Anodic aluminum oxide (AAO) membranes have traditionally served as structural supports in osmotic energy systems. Here, blind‐hole AAO membranes are demonstrated as active ion‐selective platforms with tunable nanopore structures. By balancing membrane resistance, ion selectivity, and flux, enhanced performance is achieved, delivering a maximum power ...
Khanh Nhien Vu +6 more
wiley +1 more source
Thermomechanical Treatment-Enabled Short-Circuit Diffusion Enhances Molten-Carbonate Corrosion Resistance of an Alumina-Forming Austenitic Alloy. [PDF]
Jiang H, Yu H, Zheng Y, Zhan F, La P.
europepmc +1 more source
3D finite element analysis of removable partial denture with lingual bar major connector constructed with cobalt chromium, PEEK, PEKK, and BioHPP. [PDF]
Zakaria Hashem Mostafa A +2 more
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Effect of Cold Rolling on the Mechanical Properties and Corrosion Resistance in Hydrofluoric Acid Solution of Inconel 600 Alloy. [PDF]
Dong X +6 more
europepmc +1 more source
Micro- and nano-scale topographical alterations in dental alloys after exposure to artificial saliva: a combined SEM-AFM study. [PDF]
Jusufi Osmani Z +5 more
europepmc +1 more source
Localized Corrosion by Chromium Nitride Precipitation in Low-Temperature Plasma-Nitrided Inconel 718. [PDF]
Uribe Cruz JF +4 more
europepmc +1 more source
Bone Compatibility of Experimental Ti-Ag and Ti-Cu Alloy Dental Implants in a Beagle Dog Model. [PDF]
Ohtsuka Y +5 more
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Fe-Cr-P amorphous alloys were electrodeposited in a trivalent chromium sulfate electrolyte containing glycine as complexing agent. The effects of bath composition and electrodeposition parameters such as current density, bath pH and plating time on the ...
Baosong Li, An Lin, Xu Wu
exaly +1 more source
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Dynamics of commensurate chromium alloys
Physical Review B, 1994The dynamics of commensurate chromium alloys are produced by the fluctuations of a spin-density wave consisting of bound electron-hole pairs. For a commensurate alloy at any temperature, we find a transverse spin-wave (SW) mode with frequency \ensuremath{\omega}=cq and a longitudinal amplitude mode with dispersion \ensuremath{\omega}=2\ensuremath{\surd}
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