous symmetry operations or a quarter of the holohedry) or holoaxial (a half of the previous elements). Table 1 lists space groups that can lead to and specifies the possible operations.
of symmetry higher than the crystal pointgroup (class) symmetry. This is possible in the tetragonal, trigonal, hexagonal or cubic systems, with lattices always having the highest symmetry of the system (holohedry). If the is a of the symmetry,

gives some examples of possibilities. Because the pseudomerohedry results from a serendipitous coincidence of cell dimensions, the overlap of twin lattices may not be ideal and sometimes a broadening or split of reflection profiles can be observed, especially at high resolution. Otherwise, pseudomerohedrally twinned crystals have identical characteristics to the classic twins.
cannot be distinguished from the appearance of the diffraction pattern, since reflections from different twin components overlap perfectly as a consequence of the identity of the holohedral and metrics. However, a similar situation may arise when the crystal metric fortuitously corresponds to the higher symmetry system. Such cases are termed pseudomerohedry. Again, the is a present in the highsymmetry group of the but absent in the proper symmetry class of the crystal. Table 2

Sometimes only a subset of reflections from two twin domains overlap, which is termed nonmerohedral .
This type of is characterized by abnormalities in the diffraction pattern, with some planes or lines of reflections in having different numbers of reflections to others, which cannot happen in a single (except as a result of absences resulting from screw axes or glide planes). Examples of diffraction images from nonmerohedrally twinned crystals are shown in Fig. 2If the lattices of twin components fit in less than three dimensions, diffraction images recorded from such epitaxic twins are usually characterized by streaks or overlap of reflection profiles in a particular direction. Such diffraction patterns are difficult to interpret and are similar to images from split or highly mosaic crystals.
Further discussion will be restricted to
or pseudomerohedral twins of macromolecules, excluding mirror planes or center inversions as twin operations.2. Effect of on diffraction intensities
e.g. a primitive tetragonal crystal can be indexed as orthorhombic, monoclinic or triclinic.
or exact cannot be recognized by inspection of diffraction images, since the geometric characteristics of the do not reveal that it may consist of two perfectly overlapped sets of reflections. In view of this, one of the criteria often given for identification of twins, that `the metric symmetry of the is higher than the Laue symmetry of the crystal', is not useful at the stage of the initial interpretation of diffraction images from the newly obtained crystals. This is true for any pair of subgroup/supergroup relations,However, the true symmetry of the crystal depends on its content, not on the geometry of its
therefore, the crystal symmetry should be inferred from the symmetry of the distribution of reflection intensities in The metric of the can exclude some higher symmetry systems, but cannot identify which of the lower symmetry systems (subgroups) is correct. The triclinic crystal may by chance have all cell dimensions almost equal and all angles very close to 90°, yet despite having the cubic metric, the intensities diffracted from this crystal will not merge in any symmetry higher than triclinic.In the case of I_{1} and I_{2}, the intensities measured from a crystal with the twin fraction α will be J_{1} = αI_{1} + (1 − α)I_{2} and J_{2} = (1 − α)I_{1} + αI_{2}. For perfect twins with α = 0.5, both intensities are equal and the intensities measured from such a crystal will merge perfectly in the symmetry higher than that of the real crystal If the twin fraction is smaller than 0.5, the data will merge well in the correct but in higher symmetry will give an R_{merge} value lower than 55%, expected for a completely wrong symmetry assignment. Such a behavior of R_{merge} is a simple and typical qualitative warning that a partial may be present.
twins, the symmetry of the distribution of reflection intensities in may be misleading. If the original (untwinned) intensities of the individual reflections in a pair related by the areThe above discussion refers to the distribution of reflection intensities in
Since Xrays diffracted from separate twin domains do not interfere, the intensities of reflections measured from a twinned crystal consist of the sum of the intensities of the individual twin domains, weighted by their relative volumes illuminated by the Xray beam. If the separate domains had the same orientation, as in the singlecrystal specimen, the diffracted Xrays would interfere and the intensity of the diffracted Xrays would correspond to the sum of the structure amplitudes, not the intensities. As a consequence, reflections measured from a twinned crystal display intensity statistics that differ from classic Wilson's theory. This can be explained simply as follows. A set of intensities from a single crystal is characterized by a certain low percentage of very weak reflections and a certain small amount of very strong reflections. In the twinned crystal, reflection intensities are added up in pairs related by the The probability that the connects two very weak or two very strong reflections is, therefore, rather low and, as a consequence, in the data set measured from a twinned crystal the amount of extreme, very low or very strong intensities is still smaller than in the case of a single crystal. The intensities from twinned crystals have therefore a sharper distribution around the mean value than that resulting from Wilson statistics.As pointed out by Rees (1980), the structural disorder leading to additional has an effect opposite to with the intensity distribution flatter than in Wilson's distribution.
The theory of intensity statistics for merohedrally twinned crystals was worked out by Stanley (1955, 1972) and Rees (1980, 1982). For very convenient practical comparisons, one may use the cumulative intensity distribution N(z), giving the fraction of all reflections with intensities below the limit z (Howells et al., 1950). The formulae for untwinned and perfectly twinned centric and noncentric reflections are shown in Table 3. As can be seen, the distribution for a perfectly twinned centrosymmetric crystal is the same as for an untwinned noncentrosymmetric crystal. Therefore, in the calculation of intensity statistics, the centrosymmetric reflections have to be treated separately, since in the highsymmetry cubic, hexagonal or tetragonal space groups, particularly at low resolution, the fraction of centrosymmetric reflections is significant.

The higher moments of the intensity distribution provide another global distinguishing criterion (Stanley, 1972). They have been routinely used for confirming the presence or absence of the center of symmetry in small structure crystals and are also distinctive for twinned crystals, as indicated in Table 3.
3. Detection of (pseudo)merohedral twinning
Several tests based on various properties of the intensity distributions have been proposed and used in practice in smallmolecule and macromolecular crystallography. They will be illustrated here with data collected from the pseudomerohedrally twinned P2_{1} crystal of gpD, the capsidstabilizing protein of bacteriophage λ (Yang, Dauter et al., 2000; Yang, Forrer et al., 2000), and from merohedrally twinned P4_{3} crystals of interleukin1β (Rudolph et al., 2003).
3.1. Packing considerations
The presence of V_{M}, and solvent content (Matthews, 1968) in highsymmetry crystals suggest possible IL1β crystallizes with unitcell parameters a = b = 53.9, c = 77.4 Å. In P4_{3} with four molecules in the it gives a Matthews coefficient V_{M} of 2.9 Å^{3} Da^{−1} and a solvent content of 58% (Rudolph et al., 2003). Even if this crystal was perfectly twinned, the P4_{3}22 could not be accepted, because eight molecules in the would require the V_{M} value to be 1.45 Å^{3} Da^{−1}, well below the acceptable limit of 1.75 Å^{3} Da^{−1}.
may sometimes be concluded from crystalpacking considerations. Even if the diffraction data merge well in the highsymmetry there may not be enough space in the to accommodate the required number of molecules. An unrealistically low Matthews number,3.2. Moments of intensities distribution
As mentioned above, one of the consequences of i.e. very weak). In these terms, the diffraction intensities from twinned crystals appear hypononcentric, with less variation of their values than the average. This is understandable, since results in the averaging of unrelated intensities in pairs. In a quantitative representation, the variance (and higher moments) of the intensity distribution is smaller for twinned crystals than for single specimens. The Wilson (1949) ratio 〈F〉^{2}/〈I〉 is expected to be 0.785 for normal noncentrosymmetric reflections and 0.885 for such reflections from twinned crystals, as shown in Table 3 (Stanley, 1972). Fig. 3 shows these values calculated in resolution ranges from gpD and IL1β data and, as a control, the obviously untwinned accurate data from lysozyme (Dauter et al., 1999). The points shown in the figure are considerably scattered and although on average they suggest that the crystal of lysozyme was not twinned and that those of gpD and IL1β were considerably twinned, it is difficult to satisfactorily estimate the degree of from these graphs.
is the smaller fraction of very weak as well as very strong intensities in the entire population of reflections. This is analogous to the difference between diffraction patterns of centrosymmetric and noncentrosymmetric crystals. Experienced smallstructure crystallographers are able to differentiate between the presence or absence of the center of symmetry by looking at a single precession or Weissenberg photograph, from the amount of reflections that are unobservable by eye (3.3. Britton plot of `negative intensities'
As pointed out above, the intensities measured from a twinned crystal are combined from two twin domains with weights proportional to their volumes,
where I_{1} and I_{2} are the measured intensities of a pair of reflections related by the J_{1} and J_{2} are the true intensities of these reflections as originating from untwinned crystal and α is the ratio, equal to the of the smaller twin component.
If α is smaller than 0.5, this system of equations can be solved for J_{1} and J_{2},
These equations are the basis of the detwinning procedure, which is possible only for α < 0.5. Detwinning of perfectly twinned data is impossible, since for α = 0.5 the system of detwinning equations becomes indeterminate.
Data collected from merohedrally twinned crystals can very conveniently be tested and detwinned using the Yeates & Fam http://www.doembi.ucla.edu/Services/Twinning/ ).
server at UCLA (Britton (1972) pointed out, and earlier Zalkin et al. (1964) implicitly mentioned, that the assumption of too large a value of α results in an estimation of negative true intensities. Based on this principle, Fisher & Sweet (1980) proposed a practical method for the estimation of the twin fraction α. The `Britton plot', giving the number of negative intensity estimations as a function of the assumed value of α in the detwinning procedure, has two linear asymptotes, one for α < α_{opt} and another for α > α_{opt}. The point at which these two lines cross gives the estimated value of the twin fraction. The Britton plot for gpD and IL1β is shown in Fig. 4. It suggests twin fractions of 0.34 for gpD and 0.32 for IL1β.
3.4. MurrayRust F_{1}/F_{2} plot
The J_{2}/J_{1},
equations can be rearranged to give the ratioSince both J_{1} and J_{2} are positive, neither numerator nor denominator should be negative, as pointed out by Britton (1972), and these two conditions can be expressed as α < I_{1}/(I_{1} + I_{2}) and α < I_{2}/(I_{1} + I_{2}) or, as one inequality,
or in terms of structure amplitudes,
This property was proposed by MurrayRust (1973) for estimation of the twin fraction. All points in the graph of F_{1} plotted against F_{2} should lie between the two limiting straight lines corresponding to [α/(1 − α)]^{1/2} and [(1 − α)/α]^{1/2}. The slope of the lines bounding the points on the graph can be used to estimate the twin fraction. The MurrayRust plots for gpD and IL1β are shown in Fig. 5. The twin fractions suggested by these plots are about 0.32 for gpD and 0.34 for IL1β.
3.5. Rees N(z) plot
Howells et al. (1950) first introduced the cumulative intensity distribution N(z) plot to differentiate between centrosymmetric and noncentrosymmetric crystals. The argument z is the fraction of the local average intensity, calculated in narrow resolution ranges, and N(z) is the fraction of reflections with intensities below this level. Various intensity distribution functions show different N(z) curves, particularly for low values of z. As noted above, the fraction of weak intensities is lower for noncentrosymmetric crystals than for centrosymmetric crystals and is lower still for twinned crystals, which shows up clearly on the N(z) plot. This criterion was proposed and theoretically worked out by Stanley (1955, 1972) and elaborated by Rees (1980), who gave the general formula for the cumulative intensity distribution for a noncentrosymmetric case with the twin fraction α, as indicated in Table 3. As Stanley (1955) pointed out, the N(z) curve for twinned crystals is characteristic `in having an opposite initial curvature'; it has a sigmoidal shape in contrast to an exponential character for normal crystals. He also stated that this test `would be tedious to apply', which is no longer valid after 50 years of progress in computing technology.
Fig. 6 illustrates the N(z) distributions for gpD and IL1β, together with the theoretical curves for untwinned and perfectly (α = 0.5) twinned crystals. This test qualitatively characterizes twinned crystals, but cannot provide an accurate quantitative estimation of the degree of twinning.
3.6. Yeates S(H) plot
This test, proposed by Yeates (1988, 1997), is based on the behavior of the ratio of the difference to the sum of intensities of reflections related by the H = I_{1} − I_{2}/(I_{1} + I_{2}). The dependence of the cumulative distribution of this parameter, S(H), on the twin fraction is very simple (see Table 3) and is linear in H for noncentrosymmetric crystals. The slope of the S(H) plot is 1/(1 − 2α) and depends on the factor more sensitively than the N(z) plot. Moreover, omission of pairs of weak reflection from the calculations does not bias the results, but actually leads to improved accuracy of the estimation of the twin fraction. This way of estimating a twin fraction is usually more robust and accurate than other tests. Fig. 7 illustrates the S(H) plots for gpD and IL1β. Apart from the cumulative distribution S(H), the average values 〈H〉 and 〈H^{2}〉 are characteristic for particular twin fractions, as noted in Table 3. These average values are 0.168 and 0.0408 for gpD and 0.154 and 0.0333 for IL1β, which gives an estimation of the twin fraction as 0.332 and 0.325 for gpD and as 0.346 and 0.342 for IL1β, respectively.
3.7. Local intensity differences: Lfunction
Recently, Padilla & Yeates (2003) introduced a very robust statistic, especially suited to crystals displaying abnormalities in their diffraction patterns, resulting for example from pseudocentering or anisotropy. In such cases, the intensities of some reflections are systematically different. If diffraction extends to higher resolution in one direction of than in another, the intensity statistics for such anisotropically diffracting crystals will be abnormal. Similarly, if there are multiple molecules in the related by a parallel translation by a vector close to a fraction of the some classes of reflections, depending on the parity of their indices, will have abnormally weak intensities, shifting the overall intensity statistics towards the centrosymmetric character, in the direction opposite to that of In such cases, the tests described above will not be decisive. However, the newly proposed Lfunction, based on the local intensity distribution, is very robust and unambiguous.
The quantity L is the ratio of the difference to the sum of a pair of reflections L = (I_{1} − I_{2})/(I_{1} + I_{2}), but the two reflections I_{1} and I_{2}, in contrast to the Hfunction, are not related by the Instead, they are selected in the vicinity of each other in the For pseudosymmetric crystals their indices may for example differ by 2 or 4, comparing neighboring reflections from the same parity group.
The average values of the moments of L are characteristic for twinned and untwinned crystals, as well as its cumulative distribution, N(L), are given in Table 3.
3.8. Additional remarks
In the detwinning of diffraction data and the use of the α is not too close to 0.5. Fisher & Sweet (1980) estimated that the relation between uncertainties of the detwinned, σ(J), and measured, σ(I), intensities is
tests described above, one should be aware of three important points. Firstly, detwinning is possible only ifand for α approaching 0.5 the detwinned intensities become very inaccurate. Of course, for perfect twins, with α = 0.5, detwinning is not possible at all.
Secondly, several R_{merge} value does not discriminate between perfectly twinned and nontwinned crystals. The only useful tests in such cases are those based purely on the distribution of measured intensities; that is, Wilson ratios or N(z) cumulative intensity distribution, where it does not matter whether the data have been merged in the crystal or the symmetry. It is a good practice to always check the N(z) distribution of the processed data, particularly in the hexagonal, tetragonal or cubic space groups.
tests (those of Britton, MurrayRust and Yeates) are based on comparison of the twinrelated reflection intensities. This obviously requires that the diffraction data are merged in the proper lowsymmetry However, if the data were collected from a crystal that is not twinned, the above tests would indicate perfect since the reflections connected by the potential relation (but in fact the valid symmetry operation) have equal intensities. As mentioned before, theThirdly, care should be exercised in detwinning the anomalous diffraction data in order to avoid mixing the positive and negative Friedel mates. Since macromolecules are chiral, the CCP4 (Collaborative Computational Project, Number 4, 1994) programs is −h_{max} ≤ h ≤ h_{max}, 0 ≤ k ≤ k_{max}, 0 ≤ l ≤ l_{max} and the is the twofold axis diagonal between the a and c directions, relating reflections h, k, l and l, −k, h. However, reflections with negative k do not belong to the same and have to be converted by the mirror symmetry to l, k, h (if h is positive) or to −l, k, −h (if h is negative), which requires exchanging the Friedel mates. For example, the measurement I^{+}(2, 3, 4) should be paired with I^{−}(4, 3, 2) and I^{+}(−3, 4, 5) with I^{−}(−5, 4, 3). Reflections h0l are centrosymmetric and reflections hkh and −hkh are somewhat special, since the relates them with their own Friedel mates.
operations can only be pure rotations, always relating Friedel mates of the same character. Therefore, the positive and negative Friedel mates can be detwinned separately. In practice, however, attention should be directed to the definition of the in this procedure. For example, for the monoclinic crystal of gpD, the defined as in the4. Solution of twinned crystal structures
4.1. Phasing
Not many macromolecular structures of twinned crystals are available in the literature. Basic information on these structures is collected in Table 4. However, there is probably a number of available structures that may be undetected twins (Yeates & Fam, 1999).
If the twin fraction α is smaller than 0.5, it is possible to first detwin the data and then use such data for structure solution. It is not clear over which range of α the detwinning procedure is beneficial. If α is small, it may not be necessary to apply detwinning in order to obtain the structure solution; if α is too close to 0.5, the detwinning procedure may introduce errors exceeding the effect of itself. The benefit gained from the detwinning procedure significantly depends on the accuracy of the originally measured intensities. Often, the structures can be solved from the original, not the detwinned, data. In fact, the structure of gpD was solved by MAD before detecting that the crystal used had a twin fraction of 0.36 (Yang, Dauter et al., 2000).
If the molecularreplacement calculations are performed on the original data, multiple solutions can be expected in the rotation function, reflecting different orientations of the individual twin domains with corresponding weights. In the translation function the smaller twin domain contributes additional noise, but the principal solution should correspond to the main domain.
The MIR approach relies on the small differences between the native and derivative data; if the twin fractions of derivative and native crystals are high or significantly different, the phasing procedure can be severely impaired. According to the analysis of Yeates & Rees (1987), four derivatives are necessary in principle to uniquely estimate the protein phase, instead of two as in the classic MIR approach.
The identification of heavyatom sites may be not trivial. It may not be possible to fully interpret the isomorphous difference (as well as the anomalous difference) Patterson for highly twinned crystals in any of the potential space groups. Since the Xrays diffracted by the individual twin domains do not interfere, the Patterson synthesis calculated with such data corresponds to the superposition of two Patterson maps transformed by the P4, the data can be merged in P422. In the Patterson synthesis the w = 0 will have 4mm symmetry, as expected for the 422 class, but the Harker sections in the (100) and (110) planes will not show any peaks resulting from the potential existence of dyads in the ab plane.
Certain Harker sections will reflect the higher symmetry, but the potential Harker sections originating from the operations (rotations) will be featureless, even with measured intensities merged in the higher apparent but wrong symmetry. For example, for a perfectly twinned crystal in theThe MAD and SAD approaches may be expected to be less severely impaired by
than MIR, since diffraction data are usually collected from a single specimen with a constant twin fraction.4.2. Refinement
Once the preliminary model of the structure is available, its parameters and the twin fraction can be refined, taking into account the ) and Pratt et al. (1971) or the similar iterative approach (Redinbo & Yeates, 1993; Yeates, 1997), where the calculated squared amplitudes and the derivatives are accumulated from the individual twin contributions after appropriate transformation. This approach is implemented in SHELXL (Sheldrick & Schneider, 1997; HerbstIrmer & Sheldrick, 1998) and CNS (Brünger et al., 1999). It has the additional advantage of producing on output the detwinned structure factors for standard Fourier map calculations. Almost all twinned macromolecular crystal structures have been refined in this way.
relations between structure amplitudes. This is possible by the method proposed by Jameson (19825. SAD calculations on gpD
The SeMet variant of the capsidstabilizing protein of bacteriophage λ, gpD, crystallizes in P2_{1} with unitcell parameters a = 45.51, b = 68.52, c = 45.52 Å, β = 104.4°, which are very similar to those of the native crystals. Because the a and c parameters are virtually identical, this cell can be indexed as C222_{1} with a = 56.02, b = 72.13, c = 69.03 Å, where the orthorhombic a and b axes are parallel to the diagonals between the monoclinic a and c directions. Each monomer has two SeMet residues and the contains three monomers arranged according to the noncrystallographic threefold axis. The structure has been solved from the 1.7 Å SeMAD data and refined anisotropically against the 1.1 Å native data (Yang, Forrer et al., 2000) to an R factor of 9.9% with SHELXL. Both SeMet and native crystals were pseudomerohedrally twinned (Figs. 3, 4, 5a and 6) with a twin fraction which refined with SHELXL to 0.36. The details of structure solution and some MAD tests using different programs and protocols have been published separately (Yang, Dauter et al., 2000).
Here, other phasing tests are presented based on the singlewavelength anomalous diffraction (SAD) approach. Only the 1.7 Å peakwavelength SeMet data set was used for these calculations. The original data were modified in two ways. Firstly, they were detwinned according to the principles explained above. Secondly, the intensities related by the a and c axes) were averaged, yielding data corresponding to a perfectly twinned crystal with α = 0.5. These three data sets will be referred to as gpD^{O} (original), gpD^{D} (detwinned) and gpD^{T} (twinned).
(a rotation around the twofold axis diagonal betweenFig. 8 shows the v = ½ Harker sections of the anomalous difference Patterson syntheses calculated with the three sets of data. All six selfvectors are clearly visible in all three cases. As expected, the gpD^{D} synthesis is marginally clearer than gpd^{O}, with most of the peaks corresponding to the minor twin domain suppressed. Again, as expected, the gpD^{T} synthesis has orthorhombic symmetry, since contributions of both domains were deliberately equalized.
The location of the selenium sites was also attempted by the directmethods approach with SHELXD (Schneider & Sheldrick, 2002) based on Bijvoet differences. This step was highly successful, with almost all multisolution trials leading to proper solutions of selenium sites, with a clear contrast between the last correct (sixth) and first spurious (seventh) peak (Table 5a). The results obtained from the perfectly twinned gpD^{T} data were almost as clear as from the other two sets.

The identified anomalous scatterers sites were input to SHELXE (Sheldrick, 2003) for the estimation of protein phases with a simultaneous density modification. The phase sets obtained were input to automatic model building with ARP/wARP 5.1 (Perrakis et al., 1999) in conjunction with REFMAC (Murshudov et al., 1999). The results of phasing are summarized in Table 5(b) and a region of the resulting electrondensity maps is illustrated in Fig. 9. The quality of phasing against the gpD^{O} and gpD^{D} data was practically equivalent, with an average error of 53–57°. The (CC) between the SHELXE and the final refined electrondensity maps was 63–69% overall and 71–73% for the main chain (Figs. 9a and 9b). ARP/wARP automatically built more than 90% of amino acids into both the gpD^{O} and gpD^{D} maps. The protein phase estimation was less successful with the fully twinned gpD^{T} data, where the resulting average phase error was 65° and the map was much poorer, with a CC of 49% overall (57% for main chain). This map was not clear enough for ARP/wARP, but a visual inspection showed that large portions of this map were interpretable (Fig. 9c). The stepwise model building and of the partial model and the twin fraction with SHELXL eventually led to a complete structure.
6. Conclusions
Several simple tests exist and can be used to check if the diffraction data originate from twinned crystals. Such tests are strongly recommended as a `default' for crystals of high symmetry or when unitcell dimensions are amenable to potential
Early detection of this phenomenon allows the crystallographer to avoid `unexpected' obstacles in various stages of the structure solution and model Even if the initial model can be built with the original data, the existence of if not properly accounted for, will seriously impair the process of model and the appearance of Fourier maps.The degree of the adverse effect of
on the process of solution is critically dependent on the accuracy of measured diffraction intensities and, of course, on the twin fraction. As a consequence of the resulting inaccuracies, the potentially constructive detwinning of the original data may in fact lead to more harm than benefit, considerably increasing the average error level of the estimated intensities. If the twin fraction is small, it may be not worthwhile performing the data detwinning; if it is close to 0.5, detwinning will introduce very large errors. The range of twin fraction where the data detwinning is beneficial may be different for different cases. However, it is always beneficial to account for in model and map calculation.As shown with the example of the gpD data, crystal
does not absolutely prevent the use of the anomalous signal for a successful structure solution. It may be possible even for a perfectly twinned crystal with accurately measured data and strong enough signal.Acknowledgements
The author wishes to express his gratitude to Markus Rudolph for the kind provision of the interleukin1β data set and permission to use it as a test example at the CCP4 Study Weekend (York, January 2003) and in this paper
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