1993
DOI: 10.1007/bf00617808
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Fullerene superconductivity by short-range order instability

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Cited by 5 publications
(2 citation statements)
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“…Structural phase transition at a higher temperature precedes the charge density wave order occurring at a lower temperature in the SC state. Thus, the structural transition at T ≊ 260 K is followed by a series of steps in ρ(T ) with the one occurring at T ≊ 60 K. HTS in YBCO thin films and fullerenes was previously attributed to percolative conduction between clusters [61]. Metallic cluster-based SC tunneling in Josephsonlinked networks, for which the presence of electronic energy shells is similar to those in atoms and nuclei, is the key ingredient to finding room-T SC [62].…”
Section: Resultsmentioning
confidence: 99%
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“…Structural phase transition at a higher temperature precedes the charge density wave order occurring at a lower temperature in the SC state. Thus, the structural transition at T ≊ 260 K is followed by a series of steps in ρ(T ) with the one occurring at T ≊ 60 K. HTS in YBCO thin films and fullerenes was previously attributed to percolative conduction between clusters [61]. Metallic cluster-based SC tunneling in Josephsonlinked networks, for which the presence of electronic energy shells is similar to those in atoms and nuclei, is the key ingredient to finding room-T SC [62].…”
Section: Resultsmentioning
confidence: 99%
“…Indeed, extrapolating the experimental T c ( M ) plot in Fig. 4 from [61] (M is the cluster mass in atomic units m u ≊ 1. × 10 −27 Kg), we find that a T c ≃ 50 K would correspond to a mass of about 1600m u = 133m C , with m C the mass of a C atom.…”
Section: Resultsmentioning
confidence: 99%