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Oral presentation

La-NMR study of Pr$$_{1-x}$$La$$_x$$Pb$$_3$$

Tokunaga, Yo; Suzuki, Hiroyuki*; Sakai, Hironori; Chudo, Hiroyuki; Kambe, Shinsaku; Yasuoka, Hiroshi; Homma, Yoshiya*; Aoki, Dai*; Shiokawa, Yoshinobu*

no journal, , 

no abstracts in English

Oral presentation

Time-dependent DMRG study of spin-charge separation of one-dimensional correlated electron systems

Onishi, Hiroaki; Gonzalez, I.*; Melko, R.*; Dagotto, E.*

no journal, , 

no abstracts in English

Oral presentation

4f band structure and Fermi surfaces of CeIrSi$$_3$$ by soft X-ray angle-resolved resonant photoemission spectroscopy

Okochi, Takuo; Yasui, Akira; Takeda, Yukiharu; Okane, Tetsuo; Saito, Yuji; Fujimori, Atsushi*; Yamagami, Hiroshi; Miyauchi, Yuichiro*; Okuda, Yusuke*; Settai, Rikio*; et al.

no journal, , 

We have investigated the bulk 4$$f$$ electronic structure of the non-centrosymmetric superconductor, CeIrSi$$_3$$ by soft X-ray angle-resolved photoemission spectroscopy. We have performed the angle-resolved 3$$d$$-4$$f$$ resonant photoemission and the comparison of the angle-resolved photoemission spectra of CeIrSi$$_3$$ with those of non-$$f$$ reference compound, LaIrSi$$_3$$ and revealed that the 4$$f$$ states of CeIrSi$$_3$$ well hybridized with the non-$$f$$ conduction bands.

Oral presentation

New material research in the heavy fermion 122 systems

Matsuda, Tatsuma

no journal, , 

no abstracts in English

Oral presentation

Static and dynamic properties of heavy fermion formation in USn$$_3$$

Kambe, Shinsaku; Sakai, Hironori; Tokunaga, Yo; Matsuda, Tatsuma; Haga, Yoshinori; Chudo, Hiroyuki

no journal, , 

Knight shift, T$$_1$$,T$$_{2G}$$, specific heat and susceptibility have been measured in USn$$_3$$ and analyzed in terms of spin-fluctuation model. The heavy fermion state is well described with the model, but T-dependent RKKY interaction is necessary to reproduce the crossover regime. The dynamical scaling law is suggested for the heavy fermion regime in the T$$_{2G}$$ measurements.

Oral presentation

High pressure study on actinide compounds using a diamond anvil cell

Tateiwa, Naoyuki

no journal, , 

We have developed a system based on the diamond anvil cell for high pressure experiments. Noble gas argon is used as a pressure-transmitting medium. We have tested 12 kind of pressure-transmitting media commonly used for the high pressure studies. It is found that the noble gas argon is best one for the study up to 10 GPa. We have measured the electrical resistivity of a uranium antiferromagnet U$$_2$$Zn$$_{17}$$. The pressure dependences of the antiferromagnetic transition temperature and the characteristic temperature of the itinerant electronic state are discussed. It is found that the pressure effect on the physical properties in U$$_2$$Zn$$_{17}$$ is weak compared with the other heavy fermion system.

Oral presentation

Study of the electronic structure of uranium mixed chalcogenides by soft X-ray spectroscopy

Takeda, Yukiharu; Okane, Tetsuo; Okochi, Takuo; Kobayashi, Masaki*; Fujimori, Shinichi; Saito, Yuji; Yamagami, Hiroshi; Fujimori, Atsushi; Ikeda, Shugo*; Sakai, Hironori; et al.

no journal, , 

no abstracts in English

Oral presentation

$$^{27}$$Al NMR studies of NpPd$$_5$$Al$$_2$$

Chudo, Hiroyuki; Sakai, Hironori; Tokunaga, Yo; Kambe, Shinsaku; Aoki, Dai*; Homma, Yoshiya*; Shiokawa, Yoshinobu*; Haga, Yoshinori; Ikeda, Shugo*; Matsuda, Tatsuma; et al.

no journal, , 

no abstracts in English

Oral presentation

Electronic structure of CeCoSi$$_2$$ using first principle band calculation

Yasui, Akira; Yamagami, Hiroshi

no journal, , 

We have obtained the electronic structure of CeCoSi$$_2$$, which is typical compounds in the heavy-fermion system, using a first-principle band calculation with the relativistic linearized-augmented-plane-wave method. I compared calculated results with the band dispersion and the Fermi surface (FS) formation obtained by the Ce 3$$d$$-4$$f$$ resonant angle-resolved photoemission spectra at BL23SU of SPring-8. As the result, the calculated FS formation is good agreement with experimental one. The LDA calculation explains the experimental band dispersion roughly. However there are some problems: especially, the valence band obtained by the experiment shows the energy shift to higher side compared with one by LDA calculation. This problem is due to the strong electronic correlation. Ce 4$$f$$ band which pushes down the valence band shifts to higher energy because of the strong electron-electron interaction.

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