Hidden amorphous phase and reentrant supercooled liquid in Pd-Ni-P metallic glasses
Si Lan, Y. Ren, Xiaoya Wei, B. Wang, Elliot P. Gilbert, Tamaki Shibayama, Seiichi Watanabe, Masato Ohnuma, Xun‐Li Wang
Abstract
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Si Lan, Y. Ren, Xiaoya Wei, B. Wang, Elliot P. Gilbert, Tamaki Shibayama, Seiichi Watanabe, Masato Ohnuma, Xun‐Li Wang
Abstract
Open-access reader
An anomaly in differential scanning calorimetry has been reported in a number of metallic glass materials in which a broad exothermal peak was observed between the glass and crystallization temperatures. The mystery surrounding this calorimetric anomaly is epitomized by four decades long studies of Pd-Ni-P metallic glasses, arguably the best glass-forming alloys. Here we show, using a suite of in situ experimental techniques, that Pd-Ni-P alloys have a hidden amorphous phase in the supercooled liquid region. The anomalous exothermal peak is the consequence of a polyamorphous phase transition between two supercooled liquids, involving a change in the packing of atomic clusters over medium-range length scales as large as 18 Å. With further temperature increase, the alloy reenters the supercooled liquid phase, which forms the room-temperature glass phase on quenching. The outcome of this study raises a possibility to manipulate the structure and hence the stability of metallic glasses through heat treatment.
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An anomaly in differential scanning calorimetry has been reported in a number of metallic glass materials in which a broad exothermal peak was observed between the glass and crystallization temperatures. The mystery surrounding this calorimetric anomaly is epitomized by four decades long studies of Pd-Ni-P metallic glasses, arguably the best glass-forming alloys. Here we show, using a suite of in situ experimental techniques, that Pd-Ni-P alloys have a hidden amorphous phase in the supercooled liquid region. The anomalous exothermal peak is the consequence of a polyamorphous phase transition between two supercooled liquids, involving a change in the packing of atomic clusters over medium-range length scales as large as 18 Å. With further temperature increase, the alloy reenters the supercooled liquid phase, which forms the room-temperature glass phase on quenching. The outcome of this study raises a possibility to manipulate the structure and hence the stability of metallic glasses through heat treatment.
Key concepts: Supercooling, Amorphous metal, Differential scanning calorimetry, Materials science, Quenching (fluorescence), Polyamorphism, Crystallization, Glass transition