TY - JOUR
T1 - Combining muon spin relaxation and DFT simulations of hydrogen trapping in Al6Mn
AU - Shimizu, Kazuyuki
AU - Nishimura, Katsuhiko
AU - Matsuda, Kenji
AU - Akamaru, Satoshi
AU - Nunomura, Norio
AU - Namiki, Takahiro
AU - Tsuchiya, Taiki
AU - Lee, Seungwon
AU - Higemoto, Wataru
AU - Tsuru, Tomohito
AU - Toda, Hiroyuki
N1 - Publisher Copyright:
© 2024
PY - 2024/5/1
Y1 - 2024/5/1
N2 - Hydrogen at the mass ppm level causes hydrogen embrittlement in metallic materials, but experimentally elucidating the hydrogen trapping sites is extremely difficult. We exploit the fact that positive muons can act as light isotopes of hydrogen to study the trapping state of hydrogen in matter. Zero-field muon spin relaxation experiments and density functional theory (DFT) calculations of the hydrogen trapping energy are carried out for Al6Mn. The DFT calculations reveal four possible trapping sites for hydrogen in Al6Mn, at which the hydrogen trapping energies are 0.168 (site 1), 0.312 (site 2), 0.364 (site 3), and 0.495 (site 4) in units of eV/atom. The variations in the deduced dipole field width (Δ) with temperature indicate noticeable changes at 94, 193, and 236 K. Considering the site densities, the observed Δ change temperatures are interpreted as muon trapping at sites 1, 3, and 4.
AB - Hydrogen at the mass ppm level causes hydrogen embrittlement in metallic materials, but experimentally elucidating the hydrogen trapping sites is extremely difficult. We exploit the fact that positive muons can act as light isotopes of hydrogen to study the trapping state of hydrogen in matter. Zero-field muon spin relaxation experiments and density functional theory (DFT) calculations of the hydrogen trapping energy are carried out for Al6Mn. The DFT calculations reveal four possible trapping sites for hydrogen in Al6Mn, at which the hydrogen trapping energies are 0.168 (site 1), 0.312 (site 2), 0.364 (site 3), and 0.495 (site 4) in units of eV/atom. The variations in the deduced dipole field width (Δ) with temperature indicate noticeable changes at 94, 193, and 236 K. Considering the site densities, the observed Δ change temperatures are interpreted as muon trapping at sites 1, 3, and 4.
KW - AlMn
KW - Hydrogen
KW - Hydrogen embrittlement
KW - Muon
KW - Zero-field muon spin relaxation
UR - http://www.scopus.com/inward/record.url?scp=85186119247&partnerID=8YFLogxK
U2 - 10.1016/j.scriptamat.2024.116051
DO - 10.1016/j.scriptamat.2024.116051
M3 - 学術論文
AN - SCOPUS:85186119247
SN - 1359-6462
VL - 245
JO - Scripta Materialia
JF - Scripta Materialia
M1 - 116051
ER -