In heavy-fermion compounds, f electrons show both itinerant and localized behaviour depending on the temperature. Above a characteristic temperature, T*, their magnetic properties can be described by completely localized f-electron models. On the other hand, well below T*, their Fermi surfaces can be explained by the itinerant f-electron model. These two models assume totally different natures of the f electrons, and how they transform between these states as a function of temperature has never been understood at the level of their electronic structures. Here, we use angle-resolved photoelectron spectroscopy to study the band structure of the heavy-fermion antiferromagnetic superconductor UPd"2Al"3 below and above T*, and find that the f bands, which form the Fermi surfaces at low temperatures, are excluded from the Fermi surfaces at high temperatures. This result demonstrates how the same f electrons can be both itinerant and localized. © 2007 Nature Publishing Group.
CITATION STYLE
Fujimori, S. I., Saitoh, Y., Okane, T., Fujimori, A., Yamagami, H., Haga, Y., … Onuki, Y. (2007). Itinerant to localized transition of f electrons in the antiferromagnetic superconductor UPd 2 Al 3. Nature Physics, 3(9), 618–622. https://doi.org/10.1038/nphys651
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