Yoshihiko Inada

Fermi Surface, Magnetic and Superconducting Properties of LaRhIn5 and CeTIn5 (T: Co, Rh and Ir)

We have studied Fermi surface properties of LaRhIn 5 and CeTIn 5 (T: Co, Rh and Ir) via the de Haas–van Alphen (dHvA) experiment. The Fermi surface of a non-4 f reference compound LaRhIn 5 is quasi...

Fermi surface of the heavy-fermion superconductorPrOs4Sb12

We have investigated the de Haas-van Alphen effect in the Pr-based heavy-fermion superconductor PrOs 4 Sb 1 2 . The topology of Fermi surface is close to the reference compound LaOs 4 Sb 1 2 and well explained by the band-structure calculation based on the FLAPW (full potential linearized augmented-plane-wave)-LDA (local-density approximation) +U method, where the 4f electrons are localized. We have confirmed a highly enhanced cyclotron effective mass (2.4-7.6)m 0 , which is apparently large compared to the usual Pr-based compounds.

Exotic heavy-fermion state in the filled skutterudite PrFe4P12 uncovered by the de Haas-van Alphen effect

We report the de Haas--van Alphen (dHvA) experiment on the filled skutterudite

Anomalous peak effect in CeRu2 and 2H-NbSe2: Fracturing of a flux line lattice

{\mathrm{PrFe}}_{4}{\mathrm{P}}_{12}

Superconducting Properties of CeRu2

exhibiting apparent Kondo-like behaviors in the transport and thermal properties. We have found enormously enhanced cyclotron effective mass

de Haas-van Alphen Oscillation in Both Normal and Superconducting Mixed States of CeRu2

{m}_{\mathrm{c}}^{*}=81{m}_{0}

Superconductivity of the ternary boride Li2Pd3B probed by B-11 NMR

in the high field phase, which indicates that

Fermi surface and de Haas-van Alphen oscillation in both the normal and superconducting mixed states of UPd2Al3

{\mathrm{PrFe}}_{4}{\mathrm{P}}_{12}

Cylindrical Fermi surfaces formed by a fiat magnetic Brillouin zone in uranium dipnictides

is the first Pr compound in which really heavy mass has been unambiguously confirmed. Also in the low field nonmagnetic ordered phase (LOP), we observed the dHvA branch with

Crystal growth and cylindrical Fermi surfaces of USb2

{m}_{\mathrm{c}}^{*}=10{m}_{0}