Radiation Hardness of Si Compared to 4H-SiC for Betavoltaics Assessed by Accelerated Aging Using an Electron Beam System
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Near-surface layers in Zr-18%Nb alloy were modified using ultrasonic impact treatment (UIT). The effects of the UIT processing time on a microstructural formation, omega/alpha precipitations, microhardness and corrosion are analyzed. XRD analysis, TEM and SEM observations and EDX characterization allow establishing the links between the microstructure, microhardness and corrosion behavior of the surface layers formed. At the strain extent up to e ≈ 0.3, structural formation occurs under influence of deformation induced heating, which facilitates omega precipitation in beta phase and mechanically induced oxygen transport and oxide formation. XRD analysis reveals moderate compressive residual stresses (− 160 MPa) and pronounced {110} texture after the UIT process. Generation of dislocations and hindering of their movement by nanoscale omega precipitates manifest themselves as the broadening of diffraction peaks occurred mainly owing to the lattice microstrains, and they provide marked strain hardening. The enhanced anticorrosion properties of Zr-18%Nb alloy in saline solution were concluded to be a result of the formation of a protective oxide film, {110} texture and compressive stresses.
This paper is focused on the effects of the separately applied laser heat treatment (LHT) and ultrasonic impact treatment (UIT) and the combined LHT + UIT process on the wear and friction behaviors of the hardened surface layers of the tool steel AISI D2. In comparison with the initial state, wear losses of the treated specimens after long-term wear tests were decreased by 68, 41, and 77% at the LHT, UIT, and combined LHT + UIT processes, respectively. The Abbott–Firestone bearing curves were used to analyze the material ratio and functional characterization (bearing capacity and oil capacitance) of the studied surface specimens. The wear losses registered after short (15 min) tests correlate well with the changes in experimental surface roughness Ra, and the predictive Rpk, and bearing capacity B{sub C} parameters, respectively, evaluated using the Abbott–Firestone curves and Kragelsky–Kombalov formula. The wear losses after the long-term (45 min) tests are in good correlation with the reciprocal surface microhardness HV and with the W{sub L} and W{sub P} wear parameters, respectively, estimated using Archard–Rabinowicz formula and complex roughness-and-strength approach. The observed HV increase is supported by nanotwins (LHT), by dense dislocation nets (UIT), and by dislocation cells/nanograins fixed with fine carbides (LHT + UIT) formed in the surface layers of the steel.
The crystallization behaviors and thermal stability of (Al{sub 87}Y{sub 8}Ni{sub 5}){sub 100−x}Sc{sub x} (x = 0, 1.0, 1.5) amorphous ribbons and alloy rods, produced by roller melt-spinning method and inductance casting, were investigated mainly by x-ray diffractometry (XRD) and differential scanning calorimetry (DSC). The glass transition temperatures of the (Al{sub 87}Y{sub 8}Ni{sub 5}){sub 99.0}Sc{sub 1.0} and (Al{sub 87}Y{sub 8}Ni{sub 5}){sub 98.5}Sc{sub 1.5} alloy ribbons were found to be 201 and 197 °C, respectively. Furthermore, the melting temperatures of the alloy ribbons decreased with the Sc content. This revealed that the glass-forming ability (GFA) of the metallic glass increased with increasing Sc content. Crystallization of (Al{sub 87}Y{sub 8}Ni{sub 5}){sub 100−x}Sc{sub x} (x = 0, 1.0, 1.5) amorphous ribbons occurred in the temperature range of 200 to 400 °C in three exothermic reaction stages. The peak temperatures of these three crystallization reactions shifted to higher temperatures at higher heating rates. The kinetic parameters for the first crystallization reaction, determined by Kissinger method, revealed that adding 1.5 at.% Sc increased the activation energy for crystallization from 158 to 167 kJ/mol. On the other hand, the cross-section morphology of the three different alloys revealed that a fully amorphous outer region and a partially crystallized core region formed in each alloy rod. It was also found that the thickness of the amorphous region increased with the Sc content, revealing a positive effect of Sc on the GFA.
Hypereutectoid SAE 52100 steel is extensively used in bearing applications. Microstructure modification in terms of dislocation martensite and carbide refinement was achieved for SAE 52100 steel through a simple duplex heat treatment. Refinement of prior austenite grains to less than 5 μm resulted in the conversion of conventional high-carbon twinned martensite to dislocation martensite. The concurrent refinement of austenite grains and carbide precipitates was accomplished by high-temperature austenitization followed by low-temperature tempering. This resulted in nanoscale nonstoichiometric ε-carbides within a heavily twinned martensitic structure. These nanoscale carbides acted as grain boundary pinning agents after their transformation to θ-carbides during the final austenitization process. The resulting microstructure was characterized by a fine dispersion of θ-carbides within dislocation martensite and showed roughly 24% increase in tensile strength and 30% better wear resistance compared to conventional structure.
To improve the surface properties and performance, a grain-refined surface layer was produced on AZ31B Mg alloy by a newly developed surface nano-crystallization and hardening process called surface mechanical rolling grinding treatment (SMRGT). The grain size refinement and minimal surface hardening were confirmed by the microstructure observations, XRD results and microhardness tests and were attributed to the multipass small strain-induced plastic deformation of the material during the SMRGT process. A nano-grain surface layer (average grain size of ~ 100 nm) and a graded microhardness variation (average ~ 113 HV adjacent to surface) along the thickness direction were generated. The E{sub corr} values of the as-SMRGTed samples were − 1.43 ± 0.03 and − 1.42 ± 0.02 V, increasing by ~ 30-40 mV compared with the values of the as-received (AR) sample (− 1.46 ± 0.02 V), corresponding to i{sub corr} ranging from 3.0 × 10{sup −5} to 1.0 × 10{sup −5} and 5.0 × 10{sup −6} A/cm{sup 2}, respectively. Charge transfer resistance (R{sub ct}) increased from 93.4 to 292.4 and 578.3 Ω (~ 3-6 times) with the increasing number of SMRGT passes. The corrosion resistance improvement was attributed mainly to the dramatic strain-induced surface grain refinement and minimal surface hardening that give rise to a more smooth and densely packed surface state.
The emission/ionization process under massive argon cluster bombardment was investigated by measuring the internal energy distributions of a series of benzylpyridinium ions. Argon clusters with kinetic energies between 10 and 20 keV and cluster sizes ranging from 500 to 10,000 were used to establish the influence of their size, energy, and velocity on the internal energy distribution of the secondary ions. It is shown that the internal energy distribution of secondary ions principally depends on the energy per atom or the velocity of the cluster ion beam (E/n ∝ v{sup 2}). Under low energy per atom (E/n ˂ 10 eV), the mean internal energy and fragmentation yield increase rapidly with the incident energy of individual constituents. Beyond 10 eV/atom impact (up to 40 eV/atom), the internal energy reaches a plateau and remains constant. Results were compared with those generated from bismuth cluster impacts for which the mean internal energies correspond well to the plateau values for argon clusters. However, a significant difference was found between argon and bismuth clusters concerning the damage or disappearance cross section. A 20 times smaller disappearance cross section was measured under 20 keV Ar{sub 2000}{sup +} impact compared to 25 keV Bi{sub 5}{sup +} bombardment, thus quantitatively showing the low damage effect of large argon clusters for almost the same molecular ion yield. .
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Insight into the spatial ordering and dynamics of structural heterogeneity in materials is at the heart of understanding their structure and function. X-ray photon correlation spectroscopy (XPCS) measures the dynamic structure factor providing S(Q,t) information on the spontaneous low-energy dynamics intrinsic to many materials. Combined with in situ and in operando capabilities, XPCS provides unique insight into a variety of scientific areas, including phase separation in binary alloys, aging in metallic glasses, surface dynamics during growth, domain wall dynamics in ferroic complex oxides and charge and spin density wave motion in quantum materials. In conclusion, this review summarizes some recent XPCS work in these areas and discusses scientific opportunities that will be made possible with the many-fold increase in coherent flux provided by the world-wide construction and commissioning of X-ray sources based on multi-bend achromat (MBA) storage ring (SR) lattices and high repetition rate free electron lasers (FELs).
Reconstructing hadron spectral functions through Euclidean correlation functions are of the important missions in lattice QCD calculations. However, in a Källen–Lehmann (KL) spectral representation, the reconstruction is observed to be ill-posed in practice. It is usually ascribed to the fewer observation points compared to the number of points in the spectral function. In this paper, by solving the eigenvalue problem of continuous KL convolution, we show analytically that the ill-posedness of the inversion is fundamental and it exists even for continuous correlation functions. We discussed how to introduce regulators to alleviate the predicament, in which include the Artificial Neural Networks (ANNs) representations recently proposed by the Authors in another study. The uniqueness of solutions using ANNs representations is manifested analytically and validated numerically. Reconstructed spectral functions using different regularization schemes are also demonstrated, together with their eigen-mode decomposition. We observe that components with large eigenvalues can be reliably reconstructed by all methods, whereas those with low eigenvalues need to be constrained by regulators.
Desalination of water containing high concentrations of calcium, dissolved carbon dioxide, sulfate, silica and other sparingly soluble salts is difficult because of the scaling potential. An innovative pre-treatment scheme was investigated at bench scale that selectively removes these constituents and produces a soft water to enable desalination with high feed water recovery. The process first removes dissolved carbon dioxide by air stripping at low pH. Magnesium is removed by precipitation at high pH. Calcium is removed by ion exchange (IX), and sulfate is removed by nanofiltration (NF). Cation regenerant from IX, containing calcium, and concentrate from NF, containing sulfate, is combined to precipitate gypsum. Concentrate from the desalination process consisting of a concentrated NaCl solution is used to regenerate the IX resins. The selective precipitation, IX, and NF processes were tested in laboratory experiments and produced magnesium hydroxide and gypsum at greater than 90% and 95% purity respectively. A process model was developed to calculate process performance, mass and liquid flow rates. Finally, the MRED process offers the following benefits: 1) greater recovery of brackish feedwater by a desalination process, 2) recovery of marketable commodities and 3) reduction in the volume and mass of waste products from the treatment process.