Matches in SemOpenAlex for { <https://semopenalex.org/work/W3012450323> ?p ?o ?g. }
- W3012450323 abstract "We have deposited In-doped $mathrm{S}{mathrm{b}}_{x}mathrm{T}{mathrm{e}}_{y}$ ($x:y=2:3$, 1:1, 3:1, 4:1) phase-change films, and studied their physics properties like crystallization temperature, activation energy, and optical band gap. On the basis of these parameters, a balance between thermal stability and crystallization speed can be found when In content is 20 at. %. We thus further studied their crystallization kinetics using the flash differential scanning calorimetry and the generalized Mauro-Yue-Ellison-Gupta-Allan viscosity model to investigate the potential fragile-to-strong crossover (FSC) in $mathrm{I}{mathrm{n}}_{20}{(mathrm{S}{mathrm{b}}_{2}mathrm{T}{mathrm{e}}_{3})}_{80}, mathrm{I}{mathrm{n}}_{20}{(mathrm{SbTe})}_{80}, mathrm{I}{mathrm{n}}_{20}{(mathrm{S}{mathrm{b}}_{3}mathrm{Te})}_{80}$, and $mathrm{I}{mathrm{n}}_{20}{(mathrm{S}{mathrm{b}}_{4}mathrm{Te})}_{80}$ supercooled liquids. It was found that, $mathrm{I}{mathrm{n}}_{20}{(mathrm{S}{mathrm{b}}_{3}mathrm{Te})}_{80}$ has a large crossover magnitude ($f$) of 2.4 with a distinct FSC behavior, but its maximum crystal growth rate (${U}_{mathrm{max}}$) of $0.047phantom{rule{0.16em}{0ex}}mathrm{m}phantom{rule{0.16em}{0ex}}{mathrm{s}}^{ensuremath{-}1}$ is too low to satisfy the high-speed phase-change application. The crystal growth rate of $mathrm{I}{mathrm{n}}_{3}mathrm{SbT}{mathrm{e}}_{2}$ ($mathrm{I}{mathrm{n}}_{51}mathrm{S}{mathrm{b}}_{17}mathrm{T}{mathrm{e}}_{32}$) was found to be $0.08phantom{rule{0.16em}{0ex}}mathrm{m}phantom{rule{0.16em}{0ex}}{mathrm{s}}^{ensuremath{-}1}$ without distinct FSC. In contrast, $mathrm{I}{mathrm{n}}_{20}{(mathrm{S}{mathrm{b}}_{4}mathrm{Te})}_{80}$ was demonstrated to have a larger ${U}_{mathrm{max}}$ of $0.425phantom{rule{0.16em}{0ex}}mathrm{m}phantom{rule{0.16em}{0ex}}{mathrm{s}}^{ensuremath{-}1}$ and a distinct FSC behavior with a $f$ value of 2.6, which is larger than that of typical phase-change supercooled liquid $mathrm{A}{mathrm{g}}_{5.5}mathrm{I}{mathrm{n}}_{6.5}mathrm{S}{mathrm{b}}_{59}mathrm{T}{mathrm{e}}_{29}$. The results strongly support that, obvious FSC is unique only in some phase-change supercooled liquids, but not a universal dynamic feature." @default.
- W3012450323 created "2020-03-23" @default.
- W3012450323 creator A5003709598 @default.
- W3012450323 creator A5005942513 @default.
- W3012450323 creator A5013046807 @default.
- W3012450323 creator A5042906130 @default.
- W3012450323 creator A5052441498 @default.
- W3012450323 creator A5054544752 @default.
- W3012450323 creator A5065662171 @default.
- W3012450323 creator A5067193471 @default.
- W3012450323 creator A5080207575 @default.
- W3012450323 date "2020-03-06" @default.
- W3012450323 modified "2023-10-15" @default.
- W3012450323 title "Fragile-to-strong crossover in optimized In-Sb-Te phase-change supercooled liquids" @default.
- W3012450323 cites W1019543541 @default.
- W3012450323 cites W1553703124 @default.
- W3012450323 cites W1928137569 @default.
- W3012450323 cites W1974430936 @default.
- W3012450323 cites W1975504940 @default.
- W3012450323 cites W1976810947 @default.
- W3012450323 cites W1978997020 @default.
- W3012450323 cites W1985517168 @default.
- W3012450323 cites W2006050215 @default.
- W3012450323 cites W2006344878 @default.
- W3012450323 cites W2009469164 @default.
- W3012450323 cites W2014492441 @default.
- W3012450323 cites W2019926449 @default.
- W3012450323 cites W2022950976 @default.
- W3012450323 cites W2026169376 @default.
- W3012450323 cites W2042862454 @default.
- W3012450323 cites W2046560325 @default.
- W3012450323 cites W2049486866 @default.
- W3012450323 cites W2050490913 @default.
- W3012450323 cites W2053806176 @default.
- W3012450323 cites W2060922651 @default.
- W3012450323 cites W2062529529 @default.
- W3012450323 cites W2066581052 @default.
- W3012450323 cites W2079529844 @default.
- W3012450323 cites W2083119852 @default.
- W3012450323 cites W2088062112 @default.
- W3012450323 cites W2088409295 @default.
- W3012450323 cites W2095220850 @default.
- W3012450323 cites W2098732250 @default.
- W3012450323 cites W2164767021 @default.
- W3012450323 cites W2461562275 @default.
- W3012450323 cites W2590108384 @default.
- W3012450323 cites W2604587311 @default.
- W3012450323 cites W2615553631 @default.
- W3012450323 cites W2767027953 @default.
- W3012450323 cites W2767215064 @default.
- W3012450323 cites W2768109640 @default.
- W3012450323 cites W2773490930 @default.
- W3012450323 cites W2890899448 @default.
- W3012450323 cites W2899422453 @default.
- W3012450323 cites W2908745758 @default.
- W3012450323 cites W2952143832 @default.
- W3012450323 cites W3099533788 @default.
- W3012450323 cites W2158111952 @default.
- W3012450323 doi "https://doi.org/10.1103/physrevmaterials.4.033403" @default.
- W3012450323 hasPublicationYear "2020" @default.
- W3012450323 type Work @default.
- W3012450323 sameAs 3012450323 @default.
- W3012450323 citedByCount "6" @default.
- W3012450323 countsByYear W30124503232021 @default.
- W3012450323 countsByYear W30124503232022 @default.
- W3012450323 crossrefType "journal-article" @default.
- W3012450323 hasAuthorship W3012450323A5003709598 @default.
- W3012450323 hasAuthorship W3012450323A5005942513 @default.
- W3012450323 hasAuthorship W3012450323A5013046807 @default.
- W3012450323 hasAuthorship W3012450323A5042906130 @default.
- W3012450323 hasAuthorship W3012450323A5052441498 @default.
- W3012450323 hasAuthorship W3012450323A5054544752 @default.
- W3012450323 hasAuthorship W3012450323A5065662171 @default.
- W3012450323 hasAuthorship W3012450323A5067193471 @default.
- W3012450323 hasAuthorship W3012450323A5080207575 @default.
- W3012450323 hasConcept C112964491 @default.
- W3012450323 hasConcept C121332964 @default.
- W3012450323 hasConcept C185592680 @default.
- W3012450323 hasConcept C186370098 @default.
- W3012450323 hasConcept C192562407 @default.
- W3012450323 hasConcept C199360897 @default.
- W3012450323 hasConcept C203036418 @default.
- W3012450323 hasConcept C26873012 @default.
- W3012450323 hasConcept C2781285689 @default.
- W3012450323 hasConcept C41008148 @default.
- W3012450323 hasConcept C62520636 @default.
- W3012450323 hasConcept C8010536 @default.
- W3012450323 hasConcept C97355855 @default.
- W3012450323 hasConceptScore W3012450323C112964491 @default.
- W3012450323 hasConceptScore W3012450323C121332964 @default.
- W3012450323 hasConceptScore W3012450323C185592680 @default.
- W3012450323 hasConceptScore W3012450323C186370098 @default.
- W3012450323 hasConceptScore W3012450323C192562407 @default.
- W3012450323 hasConceptScore W3012450323C199360897 @default.
- W3012450323 hasConceptScore W3012450323C203036418 @default.
- W3012450323 hasConceptScore W3012450323C26873012 @default.
- W3012450323 hasConceptScore W3012450323C2781285689 @default.
- W3012450323 hasConceptScore W3012450323C41008148 @default.
- W3012450323 hasConceptScore W3012450323C62520636 @default.
- W3012450323 hasConceptScore W3012450323C8010536 @default.