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Journal Articles

Fermi surface properties of YbCu$$_2$$Si$$_2$$

Matsuda, Tatsuma; Dung, N. D.*; Haga, Yoshinori; Ikeda, Shugo*; Yamamoto, Etsuji; Ishikura, Tatsuro*; Endo, Toyoaki*; Takeuchi, Tetsuya*; Settai, Rikio*; Onuki, Yoshichika

Physica Status Solidi (B), 247(3), p.757 - 759, 2010/03

 Times Cited Count:2 Percentile:12.12(Physics, Condensed Matter)

We succeeded in growing high-quality single crystals of a heavy electron compound YbCu$$_2$$Si$$_2$$. The electronic specific heat coefficient $$gamma$$ is determined to be 150 mJ/K$$^2cdot$$mol, which is consistent with the $$A$$ value of the electrical resistivity from Kadowaki-Woods relation. We succeeded in observing the de Haas-van Alphen (dHvA) oscillations. The dHvA frequencies and large cyclotron effective masses in YbCu$$_2$$Si$$_2$$ are highly different from those in a non-4$$f$$ reference compound YCu$$_2$$Si$$_2$$. From these dHvA results, the heavy electron state of YbCu$$_2$$Si$$_2$$ is characterized by the large contribution of 4$$f$$-electrons to the volume of the Fermi surface and also to the strong enhancement of effective mass caused by the spin fluctuations.

Journal Articles

The de Haas-van Alphen oscillation and fermi surface properties of YCu$$_2$$Si$$_2$$

Nguyen, D.; Matsuda, Tatsuma; Ikeda, Shugo*; Yamamoto, Etsuji; Haga, Yoshinori; Takeda, Yuji*; Endo, Toyoaki*; Doi, Yusuke*; Settai, Rikio*; Harima, Hisatomo*; et al.

Journal of the Physical Society of Japan, 77(9), p.094702_1 - 094702_6, 2008/09

 Times Cited Count:15 Percentile:64.38(Physics, Multidisciplinary)

We have succeeded in growing a high-quality single crystal of a non-4$$f$$ reference compound YCu$$_2$$Si$$_2$$ for a heavy-fermion superconductor CeCu$$_2$$Si$$_2$$, and observed the de Haas-van Alphen (dHvA) oscillation. The detected dHvA branches in YCu$$_2$$Si$$_2$$ indicate that the Fermi surfaces are multiply connected, and the dHvA frequencies are in the range from 9$$times10^6$$ to 2$$times10^8$$ Oe. These dHvA branches are found to be well explained by the results of energy band calculations. The corresponding cyclotron masses are light, ranging from 0.4 to 1.5 $$m_0$$, and are consistent with the electronic specific heat coefficient of 2.2 mJ/K$$^2cdot$$mol.

Journal Articles

Single crystal growth and de Haas-van Alphen effect in Lu$$_2$$Rh$$_3$$Ga$$_9$$ with quasi-two-dimensional electronic state

Nguyen, D.; Matsuda, Tatsuma; Haga, Yoshinori; Ikeda, Shugo*; Yamamoto, Etsuji; Endo, Toyoaki*; Settai, Rikio*; Harima, Hisatomo*; Onuki, Yoshichika

Journal of the Physical Society of Japan, 77(6), p.064708_1 - 064708_6, 2008/06

 Times Cited Count:1 Percentile:11.66(Physics, Multidisciplinary)

We succeeded in growing a single crystal of a layered compound Lu$$_2$$Rh$$_3$$Ga$$_9$$ with an Y$$_2$$Co$$_3$$Ga$$_9$$-type orthorhombic crystal structure by the Ga-flux method. The lattice, positional, and thermal parameters were determined by single-crystal X-ray diffraction measurement. We also measured the electrical resistivity, specific heat, and de Haas-van Alphen (dHvA) effect. The detected dHvA branches were well explained by the results of full potential LAPW energy band calculations. The electronic state was found to be quasi-two-dimensional, indicating nearly cylindrical Fermi surfaces along the [001] direction.

Journal Articles

Split Fermi surface properties of LaTGe$$_3$$ (T:transition metal) and PrCoGe$$_3$$ with the non-centrosymmetric crystal structure

Kawai, Tomoya*; Muranaka, Hiroshi*; Endo, Toyoaki*; Nguyen, D.; Doi, Yusuke*; Ikeda, Shugo*; Matsuda, Tatsuma; Haga, Yoshinori; Harima, Hisatomo*; Settai, Rikio*; et al.

Journal of the Physical Society of Japan, 77(6), p.064717_1 - 064717_15, 2008/06

 Times Cited Count:44 Percentile:83.61(Physics, Multidisciplinary)

Fermi surfaces of the non-centrosymmetric LaTGe$$_3$$ and PrCoGe$$_3$$ have been studied in detail using the de Haas-van Alphen effect. Splitting of the conduction bands due to the spin-orbit interaction was clearly observed. These results are important in understanding the exotic superconductivity realized in non-centrosymmetric structure.

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