The effect of degree of amorphousness on electronic transport behaviors in the Ni–Nb–Zr–H glassy alloys with subnanometer-sized clusters

Superior electric storage in de‐alloyed and anodic oxidized Ti–Ni–Si glassy alloy ribbons

“…4b) between a Φ Cu of 4.53–5.10 eV 25 and Φ nanocrystalline‐TiO2 of 5.23 eV 26. Since a large electric storage could be obtained by the parallel combination network of huge numbers of atomic‐size spaces, further improvements such as supercooling through higher roller speeds 27, hydrogen penetration 28 and a parallel array 8 of TiO 2 nanocavities are required.…”

Electric storage in de-alloyed Si-Al alloy ribbons

“…0.55 nm in size [9]). In this material, hydrogen atoms flow into spaces outside the clusters, enlarging the spaces and resulting in the construction of zigzag tunnels of 0.23 nm average width due to the high-pressure effect of hydrogen during electrolysis [10,11]. However, its discharge experiment put severe constraints on the practical prompt discharging, (a) Present address: Research Institute for Electromagnetic Materials -Sendai 982-0807, Japan; E-mail: fukuhara@cd.wakwak.com because the electric charge behaves as a polarized glutinous liquid that is absorbed between pairs of metallic clusters [12].…”

“…Further precise observation is called for. Since large electric storage could be obtained by the parallel combination network of huge numbers of atomic-size spaces, further improvements are also needed such as supercooling through higher roller speeds [11] and hydrogen penetration [8][9][10][11][12] for construction of surface structures with a higher density of narrow canyons.…”