2016
DOI: 10.1016/j.matlet.2015.10.027
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Reversible polyamorphic transitions in Ce65.5Al10Cu22.5Co2 metallic glass

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Cited by 6 publications
(6 citation statements)
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“…The previous research of polyamorphism in MGs reported that the variations of the relative volume indicated that a polyamorphic transition occurred [20][21][22], so we inferred that a polyamorphic transition occurred in Er 55 Al 25 Comparing the relative volume changes during compression and decompression, the results show that the polyamorphic transition in MGs is a reversible process, and reversible transition displays a strong hysteresis. These results are consistent with the previous reports in Ce-MGs [14]. The decompression data points did not re-trace the compression path, which indicated that the deformation of MGs under pressures is not entirely elastic.…”
Section: Methodssupporting
confidence: 92%
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“…The previous research of polyamorphism in MGs reported that the variations of the relative volume indicated that a polyamorphic transition occurred [20][21][22], so we inferred that a polyamorphic transition occurred in Er 55 Al 25 Comparing the relative volume changes during compression and decompression, the results show that the polyamorphic transition in MGs is a reversible process, and reversible transition displays a strong hysteresis. These results are consistent with the previous reports in Ce-MGs [14]. The decompression data points did not re-trace the compression path, which indicated that the deformation of MGs under pressures is not entirely elastic.…”
Section: Methodssupporting
confidence: 92%
“…The x-ray absorption spectroscopy and ab initio molecular dynamics (AIMD) simulations revealed that the polyamorphism in rare Earth element-based MGs (REMGs) was due to the delocalization of 4f electrons induced by pressure [6,13]. Our previous studies indicated that the polyamorphism in REMGs is a reversible phase transition, and strongly related to the rare Earth element concentration [14,15]. Recently, polyamorphic transition has also been reported in Pd 41.5 Ni 41.5 P 17 MGs [16].…”
Section: Introductionmentioning
confidence: 99%
“…During the cooling of the liquid alloy, there is a continuous change in volume and energy (enthalpy), with the derivative changing in the vicinity of T g (the slope of enthalpy is proportional to the specific heat). The glass transition temperature for a cooling rate of 10 11 K s −1 is 725 K [10]. For the obtained glass, the total and partial pair distribution functions (PDFs) g(r) were determined by the equation…”
Section: Local Atomic Structurementioning
confidence: 99%
“…in amorphous ice [8] or amorphous silicon [9], leading to a change in the state of the glass between low-density amorphous and high-density amorphous. Polyamorphic transition has also been observed in MGs, including rare-earth metals like Ce, Yb, etc [10][11][12] due to the delocalisation of 4f electrons [11]. In the case of Ce-Al alloys, depending on the ratio of atom sizes and concentrations of Ce and Al, the result of the polymorphic transition is either a stabilisation of the amorphous phase as in the example of Ce 55 Al 45 alloy or a partial devitrification as in Ce 75 Al 25 alloy [13].…”
Section: Introductionmentioning
confidence: 99%
“…The trivalent lanthanides (La through Lu except Eu and Yb) have been shown to follow a crystal structure sequence with decreasing the atomic number or increasing pressure: hcp → samarium type (Sm-type) → double hexagonal close packed (dhcp) → fcc → distorted fcc (dfcc) [9]. Except for pure rare-earth elements, lanthanide-solvent bulk metallic glasses undergo the low-density state to high-density state trasitions under high pressures [10][11][12][13][14]. This feature invites the questions: if the phase transition of the rare-earth-HEAs obey the route of rear-earth metatls under high pressures?…”
Section: Introductionmentioning
confidence: 99%