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Magnetic field and pressure phase diagrams of uranium heavy-fermion compound U$$_2$$Zn$$_{17}$$

重い電子系ウラン化合物U$$_2$$Zn$$_{17}$$の磁場/圧力相図

立岩 尚之  ; 池田 修悟*; 芳賀 芳範 ; 松田 達磨; 山本 悦嗣 ; 杉山 清寛*; 萩原 政幸*; 金道 浩一*; 大貫 惇睦*

Tateiwa, Naoyuki; Ikeda, Shugo*; Haga, Yoshinori; Matsuda, Tatsuma; Yamamoto, Etsuji; Sugiyama, Kiyohiro*; Hagiwara, Masayuki*; Kindo, Koichi*; Onuki, Yoshichika*

重い電子系化合物U$$_2$$Zn$$_{17}$$について53Tまでの磁化測定を行った。ネール温度$$T_{rm N}$$=9.7K以下の反強磁性状態で、32Tの強磁場中でメタ磁性転移が観測され、磁気相図が作成された。われわれは、U$$_2$$Zn$$_{17}$$の反強磁性転移の圧力効果をダイヤモンドアンビルセルを用いて行った。反強磁性転移温度は、4.7GPaまで圧力に強く依存せず、5GPa以上で加圧とともに増大する。電気抵抗の温度依存について理論解析の結果得られた、$$T^2$$項の係数$$A$$,反強磁性ギャップ$$Delta$$の圧力依存について議論する。

We have performed the magnetization measurements in high magnetic fields up to 53 T on single crystals of an uranium heavy fermion compound U$$_2$$Zn$$_{17}$$. In the antiferromagnetic state below the N$'e$el temperature $$T_{rm N}$$ = 9.7 K, a metamagnetic transition is found at $$H_c$$ $$simeq$$ 32 T for the field along the [11$$bar{2}$$0] direction ($$a$$-axis). The magnetic phase diagram for the field along the [11$$bar{2}$$0] direction is given. We have also carried out high pressure resistivity measurement on U$$_2$$Zn$$_{17}$$ using a diamond anvil cell up to 8.7 GPa. The N$'e$el temperature $$T_{rm N}$$ is almost pressure-independent up to 4.7 GPa and starts to increase at the higher pressure region. The pressure dependences of the coefficient of $$T^2$$ term in the electrical resistivity $$A$$, an antiferromagnetic gap $$Delta$$ and a characteristic temperature $$T_{{rho}{rm max}}$$ are discussed.

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パーセンタイル:53.36

分野:Physics, Multidisciplinary

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