2021
DOI: 10.1016/j.mtla.2021.101199
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High pressure phase evolution under hydrostatic pressure in a single imperfect crystal due to nanovoids

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Cited by 25 publications
(7 citation statements)
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“…At corner E (zone 1, opposite to the AB edges) in figure 7 An intriguing feature of HRTEM images studied here is the topological layer S 1 at h-plates S 2 (seeds) turns down at borders so to cross-link S 1 − S 2 at a self-confined (compressed) structure. It involves a type of a 'S 1 →S 2 transition' over twins mediated via a Bi-rich MnBi 4 type phase (as observed at the lattice and XRD patterns) as an intermediate melt (MI) at the anneals, as noticed at some metals/alloys and PbTiO 3 at a solid S 1 →a solid S 2 phase transition [42][43][44]. In the theoretical studies, the Ginzburge-Landau equations are applied for various nanovoid deformation behaviors of materials and different nanoscale phenomena that can propagate at 'through channels' via a partially or a fully recurring melt phase [43,44].…”
Section: Hrtem Images Of Mn 60 Bi 40 Small H-platesmentioning
confidence: 98%
“…At corner E (zone 1, opposite to the AB edges) in figure 7 An intriguing feature of HRTEM images studied here is the topological layer S 1 at h-plates S 2 (seeds) turns down at borders so to cross-link S 1 − S 2 at a self-confined (compressed) structure. It involves a type of a 'S 1 →S 2 transition' over twins mediated via a Bi-rich MnBi 4 type phase (as observed at the lattice and XRD patterns) as an intermediate melt (MI) at the anneals, as noticed at some metals/alloys and PbTiO 3 at a solid S 1 →a solid S 2 phase transition [42][43][44]. In the theoretical studies, the Ginzburge-Landau equations are applied for various nanovoid deformation behaviors of materials and different nanoscale phenomena that can propagate at 'through channels' via a partially or a fully recurring melt phase [43,44].…”
Section: Hrtem Images Of Mn 60 Bi 40 Small H-platesmentioning
confidence: 98%
“…Fu et al [ 30 ] suggested that the “strain rate effect” is a combination effect produced by the action of crack propagation, the inertial effect, and the viscous effect of free water. The DIF may not be a material property, but a physical result generated by inertial restraint, microcrack propagation, specimen size, free water and other factors with the increase in the strain rate [ 31 , 32 , 33 , 34 ].…”
Section: Test Results and Discussionmentioning
confidence: 99%
“…Moreover, a given fullerene at different sized OLF n shows different T m , indicating that the structural stability of SWF n can be effectively influenced by nanoconfinement. Such melting point profile can be utilized in a more general case, for example, temperature-induced phase transformation or stress-induced nanovoid formation/phase transformation in other structures [66][67][68]. Moreover, from an experimental point of view, novel carbon nanostructures of amorphous carbon@fullerene can be obtained by heating OLF n at critical temperatures.…”
Section: Melting Temperatures Of Swfn and Olfnmentioning
confidence: 99%