TY - JOUR
T1 - Glass-liquid transition in a less-stable metallic glass
AU - Ichitsubo, Tetsu
AU - Matsubara, Eiichiro
AU - Numakura, Hiroshi
AU - Tanaka, Katsushi
AU - Nishiyama, Nobuyuki
AU - Tarumi, Ryuichi
N1 - Copyright:
Copyright 2008 Elsevier B.V., All rights reserved.
PY - 2005/8/1
Y1 - 2005/8/1
N2 - A stable metallic glass, SMG, is often viewed as an amorphous alloy exhibiting a reversible glass ↔ liquid transition. Here we show experimentally that even in a less-stable metallic glass, LMG, which is prepared only by rapid melt quenching and promptly crystallized without glass transition at the ordinary heating rate, sufficiently rapid heating exposes the glass→liquid transition by suppressing crystallization. The experimental glass transition Tg and crystallization Tx temperatures were plotted as a function of heating rate β, for Pd42.5 Ni7.5 Cu30 P20 of SMG and for Zr70 Ni30 of LMG. Two extrapolated curves, Tg -log β and Tx -log β, intersect at a quite small β, e.g., ∼ 10-4°C/min, for SMG, whereas their intersection occurs at a large β, e.g., ∼10°C/min, for LMG. Such a large β that is comparable to conventional heating rates makes it difficult to observe the reversible glass transition in LMG, and reflects low thermal stability of the glassy state.
AB - A stable metallic glass, SMG, is often viewed as an amorphous alloy exhibiting a reversible glass ↔ liquid transition. Here we show experimentally that even in a less-stable metallic glass, LMG, which is prepared only by rapid melt quenching and promptly crystallized without glass transition at the ordinary heating rate, sufficiently rapid heating exposes the glass→liquid transition by suppressing crystallization. The experimental glass transition Tg and crystallization Tx temperatures were plotted as a function of heating rate β, for Pd42.5 Ni7.5 Cu30 P20 of SMG and for Zr70 Ni30 of LMG. Two extrapolated curves, Tg -log β and Tx -log β, intersect at a quite small β, e.g., ∼ 10-4°C/min, for SMG, whereas their intersection occurs at a large β, e.g., ∼10°C/min, for LMG. Such a large β that is comparable to conventional heating rates makes it difficult to observe the reversible glass transition in LMG, and reflects low thermal stability of the glassy state.
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U2 - 10.1103/PhysRevB.72.052201
DO - 10.1103/PhysRevB.72.052201
M3 - Article
AN - SCOPUS:33644948148
SN - 0163-1829
VL - 72
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 5
M1 - 052201
ER -