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Journal Articles

An Examination of the estimation method for the specific heat of TRU dioxide; Evaluation with PuO$$_{2}$$

Serizawa, Hiroyuki; Arai, Yasuo

Journal of Alloys and Compounds, 312(1-2), p.257 - 264, 2001/00

 Times Cited Count:12 Percentile:58.26(Chemistry, Physical)

no abstracts in English

Oral presentation

5$$f$$-electron states in NpPd$$_5$$Al$$_2$$ and the origin of the heavy fermion state

Metoki, Naoto; Aoki, Dai*; Griveau, J.-C.*; Otsuki, Junya*

no journal, , 

Non-Krammers trivalent Np$$^{3+}$$(5$$f^4$$) ion in the heavy fermion superconductor NpPd$$_5$$Al$$_2$$ shows $$J$$=4, similar to Pr$$^{3+}$$. We determined the singlet ground state of $$Gamma_1$$ and the first excited doublet of $$Gamma_5$$ above 49 K from the quantitative analysis of the magnetic susceptibility and the magnetization curve. The $$Gamma_5$$ must contribute to the heavy fermion, since the singlet ground state $$Gamma_1$$ alone cannot, where 2-channel Kondo effect appears based on $$Gamma_5$$. The low-temperature specific heat of NpPd$$_5$$Al$$_2$$ can be explained with the superposition of the heavy fermion state and localized Schottky anomaly, where the total entropy was maintained $$R$$ln3 for pseudo-triplet state. The $$LS$$-coupling scheme of AnPd$$_5$$Al$$_2$$ can be described by the corresponding $$j$$-$$j$$ coupling scheme, where Pu and Np are the hole version of Ce and Pr. The $$Gamma_1$$ in NpPd$$_5$$Al$$_2$$ is stabilized with the same mechanism as in PrT$$_2$$X$$_{20}$$, both exhibit the unconventional superconductivity.

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