We succeeded in growing a single crystal of Ce2CoIn8 by the flux method. The results of specific heat and electrical resistivity measurements indicate that Ce2CoIn8 is a heavyfermion superconductor below 0.4 K with an electronic specific heat coefficient γ as large as 500 mJ/K 2 mol-Ce.
Relatively good hard magnetic properties obtained from Nd2Fe14B films prepared by the rf sputtering technique were investigated in terms of the microstructural development. Although as-deposited films on Mo substrates deposited at substrate temperatures (Ts) of 365 °C were amorphous with the dispersion of nanocrystalline NdO particles, columnar grains of Nd2Fe14B phase with the c-axis perpendicular to the film plane developed after annealing at 650 °C at an optimized heating rate. Nd2Fe14B grain size was about 400 nm in average and NdO particles of about 10 nm were dispersed within the grains and along the grain boundaries. These films exhibited good perpendicular hard magnetic properties of Hci=1356 kA/m and (BH)MAX∼216 kJ/m3.
We have carried out high-resolution angle-resolved and resonant photoemission spectroscopy ͑RPES͒ on heavy-fermion superconductors Ce 2 CoIn 8 and Ce 2 RhIn 8 to study the electronic band structure and the nature of the Ce 4f electrons. We have experimentally determined the valence-band structure and compared them with the full-potential linear augmented plane-wave band calculations. We found that both compounds have quasitwo-dimensional cylindrical Fermi surfaces centered at the M͑A͒ point in the Brillouin zone, which may be an essential parameter for the development of the superconductivity. Comparison with the band calculations based on the itinerant and localized models suggests that the Ce 4f electrons are essentially localized in both compounds at a measured temperature of 40 K. RPES results have confirmed the localized character of the Ce 4f electrons in both compounds, with a relatively stronger localized nature in Ce 2 RhIn 8 than in Ce 2 CoIn 8 . This difference in the strength of localized character well explains the difference in the magnetic properties between the two compounds.
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