2012
DOI: 10.1140/epjb/e2012-30897-y
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On clean grain-boundaries involving growth of nonequilibrium crystalline-amorphous superconducting materials addressed by a phenomenological viewpoint

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Cited by 7 publications
(21 citation statements)
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“…For example, in Ref. [34], a fractional anomalous-growth equation employing a Riemann-Liouville derivative has been introduced to describe nucleation-and-growth processes in superconducting materials like weakly viscoelastic cuprate systems where a relationship between the order of the fractional derivative and the fractal dimension of an anomalous random walk process was found. Another example is the use of Weyl derivatives to describe nucleation-and-growth processes in model lipid membranes [35].…”
Section: Discussionmentioning
confidence: 99%
“…For example, in Ref. [34], a fractional anomalous-growth equation employing a Riemann-Liouville derivative has been introduced to describe nucleation-and-growth processes in superconducting materials like weakly viscoelastic cuprate systems where a relationship between the order of the fractional derivative and the fractal dimension of an anomalous random walk process was found. Another example is the use of Weyl derivatives to describe nucleation-and-growth processes in model lipid membranes [35].…”
Section: Discussionmentioning
confidence: 99%
“…In the mentioned multiseeding method, the number of top-seeded layers amplifies the overall effect of squeezing out the undesired molten phase. It has also been utilized in constructing a cuprate's formation model presented by a recent study [8]. The model describes a polycrystalline cuprate's formation within a nucleation-growth phase transition.…”
Section: Introductionmentioning
confidence: 99%
“…As a consequence, it led to a microstructure's growth equation formulated in terms of fractional dynamics (FD) [9,10]. A more closer (than in [8]) look at the dynamics revealed two distinguishable time scales. In what follows, we wish to explore this observation within the context of our method by making use of an address on fractional superconducting domain-growth dynamics, possibly with a Riemann-Liouville integro-differential operator of the order of α [9,11], pointing specifically to α = 1/2, cf.…”
Section: Introductionmentioning
confidence: 99%
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