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arXiv 1303.2801cond-mat.mtrl-scicond-mat.str-el
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CeMo2Si2C的价态涨落

Valence Fluctuation in CeMo2Si2C

U. B. Paramanik, Anupam, U. Burkhard, R. Prasad, C. Geibel, Z. Hossain

摘要:

本文用磁化率$χ(T)$、比热$C(T)$、电阻率$ρ(T)$和X射线吸收谱研究了Ce Mo $_{2}$ Si $_{2}$ C中Ce的价态涨落。粉末X射线衍射表明CeMo $_{2}$ Si $_{2}$ C以CeCr $_{2}$ Si $_{2}$ C型层状四元晶体结构(空间群\textit{P4/mmm})结晶。CeMo $_{2}$ Si $_{2}$ C的晶胞体积偏离预期的镧系收缩,表明该化合物中Ce离子的非三价态。磁化率的温度依赖性很弱,且磁化率值很低,说明Ce离子处于价态涨落状态。CeMo $_{2}$ Si $_{2}$ C $<$ $\widetildeν$ $>$中的正式$L_{III}$ Ce价态由X射线吸收光谱测量确定= 3.11远低于四价Ce化合物CeO中的值$<$ $\widetildeν$ $> \simeq$ 3.4 $_{2}$。比热的温度依赖性没有显示出任何异常下降到1.8 K,这排除了系统中的任何磁有序。从比热数据获得的索末菲系数为$γ$ = 23.4mJ/mol 1,K $^{2}$。电阻率在低于35 K的低温范围内遵循$T{^2}$行为,证实了费米液体行为。因此,Kadowaki Wood比$A/γ^{2}$和Sommerfeld Wilson比$χ(0)/γ$都在费米液体系统预期的范围内。为了得到一些关于电子态的信息,我们在密度泛函理论中计算了能带结构,尽管这种方法不能精确地处理4f电子。穿过费米能级的非$f$电子态主要具有Mo 4d特征.它们提供了与4f态强烈杂化的状态,导致中间价态。

英文摘要:

We report on the valence fluctuation of Ce in CeMo$_{2}$Si$_{2}$C as studied by means of magnetic susceptibility $χ(T)$, specific heat $C(T)$, electrical resistivity $ρ(T)$ and x-ray absorption spectroscopy. Powder x-ray diffraction revealed that CeMo$_{2}$Si$_{2}$C crystallizes in CeCr$_{2}$Si$_{2}$C-type layered tetragonal crystal structure (space group \textit{P4/mmm}). The unit cell volume of CeMo$_{2}$Si$_{2}$C deviates from the expected lanthanide contraction, indicating non-trivalent state of Ce ions in this compound. The observed weak temperature dependence of the magnetic susceptibility and its low value indicate that Ce ions are in valence fluctuating state. The formal $L_{III}$ Ce valence in CeMo$_{2}$Si$_{2}$C $<$$\widetildeν$$>$ = 3.11 as determined from x-ray absorption spectroscopy measurement is well bellow the value $<$$\widetildeν$$> \simeq$ 3.4 in tetravalent Ce compound CeO$_{2}$. The temperature dependence of specific heat does not show any anomaly down to 1.8 K which rules out any magnetic ordering in the system. The Sommerfeld coefficient obtained from the specific heat data is $γ$ = 23.4 mJ/mol\,K$^{2}$. The electrical resistivity follows the $T{^2}$ behavior in the low temperature range below 35 K confirming a Fermi liquid behavior. Accordingly both the Kadowaki Wood ratio $A/γ^{2}$ and the Sommerfeld Wilson ratio $χ(0)/γ$ are in the range expected for Fermi-liquid systems. In order to get some information on the electronic states, we calculated the band structure within the density functional theory, eventhough this approach is not able to treat 4f electrons accurately. The non-$f$ electron states crossing the Fermi level have mostly Mo 4d character. They provide the states with which the 4f sates are strongly hybridized, leading to the intermediate valent state.

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