Evolution of Fermi Surface Properties in CexLa1-xB6 and PrxLa1-xB6

  • Endo Motoki
    Graduate School of Science and Center for Low Temperature Science, Tohoku University
  • Nakamura Shintaro
    Institute for Materials Research and Center for Low Temperature Science, Tohoku University
  • Isshiki Toshiyuki
    Graduate School of Science and Center for Low Temperature Science, Tohoku University
  • Kimura Noriaki
    Graduate School of Science and Center for Low Temperature Science, Tohoku University
  • Nojima Tsutomu
    Institute for Materials Research and Center for Low Temperature Science, Tohoku University
  • Aoki Haruyoshi
    Graduate School of Science and Center for Low Temperature Science, Tohoku University
  • Harima Hisatomo
    Department of Physics, Kobe University
  • Kunii Satoru
    Faculty of Engineering, Tohoku Gakuin University

書誌事項

タイトル別名
  • Evolution of Fermi Surface Properties in CexLa1−xB6 and PrxLa1−xB6
  • Evolution of Fermi Surface Properties in Ce<sub><i>x</i></sub>La<sub>1-<i>x</i></sub>B<sub>6</sub> and Pr<sub><i>x</i></sub>La<sub>1-<i>x</i></sub>B<sub>6</sub>

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抄録

We report the de Haas–van Alphen (dHvA) effect measurements of the Fermi surface properties in LaB6, CexLa1−xB6 (x=0.1, 0.25, 0.5, 0.75, 1.0) and PrxLa1−xB6 (x=0.25, 0.5, 0.75, 1.0) with particular attention to the spin dependence of the Fermi surface properties. The Fermi surface shape and dimension of CexLa1−xB6 change considerably with Ce concentration, while those of PrxLa1−xB6 change very slightly up to x=0.75, and in PrB6 the Fermi surface splits into the up and down spin Fermi surfaces. The effective mass of CexLa1−xB6 increases considerably with Ce concentration and is nearly proportional to the number of Ce ions, whereas that of PrxLa1−xB6 increases slightly with Pr concentration. In CexLa1−xB6 the effective mass depends very strongly on field and increases divergently with decreasing field, while that of PrxLa1−xB6 increases slightly with decreasing field. The contribution to the dHvA signal from the conduction electrons of one spin direction diminishes with Ce concentration and appears to disappear somewhere around x=0.25–0.5. A weak spin dependence is also found in PrxLa1−xB6. The behaviors of CexLa1−xB6 and PrxLa1−xB6 are compared to discuss the origin of the spin dependence of the Fermi surface properties.

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