Radiation-damage-induced Phasing Research Articles

Probabilistic Estimate of |Foa| from FEL Data

The method of the joint probability distribution function was applied in order to estimate the normal structure factor amplitudes of the anomalous scatterer substructure in a FEL experiment. The two-wavelength case was examined. In this, the prior knowledge of the moduli | F 1 + | , | F 1 − | , | F 2 + | , | F 2 − | was used to predict the value of | F 0 a | , which is the structure factor amplitude arising from the normal scattering of the heavy atom anomalous scatterers. The mathematical treatment provides a solid theoretical basis for the RIP (Radiation-damage Induced Phasing) method, which was originally proposed in order to take the radiation damage induced by synchrotron radiation sources into account. This was further adapted to exploit FEL data, where the crystal damage is usually more massive.

X-ray and UV radiation-damage-induced phasing using synchrotron serial crystallography.

Specific radiation damage can be used to determine phases de novo from macromolecular crystals. This method is known as radiation-damage-induced phasing (RIP). One limitation of the method is that the dose of individual data sets must be minimized, which in turn leads to data sets with low multiplicity. A solution to this problem is to use data from multiple crystals. However, the resulting signal can be degraded by a lack of isomorphism between crystals. Here, it is shown that serial synchrotron crystallography in combination with selective merging of data sets can be used to determine high-quality phases for insulin and thaumatin, and that the increased multiplicity can greatly enhance the success rate of the experiment.

Radiation Damage and Racemic Protein Crystallography Reveal the Unique Structure of the GASA/Snakin Protein Superfamily.

Proteins from the GASA/snakin superfamily are common in plant proteomes and have diverse functions, including hormonal crosstalk, development, and defense. One 63-residue member of this family, snakin-1, an antimicrobial protein from potatoes, has previously been chemically synthesized in a fully active form. Herein the 1.5 Å structure of snakin-1, determined by a novel combination of racemic protein crystallization and radiation-damage-induced phasing (RIP), is reported. Racemic crystals of snakin-1 and quasi-racemic crystals incorporating an unnatural 4-iodophenylalanine residue were prepared from chemically synthesized d- and l-proteins. Breakage of the C-I bonds in the quasi-racemic crystals facilitated structure determination by RIP. The crystal structure reveals a unique protein fold with six disulfide crosslinks, presenting a distinct electrostatic surface that may target the protein to microbial cell surfaces.

Radiation Damage and Racemic Protein Crystallography Reveal the Unique Structure of the GASA/Snakin Protein Superfamily

AbstractProteins from the GASA/snakin superfamily are common in plant proteomes and have diverse functions, including hormonal crosstalk, development, and defense. One 63‐residue member of this family, snakin‐1, an antimicrobial protein from potatoes, has previously been chemically synthesized in a fully active form. Herein the 1.5 Å structure of snakin‐1, determined by a novel combination of racemic protein crystallization and radiation‐damage‐induced phasing (RIP), is reported. Racemic crystals of snakin‐1 and quasi‐racemic crystals incorporating an unnatural 4‐iodophenylalanine residue were prepared from chemically synthesized d‐ and l‐proteins. Breakage of the C−I bonds in the quasi‐racemic crystals facilitated structure determination by RIP. The crystal structure reveals a unique protein fold with six disulfide crosslinks, presenting a distinct electrostatic surface that may target the protein to microbial cell surfaces.

Radiation-damage-induced phasing: a case study using UV irradiation with light-emitting diodes.

Exposure to X-rays, high-intensity visible light or ultraviolet radiation results in alterations to protein structure such as the breakage of disulfide bonds, the loss of electron density at electron-rich centres and the movement of side chains. These specific changes can be exploited in order to obtain phase information. Here, a case study using insulin to illustrate each step of the radiation-damage-induced phasing (RIP) method is presented. Unlike a traditional X-ray-induced damage step, specific damage is introduced via ultraviolet light-emitting diodes (UV-LEDs). In contrast to UV lasers, UV-LEDs have the advantages of small size, low cost and relative ease of use.

Practical Radiation Damage-Induced Phasing.

Although crystallographers typically seek to mitigate radiation damage in macromolecular crystals, in some cases, radiation damage to specific atoms can be used to determine phases de novo. This process is called radiation damage-induced phasing or "RIP." Here, we provide a general overview of the method and a practical set of data collection and processing strategies for phasing macromolecular structures using RIP.

Microfluidic sorting of protein nanocrystals by size for X-ray free-electron laser diffraction.

The advent and application of the X-ray free-electron laser (XFEL) has uncovered the structures of proteins that could not previously be solved using traditional crystallography. While this new technology is powerful, optimization of the process is still needed to improve data quality and analysis efficiency. One area is sample heterogeneity, where variations in crystal size (among other factors) lead to the requirement of large data sets (and thus 10–100 mg of protein) for determining accurate structure factors. To decrease sample dispersity, we developed a high-throughput microfluidic sorter operating on the principle of dielectrophoresis, whereby polydisperse particles can be transported into various fluid streams for size fractionation. Using this microsorter, we isolated several milliliters of photosystem I nanocrystal fractions ranging from 200 to 600 nm in size as characterized by dynamic light scattering, nanoparticle tracking, and electron microscopy. Sorted nanocrystals were delivered in a liquid jet via the gas dynamic virtual nozzle into the path of the XFEL at the Linac Coherent Light Source. We obtained diffraction to ∼4 Å resolution, indicating that the small crystals were not damaged by the sorting process. We also observed the shape transforms of photosystem I nanocrystals, demonstrating that our device can optimize data collection for the shape transform-based phasing method. Using simulations, we show that narrow crystal size distributions can significantly improve merged data quality in serial crystallography. From this proof-of-concept work, we expect that the automated size-sorting of protein crystals will become an important step for sample production by reducing the amount of protein needed for a high quality final structure and the development of novel phasing methods that exploit inter-Bragg reflection intensities or use variations in beam intensity for radiation damage-induced phasing. This method will also permit an analysis of the dependence of crystal quality on crystal size.

Towards RIP using free-electron laser SFX data.

Here, it is shown that simulated native serial femtosecond crystallography (SFX) cathepsin B data can be phased by rapid ionization of sulfur atoms. Utilizing standard software adopted for radiation-damage-induced phasing (RIP), the effects on both substructure determination and phasing of the number of collected patterns and fluences are explored for experimental conditions already available at current free-electron laser facilities.

Alternative phasing method in macromolecular crystallography

Selenium is the most widely used heavy atom for experimental phasing, either by single anomalous scattering (SAD) or multiple-wavelength anomalous diffraction (MAD) procedures. The use of the single isomorphous replacement (SIR) or single isomorphous replacement with anomalous scattering (SIRAS) phasing procedure with selenomethionine (Mse) containing proteins is not so commonly used, as it requires isomorphous native data. Several non-redundant X-ray diffraction data sets from various Mse derivatised protein crystals were collected at energies far below the absorption edge before and after exposing the crystal to ultraviolet (UV) radiation with 266 nm lasers. A detailed analysis revealed that significant changes in diffracted intensities were induced by ultraviolet irradiation whilst retaining crystal isomorphism. These intensity changes allowed the crystal structures to be solved by the radiation damage-induced phasing (RIP) technique [1]. These can be coupled with the anomalous signal from the dataset collected at the selenium absorption edge to obtain SIRAS phases in a UV-RIPAS phasing experiment [2]. Inspection of the crystal structures and electron-density maps demonstrated that covalent bonds between selenium and carbon at all sites located in the core of the proteins or in a hydrophobic environment were much more susceptible to UV radiation-induced cleavage than other bonds typically present in Mse proteins. The rapid UV radiation-induced bond cleavage opens a reliable new paradigm for phasing at synchrotron [1,2] and at in-house X-ray source [3].

Sulfur-SAD phasing and UV-RIP analysis on a single Cysteine bridge protein

The advantage of using the anomalous signal of sulfur for phase determination is that only a single, well-diffracting crystal is needed and that a native structure will be obtained. Using long-wavelength S-SAD to a resolution of 1.9 Å we have determined the novel structure of an 89 residue protein with only 2 Cysteines fixed in a disulfide bridge. To the best of our knowledge, the Bijvoet ratio in our example is one of the smallest for which a successful structure solution by S-SAD has been reported. Data were collected on 3 different volumes of a single crystal at beamline 14.1. at BESSY II, Berlin [1], at a wavelength of 1.8 Å. At this wavelength the maximum resolution obtainable was 1.9 Å. The data were processed in space group I222 with a low resolution R-factor of 3.2% and a multiplicity of 17. Based on an anomalous correlation coefficient cut off at 30% the signal extends to 2.6 Å. The sulfur substructure was determined using AutoSol/HYSS [2] showing a total of four clear sulfur positions in the asymmetric unit with a resulting FOM of 0.27 and a BAYES Coefficient of 0.36. The crystal has a solvent content of 62% and the structure reveals a dimer and large solvent channels. Density modification lead to well-defined electron density maps for the protein and associated solvent molecules. This example demonstrates that S-SAD phase determination can work with as little as one S-atom per 45 amino acid residues. Additionally, we performed a UV-RIP (ultraviolet radiation damage-induced phasing) experiment in which a dataset was collected before and after irradiating the crystal with a hard UV laser. An isomorphous difference map shows the clear disruption of both disulfide bridges and we are currently working on combined phasing using both anomalous and isomorphous differences based on the S-SAD and UV-RIP data.

Segmenting data sets for RIP

Specific radiation damage can be used for the phasing of macromolecular crystal structures. In practice, however, the optimization of the X-ray dose used to `burn' the crystal to induce specific damage can be difficult. Here, a method is presented in which a single large data set that has not been optimized in any way for radiation-damage-induced phasing (RIP) is segmented into multiple sub-data sets, which can then be used for RIP. The efficacy of this method is demonstrated using two model systems and two test systems. A method to improve the success of this type of phasing experiment by varying the composition of the two sub-data sets with respect to their separation by image number, and hence by absorbed dose, as well as their individual completeness is illustrated.

Single isomorphous replacement phasing of selenomethionine-containing proteins using UV-induced radiation damage

The most commonly used heavy-atom derivative, selenium, requires the use of a tunable beamline to access the Se K edge for experimental phasing using anomalous diffraction methods, whereas X-ray diffraction experiments for selenium-specific ultraviolet radiation-damage-induced phasing can be performed on fixed-wavelength beamlines or even using in-house X-ray sources. Several nonredundant X-ray diffraction data sets were collected from three different selenomethionine (Mse) derivatized protein crystals at energies far below the absorption edge before and after exposing the crystal to ultraviolet (UV) radiation using 266 nm lasers of flux density 1.7 × 10¹⁵ photons s⁻¹ mm⁻² for 10-50 min. A detailed analysis revealed that significant changes in diffracted intensities were induced by ultraviolet irradiation whilst retaining crystal isomorphism. These intensity changes allowed the crystal structures to be solved by the radiation-damage-induced phasing (RIP) technique. Inspection of the crystal structures and electron-density maps demonstrated that covalent bonds between selenium and carbon at all sites located in the core of the proteins or in a hydrophobic environment were much more susceptible to UV radiation-induced cleavage than other bonds typically present in Mse proteins. The rapid UV radiation-induced bond cleavage opens a reliable new paradigm for phasing when no tunable X-ray source is available. The behaviour of Mse derivatives of various proteins provides novel insights and an initial basis for understanding the mechanism of selenium-specific UV radiation damage.

Update on the tutorial for learning and teaching macromolecular crystallography

Two new experiments (single isomorphous replacement including anomalous-scattering effects and radiation damage-induced phasing) have been designed to complement the five experiments (sulfur single-wavelength anomalous diffraction, multiple-wavelength anomalous diffraction, molecular replacement, ion binding and ligand binding) of the first edition of the previously described tutorial for learning and teaching macromolecular crystallography [Faust, Panjikar, Mueller, Parthasarathy, Schmidt, Lamzin & Weiss (2008). J. Appl. Cryst. 41, 1161–1172]. Furthermore, the tutorial has been re-organized and in part re-written to reflect the comments and suggestions of users. The most significant overhaul was applied to the data-processing part of the tutorial. Nevertheless, the convenient features that all of the utilized proteins used are commercially available and that they can be easily and reproducibly crystallized and mounted for diffraction data collection have been retained. Also, for all of the seven experiments the raw diffraction images and the processed data are provided for illustrating and teaching the steps of data processing and structure determination.

Structure of SRP14 from theSchizosaccharomyces pombesignal recognition particle

The signal recognition particle (SRP) Alu domain has been implicated in translation elongation arrest in yeasts and mammals. Fission yeast SRP RNA is similar to that of mammals, but has a minimal Alu-domain RNA lacking two stem-loops. The mammalian Alu-domain proteins SRP9 and SRP14 bind their cognate Alu RNA as a heterodimer. However, in yeasts, notably Saccharomyces cerevisiae, SRP14 is thought to bind Alu RNA as a homodimer, the SRP9 protein being replaced by SRP21, the function of which is not yet clear. Structural characterization of the Schizosaccharomyces pombe Alu domain may thus help to identify the critical features required for elongation arrest. Here, the crystal structure of the SRP14 subunit of S. pombe SRP (SpSRP14) which crystallizes as a homodimer, is presented. Comparison of the SpSRP14 homodimer with the known structure of human SRP9/14 in complex with Alu RNA suggests that many of the protein-RNA contacts centred on the conserved U-turn motif are likely to be conserved in fission yeast. Initial attempts to solve the structure using traditional selenomethionine SAD labelling failed. However, two As atoms originating from the cacodylate buffer were found to make cysteine adducts and strongly contributed to the anomalous substructure. These adducts were highly radiation-sensitive and this property was exploited using the RIP (radiation-damage-induced phasing) method. The combination of SAD and RIP phases yielded an interpretable electron-density map. This example will be of general interest to crystallographers attempting de novo phasing from crystals grown in cacodylate buffer.

Differential specific radiation damage in the CuII-bound and PdII-bound forms of an α-helical foldamer: a case study of crystallographic phasing by RIP and SAD

The high photon flux at third-generation synchrotron sources can inflict significant primary radiation damage upon macromolecular crystals, even when the crystals are cryocooled. However, specific radiation-induced structural changes can be exploited for de novo phasing by an approach known as radiation damage-induced phasing (RIP). Here, RIP and single-wavelength anomalous dispersion (SAD) phasing were alternatively used to derive experimental phases to 1.2 A resolution for crystals of an alpha-helical 18-residue peptide, MINTS, which was derived from the neurotoxin apamin and the palladium-bound structure of which is now reported. Helix formation is induced by the binding of palladium (or copper) to two histidines spaced four residues apart, while two disulfide bonds tether the N-terminal helix to the C-terminal loop-like part of the peptide. Either RIP or SAD phasing of the palladium-bound and copper-bound forms of MINTS, which crystallized in different space groups, resulted in density maps of superb quality. Surprisingly, RIP phasing of the metal-bound complex structures of MINTS was a consequence of differential radiation damage, resting primarily on the reduction of the disulfide bonds in Pd-MINTS and on depletion of the metal sites in Cu-MINTS. Its miniprotein-like characteristics, versatile metal-binding properties and ease of crystallization suggest MINTS to be a convenient test specimen for methods development in crystallographic phasing based on either synchrotron or in-house X-ray diffraction data.

The Solution and Crystal Structures of a Module Pair from the Staphylococcus aureus-Binding Site of Human Fibronectin—A Tale with a Twist

An important goal of structural studies of modular proteins is to determine the inter-module orientation, which often influences biological function. The N-terminal domain of human fibronectin (Fn) is composed of a string of five type 1 modules (F1). Despite their small size, to date F1 modules have proved intractable to X-ray structure solution, although there are several NMR structures available. Here, we present the first structures (two X-ray models and an NMR-derived model) of the 2F13F1 module pair, which forms part of the binding site for Fn-binding proteins from pathogenic bacteria. The crystallographic structure determination was aided by the novel technique of UV radiation damage-induced phasing. The individual module structures are very similar in all three models. In the NMR structure and one of the X-ray structures, a similar but smaller interdomain interface than that observed previously for 4F15F1 is seen. The other X-ray structure has a different interdomain orientation. This work underlines the benefits of combining X-ray and NMR data in the studies of multi-domain proteins.

Phasing Macromolecular Structures with UV-Induced Structural Changes

Experimental phasing of macromolecular crystal structures relies on the accurate measurement of two or more sets of reflections from isomorphous crystals, where the scattering power of a few atoms is different for each set. Recently, it was demonstrated that X-ray-induced intensity differences can also contain phasing information, exploiting specific structural changes characteristic of X-ray damage. This method (radiation damage-induced phasing; RIP) has the advantage that it can be performed on a single crystal of the native macromolecule. However, a drawback is that X-rays introduce many small changes to both solvent and macromolecule. In this study, ultraviolet (UV) radiation has been used to induce specific changes in the macromolecule alone, leading to a larger contrast between radiation-susceptible and nonsusceptible sites. Unlike X-ray RIP, UV RIP does not require the use of a synchrotron. The method has been demonstrated for a series of macromolecules.

Radiation-induced site-specific damage of mercury derivatives: phasing and implications

The behavior of mercury-derivatized triclinic crystals of a 60 kDa protein target from the New York Structural GenomiX Research Consortium provides novel insights into the mechanism of heavy-atom-specific radiation damage and its potential exploitation for de novo structure solution. Despite significant anomalous signal, structure solution by classic SAD and MAD phasing approaches was not successful. A detailed analysis revealed that significant isomorphic variation of the diffracted intensities was induced by X-ray irradiation. These intensity changes allowed the crystal structure to be solved by the radiation-damage-induced phasing (RIP) technique. Inspection of the crystal structure and electron-density maps demonstrated that the covalent S-Hg bonds at all four derivatized cysteine sites were much more susceptible to radiation-induced cleavage than other bonds typically present in native proteins. A simple diagnostic is described to identify the fingerprint of such decay at the time of data collection/processing. The rapid radiation-induced decomposition of mercury adducts is consistent with the difficulties frequently associated with the experimental phasing of mercury derivatives and suggests a straightforward solution to overcome this limitation by radiation-damage-induced phasing with anomalous scattering (RIPAS). These results indicate that historically recalcitrant and newly emerging difficulties associated with Hg phasing should be revisited.

Improving radiation-damage substructures for RIP

Specific radiation damage can be used to solve macromolecular structures using the radiation-damage-induced phasing (RIP) method. The method has been investigated for six disulfide-containing test structures (elastase, insulin, lysozyme, ribonuclease A, trypsin and thaumatin) using data sets that were collected on a third-generation synchrotron undulator beamline with a highly attenuated beam. Each crystal was exposed to the unattenuated X-ray beam between the collection of a 'before' and an 'after' data set. The X-ray 'burn'-induced intensity differences ranged from 5 to 15%, depending on the protein investigated. X-ray-susceptible substructures were determined using the integrated direct and Patterson methods in SHELXD. The best substructures were found by downscaling the 'after' data set in SHELXC by a scale factor K, with optimal values ranging from 0.96 to 0.99. The initial substructures were improved through iteration with SHELXE by the addition of negatively occupied sites as well as a large number of relatively weak sites. The final substructures ranged from 40 to more than 300 sites, with strongest peaks as high as 57sigma. All structures except one could be solved: it was not possible to find the initial substructure for ribonuclease A, however, SHELXE iteration starting with the known five most susceptible sites gave excellent maps. Downscaling proved to be necessary for the solution of elastase, lysozyme and thaumatin and reduced the number of SHELXE iterations in the other cases. The combination of downscaling and substructure iteration provides important benefits for the phasing of macromolecular structures using radiation damage.

Phasing in the presence of radiation damage

In the accurate estimation of small signals, redundancy of observations is often seen as an essential tool for the experimenter. This is particularly true during macromolecular structure determination by single-wavelength anomalous dispersion (SAD), where the exploitable signal can be less than a few percent. At the most intense undulator synchrotron beamlines, the effect of radiation damage can be such that all usable signal is obscured. Here the magnitude of this effect in experiments performed at the Se K-edge is quantified. Six successive data sets were collected on the same crystal, interspersed with two exposures to the X-ray beam during which data were not collected. It is shown that the very first data set has excellent phasing statistics, whereas these statistics degrade for the later data sets. Merging several data sets into one, highly redundant, data set only gave moderate improvements as a result of the presence of radiation damage. Part of the damage could be corrected for using a linear interpolation scheme. Interpolation of the data to a low-dose as well as to a high-dose data set allowed us to combine the SAD method with the radiation-damage induced phasing (RIP) technique, which further improved the experimental phases, especially after density modification. Some recommendations are given on how to mitigate the effect of radiation damage during structure determination.