Peter Jeglič

TL;DR: In Cs3C60, where the molecular valences are precisely assigned, the superconducting state at 38 kelvin emerges directly from a localized electron antiferromagnetic insulating state with the application of pressure, with a dependence of the transition temperature on pressure-induced changes of anion packing density that is not explicable by Bardeen-Cooper-Schrieffer (BCS) theory.

TL;DR: The existence of two superconductor packings of the same electronically active unit reveals that Tc scales universally in a structure-independent dome-like relationship with proximity to the Mott metal–insulator transition, which is governed by the role of electron correlations characteristic of high-temperature superconducting materials other than fullerides.

TL;DR: The Jahn-Teller metal is identified as a fluctuating microscopically heterogeneous coexistence of both localized and itinerant electrons that connects the insulating and superconducting states of fullerides.

TL;DR: In this paper, the magnetic susceptibility, the electrical resistivity, the specific heat, the thermoelectric power, the Hall coefficient, and the thermal conductivity of the monoclinic approximants to the decagonal quasicrystal were investigated.

TL;DR: In this article, anisotropic physical properties (magnetic susceptibility, electrical resistivity, thermoelectric power, Hall coefficient, and thermal conductivity) of the orthorhombic approximant to the decagonal phase were investigated.