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arXiv 2602.09753cond-mat.str-el
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在铀-铪氢化物中稳定α-UH₃:结构、磁性、热力学和输运性质

Stabilization of $α$-UH$_3$ in U-Hf Hydrides: Structural, Magnetic, Thermodynamic, and Transport Properties

Charles University, Prague, Czech Republic(查理大学);Institute of Physics (FZU), Czech Academy of Sciences, Prague, Czech Republic(捷克科学院物理研究所)

Shanmukh Veera Venkata Uday Kumar Devanaboina, Oleksandra Koloskova, Silvie Maskova-Cerna, Ladislav Havela

AI总结:

通过铪掺杂稳定α-UH₃相,研究其磁性、热力学和输运性质,发现居里温度分布和电阻特性随铪含量变化。

摘要:

铪的掺杂稳定了铀氢化物中不稳定的体心立方(bcc)α-UH₃相,使能够系统地测量其磁性、热力学和输运性质。(UH₃)₁₋ₓHfₓ氢化物(x=0.10, 0.15, 0.30, 0.40)通过氢化铀-铪前驱合金获得。粉末X射线衍射显示,随着x的增加,β-UH₃相逐渐被抑制,当x=0.30时α-UH₃占主导地位,当x=0.40时β-UH₃几乎完全被抑制。磁化测量显示所有组成均表现出铁磁行为,居里温度范围在T_C≈178-185 K之间,最大值出现在x=0.15附近;然而,自发磁化强度随铪含量显著降低,从纯β-UH₃中的1.0μB/U降至(UH₃)₀.₆₀Hf₀.₄₀中的0.46μB/U。比热数据表明,在α-UH₃丰富的氢化物样品中,居里异常显著变宽,这与铁磁非均匀性导致的T_C值分布一致。比热还显示随着铪浓度增加,Sommerfeld系数单调减小,反映了费米能级处电子态密度的减少,尤其是在(UH₃)₀.₆₀Hf₀.₄₀中。 (UH₃)₀.₆₀Hf₀.₄₀的电阻率非常大,表现出2-300 K范围内的稳健负温度系数,并且仅显示出弱磁电阻,表明输运处于强无序主导的非相干 regime。

英文摘要:

Hf substitution stabilizes the metastable body-centered cubic (bcc) $α$-UH$3$ phase in uranium hydrides, enabling systematic measurements of its magnetic, thermodynamic, and transport properties. (UH$3$)${1-x}$Hf$x$ hydrides ($x = 0.10, 0.15, 0.30, 0.40$) were obtained by hydrogenation of U${1-x}$Hf$x$ precursor alloys. Powder X-ray diffraction shows a progressive suppression of $β$-UH$3$ phase with increasing $x$, with $α$-UH$3$ domination at $x = 0.30$ and $β$-UH$3$ nearly fully suppressed at $x = 0.40$. Magnetization measurements show ferromagnetic behavior for all compositions with Curie temperatures in the range $T\mathrm{C} \approx 178$--$185$ K and a maximum near $x = 0.15$; however, the spontaneous magnetization is strongly reduced with Hf content, decreasing from $1.0,μ\mathrm{B}$/U in pure $β$-UH$3$ to $0.46,μ\mathrm{B}$/U for (UH$3$)${0.60}$Hf${0.40}$. Specific-heat data show a broadened Curie anomaly in the $α$-UH$3$ rich hydride samples, consistent with a distribution of $T\mathrm{C}$ values arising from ferromagnetic inhomogeneities. Specific heat also reveals a monotonic decrease in the Sommerfeld coefficient with increasing Hf concentration, reflecting a reduction in the electronic density of states at the Fermi level, especially in (UH$3$)${0.60}$Hf${0.40}$. The resistivity of (UH$3$)${0.60}$Hf${0.40}$ is very large, exhibits a robust negative temperature coefficient over 2--300 K, and shows only weak magnetoresistance, placing transport in a strongly incoherent, disorder-dominated regime.

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