J. Bernard Heymann

Images in the electron microscope are formed by electron scattering and focusing. The spherical geometry of these processes gives rise to two coherent, conjugate spherical wave fronts, known as Ewald spheres. These spheres are associated with the two halves of the contrast transfer function (CTF), and their widths are determined by the focal gradient through the specimen. To properly correct for the CTF, each half of the CTF must be applied to an image individually and integrated into the reconstruction into the corresponding Ewald sphere. Theory indicates that this dual Ewald sphere reconstruction method should recover the maximal amount of information possible. This method was compared to the other reconstruction methods commonly used: the projection approximation (ignoring the Ewald sphere), the simple insertion and the single sideband methods. In simulated reconstructions the dual Ewald sphere method recovered the most information when the correct half of the CTF is matched to the corresponding Ewald sphere. If the wrong half is matched, the result worse than the projection approximation method. Examining reconstructions from real data indicated that the dual Ewald sphere method performs at least as well as the simple insertion method, but not as good as in simulations. The likely reason is the two-fold ambiguity in the assigned orientations of the particle images, which remains an issue to pursue in further studies. In conclusion, the dual Ewald sphere reconstruction method may offer the best way to calculate very high resolution reconstructions when the micrograph quality warrants it.

CryoEM reconstructions must be performed along the Ewald spheres to achieve resolutions beyond the projection approximation limit. The linear theory of image formation models the scattering from the specimen and focusing by the objective lens as two conjugate Ewald spheres that correspond to the two halves of the contrast transfer function (CTF). A focal series of micrographs mimics the focal gradient inherent in the Ewald wavefront, and its 3D Fourier transform provides a visual representation of the conjugate Ewald spheres. To better understand the nature of the Ewald spheres, focal series of graphene oxide as a thin specimen and platinum–iridium as a strongly scattering specimen were acquired. An algorithm was developed to fit and correct the CTF of the whole focal series. Correcting for the one half of the CTF flattens one of the Ewald spheres in the 3D transform, while doubling the curvature of the other. This yields the best representation of the Ewald sphere and thus the `exit wave', and can be performed on every single micrograph. The 2D reconstruction as the sum of the partial CTF corrected transforms recovers missing information in the individual micrographs and increases the signal-to-noise ratio. Iterative refinement of the reconstructed image against the amplitudes of the original focal series recovers the second Ewald sphere only at frequencies where the two spheres overlap, but introduces artifacts. The conclusion is that the correct way to account for the Ewald spheres in cryoEM is to apply the two halves of the CTF to a particle image and incorporate the two results into their corresponding spheres within the cryoEM reconstruction.

Herpesviruses are prevalent infectious agents in humans, with complex structures and life cycles. The viability and detail of a model of capsid assembly and maturation can now be examined against the recently available mature herpesvirus capsids structures. The first large assembly product is the icosahedral procapsid with an outer shell composed of major capsid proteins (MCPs) connected by triplexes (heterotrimers composed of one Tri1 protein and two Tri2 proteins), and an inner shell of scaffold proteins. The asymmetric triplexes have specific and conserved orientations, suggesting a key role in assembly. In the mature capsid structures, triplexes bound to three MCPs may represent an assembly unit where, in most cases, the N-terminus of one MCP wraps around the E-loop of another MCP. The model accommodates the incorporation of a portal into capsid, required for genome encapsidation and viral viability. Cleavage of the scaffold triggers maturation of procapsid. Each of the MCPs rotates mostly as a rigid body, except for the flexible peripheral parts that remodel to close the capsid inner surface. Angularization of the capsid shifts the portal outward to a better contact with the capsid shell. Understanding these events in the herpesvirus life cycle to atomic detail could facilitate the development of drugs that uniquely target assembly and maturation.

Herpesviruses are prevalent infectious agents in humans, with complex structures and life cycles. The viability and detail of a model of capsid assembly and maturation can now be examined against the recently available mature herpesvirus capsids structures. The first large assembly product is the icosahedral procapsid with an outer shell composed of major capsid proteins (MCPs) connected by triplexes, and an inner shell of scaffold proteins. The asymmetric triplexes have specific and conserved orientations, suggesting a key role in assembly. In the mature capsid structures, triplexes bound to three MCPs may represent an assembly unit where, in most cases, the N-terminus of one MCP wraps around the E-loop of another MCP. The model accommodates the incorporation of a portal into capsid, required for genome encapsidation and viral viability. Cleavage of the scaffold triggers maturation of procapsid. Each of the MCPs rotates mostly as a rigid body, except for the flexible peripheral parts that remodel to close the capsid floor. Angularization of the capsid shifts the portal outward to a better contact with the capsid shell. Understanding these events in the herpesvirus life cycle to atomic detail will facilitate the development of drugs that uniquely target assembly and maturation.

In January 2020, a workshop was held at EMBL-EBI (Hinxton, UK) to discuss data requirements for the deposition and validation of cryoEM structures, with a focus on single-particle analysis. The meeting was attended by 47 experts in data processing, model building and refinement, validation, and archiving of such structures. This report describes the workshop's motivation and history, the topics discussed, and the resulting consensus recommendations. Some challenges for future methods-development efforts in this area are also highlighted, as is the implementation to date of some of the recommendations.

From the first isolation of the cystovirus bacteriophage Φ6 from Pseudomonas syringae 50 years ago, we have progressed to a better understanding of the structure and transformations of many parts of the virion. The three-layered virion, encapsulating the tripartite double-stranded RNA (dsRNA) genome, breaches the cell envelope upon infection, generates its own transcripts, and coopts the bacterial machinery to produce its proteins. The generation of a new virion starts with a procapsid with a contracted shape, followed by the packaging of single-stranded RNA segments with concurrent expansion of the capsid, and finally replication to reconstitute the dsRNA genome. The outer two layers are then added, and the fully formed virion released by cell lysis. Most of the procapsid structure, composed of the proteins P1, P2, P4, and P7 is now known, as well as its transformations to the mature, packaged nucleocapsid. The outer two layers are less well-studied. One additional study investigated the binding of the host protein YajQ to the infecting nucleocapsid, where it enhances the transcription of the large RNA segment that codes for the capsid proteins. Finally, I relate the structural aspects of bacteriophage Φ6 to those of other dsRNA viruses, noting the similarities and differences.

From the first isolation of the cystovirus bacteriophage Φ6 from Pseudomonas syringae 50 years ago, we have progressed to a better understanding of the structure and transformations of the many parts of the virion. The three-layered virion encapsulating the tripartite double stranded RNA (dsRNA) genome, breaches the cell envelope on infection, generates its own transcripts, and coopts the bacterial machinery to produce its proteins. The generation of new virions starts with a procapsid with a contracted shape, followed by packaging single stranded RNA segments with concurrent expansion of the capsid, and finally replication to reconstitute the dsRNA genome. The outer two layers are then added, and the fully formed virions released by cell lysis. Most of the procapsid structure composed of the proteins P1, P2, P4 and P7 is now known, as well as its transformations to the mature, packaged nucleocapsid. The outer two layers are less well studied. One additional study investigated the binding of the host protein YajQ to the infecting nucleocapsid, where it enhances the transcription of the large RNA segment that codes for the capsid proteins. Finally, we relate the structural aspects of bacteriophage Φ6 top those of other dsRNA viruses, noting the similarities and differences.

In our quest to solve biomolecular structures to higher resolutions in cryoEM, care must be taken to deal with all aspects of image formation in the electron microscope. One of these is the Ewald sphere/focus gradient that derives from the scattering geometry in the microscope and its implications for recovering high resolution and handedness information. While several methods to deal with it has been proposed and implemented, there are still questions as to the correct approach. At the high acceleration voltages used for cryoEM, the traditional projection approximation that ignores the Ewald sphere breaks down around 2-3 Å and with large particles. This is likely not crucial for most biologically interesting molecules, but is required to understand detail about catalytic events, molecular orbitals, orientation of bound water molecules, etc. Through simulation I show that integration along the Ewald spheres in frequency space during reconstruction, the “simple insertion method” is adequate to reach resolutions to the Nyquist frequency. Both theory and simulations indicate that the handedness information encoded in such phases is irretrievably lost in the formation of real space images. The conclusion is that correct reconstruction along the Ewald spheres avoids the limitations of the projection approximation.