TY - GEN
T1 - Strain glass
T2 - Glassy martensite
AU - Wang, Y.
AU - Ren, X.
AU - Otsuka, K.
PY - 2008
Y1 - 2008
N2 - "Glass", a frozen disordered-state, has been found in areas as diverse as amorphous solids, magnetic alloys, ferroelectrics, superconductors, and even in models of biological evolutions. In the present review we introduce a new class of glass-the "strain-glass", which was discovered very recently. Strain glass is derived from a martensitic system, where the local-strain is frozen in disordered configuration. The first example of strain glass was found in the well-studied Ni-rich Ti50-xNi50-x martensitic system in its "non-transforming" composition regime (x>1.5). Contrasting to the familiar martensitic transition, the strain glass transition is not accompanied by a change in the average structure, or a thermal peak in the DSC measurement. It involves a dynamic freezing process with broken ergodicity, during which nano-sized martensite domains are frozen. More interestingly, the seemingly "non-martensitic" strain glass exhibits unexpected properties: shape memory effect and superelasticity, like a normal martensitic alloy. Strain glass bears a striking similarity with other two classes of glasses: cluster-spin glass and ferroelectric relaxor. These ferroic-transition-derived glasses can be considered as a more general class of glass: ferroic glass. The finding of strain glass may provide new opportunities for martensite research from both fundamental side and application side.
AB - "Glass", a frozen disordered-state, has been found in areas as diverse as amorphous solids, magnetic alloys, ferroelectrics, superconductors, and even in models of biological evolutions. In the present review we introduce a new class of glass-the "strain-glass", which was discovered very recently. Strain glass is derived from a martensitic system, where the local-strain is frozen in disordered configuration. The first example of strain glass was found in the well-studied Ni-rich Ti50-xNi50-x martensitic system in its "non-transforming" composition regime (x>1.5). Contrasting to the familiar martensitic transition, the strain glass transition is not accompanied by a change in the average structure, or a thermal peak in the DSC measurement. It involves a dynamic freezing process with broken ergodicity, during which nano-sized martensite domains are frozen. More interestingly, the seemingly "non-martensitic" strain glass exhibits unexpected properties: shape memory effect and superelasticity, like a normal martensitic alloy. Strain glass bears a striking similarity with other two classes of glasses: cluster-spin glass and ferroelectric relaxor. These ferroic-transition-derived glasses can be considered as a more general class of glass: ferroic glass. The finding of strain glass may provide new opportunities for martensite research from both fundamental side and application side.
KW - Ferroic glass
KW - Martensitic transition
KW - Point defects
KW - Shape memory effect
KW - Strain glass transition
KW - Ti-Ni
UR - https://www.scopus.com/pages/publications/56349138724
U2 - 10.4028/www.scientific.net/msf.583.67
DO - 10.4028/www.scientific.net/msf.583.67
M3 - 会议稿件
AN - SCOPUS:56349138724
T3 - Materials Science Forum
SP - 67
EP - 84
BT - Materials Science Forum - Advances in Shape Memory Materials
PB - Trans Tech Publications Ltd
ER -