J. Phys. Soc. Jpn. 74 (2005) pp. 1930-1933 |Next Article| |Table of Contents|
|Full Text PDF (159K)| |Buy This Article|
Letters
Role of p– f Hybridization in the Metal–Nonmetal Transition of PrRu4P12
Kazuaki Iwasa,
Lijie Hao,
Tomoo Hasegawa,
Toshiaki Takagi,
Kenji Horiuchi,
Yoshiaki Mori,
Youichi Murakami,
Keitaro Kuwahara1,
Masahumi Kohgi1,
Hitoshi Sugawara2,
Shanta Ranjan Saha3,
Yuji Aoki1 and
Hideyuki Sato1
Department of Physics, Tohoku University, Sendai 980-8578
1Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397
2Department of Mathematical and Natural Sciences, The University of Tokushima, Tokushima 770-8502
3Muon Science Laboratory, Institute of Material Structure Science, High Energy Accelerator Research Organization, Tsukuba, Ibaraki 305-0801
(Received April 27, 2005; Accepted May 2, 2005)
Electronic state evolution in the metal–nonmetal transition of PrRu4P12 has been studied by X-ray and polarized neutron diffraction experiments. It has been revealed that, in the low-temperature nonmetallic phase, two inequivalent crystal-field (CF) schemes of Pr3+ 4 f2 electrons with Γ1 and Γ4(2) ground states are located at Pr1 and Pr2 sites forming the bcc unit cell surrounded by the smaller and larger cubic Ru-ion sublattices, respectively. This modulated electronic state can be explained by the p– f hybridization mechanism taking two intermediate states of 4 f1 and 4 f3. The p– f hybridization effect plays an important role in the electronic energy gain in the metal–nonmetal transition originated from the Fermi surface nesting.
©2005 The Physical Society of Japan
KEYWORDS:
metal–nonmetal transition, Fermi surface nesting, crystal-field state, p– f hybridization
URL:
http://jpsj.ipap.jp/link?JPSJ/74/1930/
DOI: 10.1143/JPSJ.74.1930
- Y. Aoki, H. Sugawara, H. Harima and H. Sato:
J. Phys. Soc. Jpn. 74 (2005) 209[IPAP].
- H. Harima and K. Takegahara:
J. Phys.: Condens. Matter 15 (2003) S2081[IoP STACKS].
- C. Sekine, T. Uchiumi, I. Shirotani and T. Yagi:
Phys. Rev. Lett. 79 (1997) 3218[APS].
- C. H. Lee, H. Matsuhata, A. Yamamoto, T. Ohta, H. Takazawa, K. Ueno, C. Sekine, I. Shirotani and T. Hirayama:
J. Phys.: Condens. Matter 13 (2001) L45[IoP STACKS].
- H. Harima and K. Takegahara:
Physica B 312–313 (2002) 843[CrossRef].
- S. R. Saha, H. Sugawara, T. Namiki, Y. Aoki and H. Sato:
J. Phys.: Condens. Matter 15 (2003) S2163[IoP STACKS].
- S. R. Saha, H. Sugawara, Y. Aoki, H. Sato, Y. Inada, H. Shishido, R. Settai, Y. Ōnuki and H. Harima:
Phys. Rev. B. 71 (2005) 132502[APS].
- K. Iwasa, L. Hao, K. Kuwahara, M. Kohgi, S. R. Saha, H. Sugawara, Y. Aoki and H. Sato:
Physica B 359–361 (2005) 833[CrossRef].
- K. Iwasa, L. Hao, K. Kuwahara, M. Kohgi, S. R. Saha, H. Sugawara, Y. Aoki, H. Sato, T. Tayama and T. Sakakibara: to be published in Phys. Rev. B 71 (2005).
- J. Otsuki, H. Kusunose and Y. Kuramoto:
J. Phys. Soc. Jpn. 74 (2005) 200[IPAP].
- L. Hao, K. Iwasa, K. Kuwahara, M. Kohgi, S. R. Saha, H. Sugawara, Y. Aoki, H. Sato, C. Sekine, C. H. Lee and H. Harima:
J. Magn. Magn. Mater. 272–276 (2004) e271[CrossRef].
- S. H. Curnoe, H. Harima, K. Takegahara and K. Ueda:
Physica B 312–313 (2002) 837[CrossRef].
- S. H. Curnoe, K. Ueda, H. Harima and K. Takegahara:
J. Phys. Chem. Solids 63 (2002) 1207[CrossRef].
- H. Harima, K. Takegahara, K. Ueda and S. H. Curnoe: Acta Phys. Pol. B 34 (2003) 1189.
- C. H. Lee, H. Matsuhata, H. Yamaguchi, C. Sekine and I. Shirotani:
J. Magn. Magn. Mater. 272–276 (2004) 426[CrossRef].
- E. J. Lisher and J. B. Forsyth: Acta. Crystallogr., Sect. A 27 (1971) 545.
- C. Sekine, T. Inaba, I. Shirotani, M. Yokoyama, H. Amitsuka and T. Sakakibara:
Physica B 281–282 (2000) 303[CrossRef].
- The discrepancy between the calculation and the experimental results comes from the poorer accuracy of |µa- µb| due to the low number of measured antiferromagnetic reflections compared to the ferromagnetic ones giving the averaged moment value. In addition, the used magnetic form factor may not be appropriate for the strongly hybridized 4 f electrons.
- Since the ratios of resistivity at the lowest temperature to that at TM–I in refs. [Sekine97] and [Saha_R_03] are different from each other, the resistivity is considered to depend on the sample quality. Concerning the carrier mobility as well as carrier density, the strongly temperature-dependent Hall coefficient
[S. R. Saha et al.: J. Magn. Magn. Mater. 272–276 (2004) e317[Elsevier]] is a key phenomenon.
- H. Takahashi and T. Kasuya:
J. Phys. C 18 (1985) 2697[IoP STACKS].