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Abstract: Many secreted eukaryotic proteins are N-glycosylated with oligosaccharides composed of a high-mannose N-glycan core and, in the specific case of yeast cell-wall proteins, an extended α-1,6-mannan backbone carrying a number of α-1,2- and α-1,3-mannose substituents of varying lengths. α-Mannosidases from CAZy family GH92 release terminal mannose residues from these N-glycans, providing access for the α-endomannanases, which then degrade the α-mannan backbone. Most characterized GH92 α-mannosidases consist of a single catalytic domain, while a few have extra domains including putative carbohydrate-binding modules (CBMs). To date, neither the function nor the structure of a multi-domain GH92 α-mannosidase CBM has been characterized. Here, the biochemical investigation and crystal structure of the full-length five-domain GH92 α-1,2-mannosidase from Neobacillus novalis (NnGH92) with manno­imidazole bound in the active site and an additional mannoimidazole bound to the N-terminal CBM32 are reported. The structure of the catalytic domain is very similar to that reported for the GH92 α-mannosidase Bt3990 from Bacteroides thetaiotaomicron, with the substrate-binding site being highly conserved. The function of the CBM32s and other NnGH92 domains was investigated by their sequential deletion and suggested that whilst their binding to the catalytic domain was crucial for the overall structural integrity of the enzyme, they appear to have little impact on the binding affinity to the yeast α-mannan substrate. These new findings provide a better understanding of how to select and optimize other multi-domain bacterial GH92 α-mannosidases for the degradation of yeast α-mannan or mannose-rich glycans.

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Abstract: Tetragonal CuMnAs is a room temperature antiferromagnet with an electrically reorientable Néel vector and a Dirac semimetal candidate. Direct measurements of the electronic structure of single-crystalline thin films of tetragonal CuMnAs using angle-resolved photoemission spectroscopy (ARPES) are reported, including Fermi surfaces (FS) and energy-wavevector dispersions. After correcting for a chemical potential shift of ≈− 390 meV (hole doping), there is excellent agreement of FS, orbital character of bands, and Fermi velocities between the experiment and density functional theory calculations. In addition, 2×1 surface reconstructions are found in the low energy electron diffraction (LEED) and ARPES. This work underscores the need to control the chemical potential in tetragonal CuMnAs to enable the exploration and exploitation of the Dirac fermions with tunable masses, which are predicted to be above the chemical potential in the present samples.

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Abstract: In this thesis, the static and dynamic properties of magnetic multilayer samples were studied using a variety of experimental techniques, based both at Exeter and the Diamond Light Source (DLS) and Advanced Light Source (ALS) synchrotron facilities. The exchange interaction, which acts to align spins, is a fundamental part in these magnetic multilayer samples. First, the glancing angle deposition (GLAD) technique was investigated as a tool for creating magnetic multilayers with exciting new exchange interactions. For this, Co thin films were grown by DC magnetron sputtering to tailor the magnetic anisotropy of the samples. These Co samples were structurally characterized using x-ray diffraction (XRD) and transmission electron microscopy (TEM). Vibrating sample magnetometry (VSM) was then performed to investigate the magnetic properties of the thin films as a result of the GLAD technique. From this, the necessary conditions for effective anisotropy control using the GLAD technique were identified. Synchrotron x-ray measurements, such as x-ray magnetic circular / linear dichroism (XMCD/XMLD) for static measurements, are vital for investigating magnetic multilayer samples with elemental resolution. To add depth-sensitivity to the synchrotron measurements, the idea of an ultra-thin Mn “spy layer” was investigated by inserting different thicknesses (tMn) of Mn into the NiFe layer in a FePt / NiFe bilayer. The effect on the static magnetic properties was studied using VSM and XMCD hysteresis loops before structural information was obtained using scanning transmission electron microscopy (STEM). The magnetization dynamics were probed using vector network analyzer ferromagnetic resonance (VNA-FMR) and element resolved x-ray ferromagnetic resonance (XFMR) measurements. From this, the ideal “spy layer” thickness of Mn was found to lie in the region 0Å < tMn < 5Å . Spin currents are a dynamic process found in magnetic multilayers and are driven by the exchange interaction. The measurement of a transverse charge current generated via the inverse spin Hall effect (ISHE) has become the principal technique for observing spin currents. During ISHE measurements, parasitic microwave effects were observed and a method to separate out the inverse spin Hall effect was identified. This method was then tested for a reference YIG / Pt bilayer. A more complex NiFe / NiO / Pd / FeCo sample was then studied using this procedure and the ISHE voltage was identified, despite the presence of additional parasitic effects. In addition to the DC spin current component, there is an AC spin current contribution. The AC spin current component was also investigated for the NiFe / NiO / Pd / FeCo sample series using XMCD, XMLD and XFMR measurements. The XMCD and XMLD data revealed the Ni and (Fe)Co spins possess perpendicular in-plane coupling relative to the magnetic moments within the NiO layer. To understand the magnetization dynamics in these samples, an evanescent spin wave model was invoked. This provides crucial insights for interpreting spin current propagation through NiO. Through the combination of work described above, new avenues for the fabrication of magnetic multilayers and the measurement of the magnetization dynamics in such systems are presented to yield a more complete understanding of the crucial role of the exchange interaction in the magnetization dynamics of magnetic multilayers.

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Abstract: Macroscopic scale hollow microcrystals are a promising group of materials for gas and liquid uptake as well as sensing. In this contribution we describe the structure of hollow hexagonal cross-section crystals formulated as salts of a silicon catecholate anion and a tetramethylenediamine (TEMED) cation. Using a combination of X-ray single crystal diffraction, Raman spectroscopy and quantum chemistry we explore the structural properties of the hollow microcrystals. With the X-ray structural data as a starting point and assisted with quantum chemistry we compute Raman tensors to fit polarisation sensitive spectral responses and predict the orientation and packing of unit cells in respect to the long and short axis of the synthesised microcrystals. Using these newly developed methods for predicting molecular Raman responses in space with dependence on local orientation, we present the quantitative analysis of experimental Raman images of both hexagonal and tetragonal cross section hollow microcrystals formed from silicon catecholate anions using different amines as counterions. We describe the distributions of chemical components at the surfaces and edges of microcrystals, address the effect of catcholate hydrophobicity on water uptake and discuss possible strategies in chemical and post-assembly modifications to widen the functional properties of this group of environmentally friendly silicon organic framework (SOF) materials.

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Abstract: Lysine acetylation in histone tails is a key post-translational modification that controls transcription activation. Histone deacetylase complexes remove histone acetylation, thereby repressing transcription and regulating the transcriptional output of each gene. Although these complexes are drug targets and crucial regulators of organismal physiology, their structure and mechanisms of action are largely unclear. Here, we present the structure of a complete human SIN3B histone deacetylase holo-complex with and without a substrate mimic. Remarkably, SIN3B encircles the deacetylase and contacts its allosteric basic patch thereby stimulating catalysis. A SIN3B loop inserts into the catalytic tunnel, rearranges to accommodate the acetyl-lysine moiety, and stabilises the substrate for specific deacetylation, which is guided by a substrate receptor subunit. Our findings provide a model of specificity for a main transcriptional regulator conserved from yeast to human and a resource of protein-protein interactions for future drug designs.