TY - JOUR
T1 - High-energy-resolution photoemission study of and
AU - Kumigashira, H.
AU - Chainani, A.
AU - Yokoya, T.
AU - Akaki, O.
AU - Takahashi, T.
AU - Ito, M.
AU - Kasaya, M.
AU - Sakai, O.
N1 - Copyright:
Copyright 2017 Elsevier B.V., All rights reserved.
PY - 1996
Y1 - 1996
N2 - We studied the electronic structure of isostructural (Formula presented) and (Formula presented) using high-resolution low-temperature photoemission spectroscopy. (Formula presented) is a typical valence fluctuation material, while (Formula presented) is a low (Formula presented)(∼10 K) heavy-fermion system. The valence-band spectra show that Ni 3d derived states appear at energies closer to the Fermi level ((Formula presented)) compared to the Pt 5d derived states. The near-(Formula presented) spectra exhibit the characteristic spin-orbit splitting of 4f states (4(Formula presented) and 4(Formula presented)), with higher 4(Formula presented) intensity in (Formula presented) than in (Formula presented). Numerical simulations based on the single-impurity Anderson model show that the hybridization between the conduction band and f electrons is stronger in (Formula presented) than in (Formula presented). This is qualitatively understood in terms of proximity of Ni 3d states to the f level. The obtained spectroscopic results were discussed in comparison with transport and magnetic measurements.
AB - We studied the electronic structure of isostructural (Formula presented) and (Formula presented) using high-resolution low-temperature photoemission spectroscopy. (Formula presented) is a typical valence fluctuation material, while (Formula presented) is a low (Formula presented)(∼10 K) heavy-fermion system. The valence-band spectra show that Ni 3d derived states appear at energies closer to the Fermi level ((Formula presented)) compared to the Pt 5d derived states. The near-(Formula presented) spectra exhibit the characteristic spin-orbit splitting of 4f states (4(Formula presented) and 4(Formula presented)), with higher 4(Formula presented) intensity in (Formula presented) than in (Formula presented). Numerical simulations based on the single-impurity Anderson model show that the hybridization between the conduction band and f electrons is stronger in (Formula presented) than in (Formula presented). This is qualitatively understood in terms of proximity of Ni 3d states to the f level. The obtained spectroscopic results were discussed in comparison with transport and magnetic measurements.
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U2 - 10.1103/PhysRevB.53.2565
DO - 10.1103/PhysRevB.53.2565
M3 - Article
AN - SCOPUS:0039942217
SN - 1098-0121
VL - 53
SP - 2565
EP - 2568
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 5
ER -