Yasuhiro Takabayashi

Bulk superconductivity at 38 K in a molecular system

\ensuremath{\alpha}\text{-FeSe}

Crystal structure of the new FeSe1−x superconductor

with the PbO structure is a key member of the family of high-

The disorder-free non-BCS superconductor Cs3C60 emerges from an antiferromagnetic insulator parent state.

{T}_{c}

Polymorphism control of superconductivity and magnetism in Cs3C60 close to the Mott transition

iron pnictide and chalcogenide superconductors, as while it possesses the basic layered structural motif of edge-sharing distorted

Crystal structure and phase transitions across the metal-superconductor boundary in the SmFeAsO 1 − x F x ( 0 ≤ x ≤ 0.20 ) family

{\text{FeSe}}_{4}

Electronic structure of Eu@C60 studied by XANES and UV-VIS absorption spectra

tetrahedra, it lacks interleaved ion spacers or charge-reservoir layers. We find that the application of hydrostatic pressure first rapidly increases

Synthesis and physical properties of metal-doped picene solids

{T}_{c}

Cation vacancy order in the K0.8+xFe1.6−ySe2 system: Five-fold cell expansion accommodates 20% tetrahedral vacancies

which attains a broad maximum of 37 K at

Optimized unconventional superconductivity in a molecular Jahn-Teller metal.

\ensuremath{\sim}7\text{ }\text{GPa}