Coherent diffraction of single Rice Dwarf virus particles using hard X-rays at the Linac Coherent Light Source

Single particle diffractive imaging data from Rice Dwarf Virus (RDV) were recorded using the Coherent X-ray Imaging (CXI) instrument at the Linac Coherent Light Source (LCLS). RDV was chosen as it is a wellcharacterized model system, useful for proof-of-principle experiments, system optimization and algorithm development. RDV, an icosahedral virus of about 70 nm in diameter, was aerosolized and injected into the approximately 0.1 mu m diameter focused hard X-ray beam at the CXI instrument of LCLS. Diffraction patterns from RDV with signal to 5.9 angstrom ngstrom were recorded. The diffraction data are available through the Coherent X-ray Imaging Data Bank (CXIDB) as a resource for algorithm development, the contents of which are described here.11Ysciescopu

X-ray screening identifies active site and allosteric inhibitors of SARS-CoV-2 main protease

The coronavirus disease (COVID-19) caused by SARS-CoV-2 is creating tremendous human suffering. To date, no effective drug is available to directly treat the disease. In a search for a drug against COVID-19, we have performed a high-throughput X-ray crystallographic screen of two repurposing drug libraries against the SARS-CoV-2 main protease (M^(pro)), which is essential for viral replication. In contrast to commonly applied X-ray fragment screening experiments with molecules of low complexity, our screen tested already approved drugs and drugs in clinical trials. From the three-dimensional protein structures, we identified 37 compounds that bind to M^(pro). In subsequent cell-based viral reduction assays, one peptidomimetic and six non-peptidic compounds showed antiviral activity at non-toxic concentrations. We identified two allosteric binding sites representing attractive targets for drug development against SARS-CoV-2

Optimizing the geometry of aerodynamic lens injectors for single-particle coherent diffractive imaging of gold nanoparticles

Single-particle x-ray diffractive imaging (SPI) of small (bio-)nanoparticles (NPs) requires optimized injectors to collect sufficient diffraction patterns to reconstruct the NP structure with high resolution. Typically, aerodynamic-lens-stack injectors are used for single NP injection. However, current injectors were developed for larger NPs (100 nm) and their ability to generate high-density NP beams suffers with decreasing NP size. Here, an aerodynamic-lens-stack injector with variable geometry and the geometry-optimization procedure are presented. The optimization for 50 nmgold NP (AuNP) injection using a numerical simulation infrastructure capable of calculating the carrier gas flow and the particle trajectories through the injector is introduced. The simulations are experimentally validated using spherical AuNPs and sucrose NPs. In addition, the optimized injector is compared to the standard-installation “Uppsala-injector” for AuNPs and results for these heavy particles show a shift in the particle-beam focus position rather than a change in beam size, which results in a lower gas background for the optimized injector. Optimized aerodynamic-lens stack injectors will allow to increase NP beam density, reduce the gas background, discover the limits of current injectors, and contribute to structure determination of small NPs using SPI

Optimizing the geometry of aerodynamic lens injectors for single-particle coherent diffractive imaging of gold nanoparticles

Single-particle x-ray diffractive imaging (SPI) of small (bio-)nanoparticles (NPs) requires optimized injectors to collect sufficient diffraction patterns to reconstruct the NP structure with high resolution. Typically, aerodynamic-lens-stack injectors are used for single NP injection. However, current injectors were developed for larger NPs (100 nm) and their ability to generate high-density NP beams suffers with decreasing NP size. Here, an aerodynamic-lens-stack injector with variable geometry and the geometry-optimization procedure are presented. The optimization for 50 nm gold NP (AuNP) injection using a numerical simulation infrastructure capable of calculating the carrier gas flow and the particle trajectories through the injector is introduced. The simulations are experimentally validated using spherical AuNPs and sucrose NPs. In addition, the optimized injector is compared to the standard-installation “Uppsala-injector” for AuNPs and results for these heavy particles show a shift in the particle-beam focus position rather than a change in beam size, which results in a lower gas background for the optimized injector. Optimized aerodynamic-lens stack injectors will allow to increase NP beam density, reduce the gas background, discover the limits of current injectors, and contribute to structure determination of small NPs using SPI

DNA-Origami-Assisted Flow-Aligned Single-Particle Diffractive Imaging using XFEL Pulses

Outrunning radiation damage, highly intense femtosecond pulses of X-ray free-electron lasers (XFELs) open up the possibility of structure determination of macromolecules to viruses at room temperature, by aggregating diffraction patterns recorded from uncrystallized single-particles. A key challenge in XFEL single-particle diffractive imaging (SPI) is to either constrain the orientation of the particle or to determine it from each of the very noisy weak diffraction patterns. Here we report a unique approach to address these challenges using structural DNA nanotechnology. A DNA-origami “rigid tail” is site-specifically attached to the macromolecule to flow-align it in a thin liquid jet, and also provides a strong holographic reference. In a proof-of-principle study, the computational design and production of the DNA-origami-target construct has been achieved and the experimental results obtained from the Linac Coherent Light Source (LCLS), USA show the alignment of the target single-particle, consistent with simulations, at extremely low concentrations approaching single-molecule in the interaction region with the nanofocus hard X-ray laser beam, in a sum of as few as a thousand single-shots. The results open up the possibility of single-molecule diffractive imaging in solution with XFEL pulses. Acknowledgements: The Human Frontier Science Program (RGP0010/2017)

Femtosecond Single-Particle Diffractive Imaging of 3D DNA-Origami Molecular Scaffolds with XFEL Pulses

Single-particle diffractive imaging is one of the key foundational goals behind the establishment of X-ray Free-Electron Laser (XFEL) facilities. Outrunning radiation damage, extremely intense femtosecond XFEL pulses open up the possibility of imaging uncrystallized aperiodic single-particles frozen in time at room-temperature at the timescales of atomic and electronic motions and thus enabling the capturing of complete energy landscape of molecules both at ground and excited states with sufficiently large data. Despite the current sample-delivery and background scattering challenges, there has been a steady progress in XFEL-single-particle imaging (XFEL-SPI), especially with large symmetric viruses. As a step towards XFEL imaging of single-macromolecules and small-proteins, here we report the coherent diffractive imaging of 3D DNA-origami molecular scaffolds using the soft-X-ray pulses at the European X-ray Free-Electron Laser (EuXFEL). Asymmetric and symmetric 3D DNA-origami scaffold structures were nebulized and delivered to the XFEL beam using an aerodynamic lens stack. The aerosolized DNA-origami structures were intact, and tens-of-thousands of diffraction patterns with expected size and shape matching the simulations of corresponding cryo-EM structures were collected, which were 3D mergeable in the reciprocal space with the expand-maximize-compression (EMC) algorithm. This first demonstration of imaging intact electrospray-aerosolized 3D DNA-origami structures is an important first step towards exploring the application of DNA-origami in XFEL diffractive imaging, especially as, but not-limited-to, molecular scaffolds for small proteins, as references in holographic single-particle imaging or as carriers of strongly-scattering nanoparticle references, and also in time-resolved diffractive imaging of photonic/photoactivatable DNA-origami machines

Femtosecond x-ray diffraction from an aerosolized beam of protein nanocrystals

We demonstrate near-atomic-resolution Bragg diffraction from aerosolized single granulovirus crystals using an x-ray free-electron laser. The form of the aerosol injector is nearly identical to conventional liquid-microjet nozzles, but the x-ray-scattering background is reduced by several orders of magnitude by the use of helium carrier gas rather than liquid. This approach provides a route to study the weak diffuse or lattice-transform signal arising from small crystals. The high speed of the particles is particularly well suited to upcoming MHz-repetition-rate x-ray free-electron lasers

Correlations in Scattered X-Ray Laser Pulses Reveal Nanoscale Structural Features of Viruses

We use extremely bright and ultrashort pulses from an x-ray free-electron laser (XFEL) to measure correlations in x rays scattered from individual bioparticles. This allows us to go beyond the traditional crystallography and single-particle imaging approaches for structure investigations. We employ angular correlations to recover the three-dimensional (3D) structure of nanoscale viruses from x-ray diffraction data measured at the Linac Coherent Light Source. Correlations provide us with a comprehensive structural fingerprint of a 3D virus, which we use both for model-based and ab initio structure recovery. The analyses reveal a clear indication that the structure of the viruses deviates from the expected perfect icosahedral symmetry. Our results anticipate exciting opportunities for XFEL studies of the structure and dynamics of nanoscale objects by means of angular correlations

Macromolecular diffractive imaging using imperfect crystals

The three-dimensional structures of macromolecules and their complexes are mainly elucidated by X-ray protein crystallography. A major limitation of this method is access to high-quality crystals, which is necessary to ensure X-ray diffraction extends to sufficiently large scattering angles and hence yields information of sufficiently high resolution with which to solve the crystal structure. The observation that crystals with reduced unit-cell volumes and tighter macromolecular packing often produce higher-resolution Bragg peaks suggests that crystallographic resolution for some macromolecules may be limited not by their heterogeneity, but by a deviation of strict positional ordering of the crystalline lattice. Such displacements of molecules from the ideal lattice give rise to a continuous diffraction pattern that is equal to the incoherent sum of diffraction from rigid individual molecular complexes aligned along several discrete crystallographic orientations and that, consequently, contains more information than Bragg peaks alone. Although such continuous diffraction patterns have long been observed—and are of interest as a source of information about the dynamics of proteins—they have not been used for structure determination. Here we show for crystals of the integral membrane protein complex photosystem II that lattice disorder increases the information content and the resolution of the diffraction pattern well beyond the 4.5 $\mathring{A}$ limit of measurable Bragg peaks, which allows us to phase the pattern directly. Using the molecular envelope conventionally determined at 4.5 $\mathring{A}$ as a constraint, we obtain a static image of the photosystem II dimer at a resolution of 3.5 $\mathring{A}$. This result shows that continuous diffraction can be used to overcome what have long been supposed to be the resolution limits of macromolecular crystallography, using a method that exploits commonly encountered imperfect crystals and enables model-free phasing

Femtosecond structural dynamics drives the trans/cis isomerization in photoactive yellow protein.

A variety of organisms have evolved mechanisms to detect and respond to light, in which the response is mediated by protein structural changes after photon absorption. The initial step is often the photoisomerization of a conjugated chromophore. Isomerization occurs on ultrafast time scales and is substantially influenced by the chromophore environment. Here we identify structural changes associated with the earliest steps in the trans-to-cis isomerization of the chromophore in photoactive yellow protein. Femtosecond hard x-ray pulses emitted by the Linac Coherent Light Source were used to conduct time-resolved serial femtosecond crystallography on photoactive yellow protein microcrystals over a time range from 100 femtoseconds to 3 picoseconds to determine the structural dynamics of the photoisomerization reaction