Max-Planck Institute for Chemical Physics of Solids, D-01187 Dresden, Germany.
J Phys Condens Matter. 2012 Apr 4;24(13):135602. doi: 10.1088/0953-8984/24/13/135602. Epub 2012 Mar 9.
A detailed (31)P (I = 1/2) and (75)As (I = 3/2) NMR study on polycrystalline CeFeAs(1-x)P(x)O alloys is presented. The magnetism of CeFeAsO changes drastically upon P substitution on the As site. CeFePO is a heavy fermion system without long-range order whereas CeFeAsO exhibits an Fe 3d SDW type of ordering accompanied by a structural transition from tetragonal (TT) to orthorhombic (OT) structure. Furthermore, Ce 4f(1) orders antiferromagnetically (AFM) at low temperature. At the critical concentration where the Fe magnetism is diminished the Ce-Ce interaction changes to a ferromagnetic (FM) type of ordering. Three representative samples of the CeFeAs(1-x)P(x)O (x = 0.05, 0.3 and 0.9) series are systematically investigated. (1) For the x = 0.05 alloy a drastic change of the linewidth at 130 K indicates the AFM-SDW type of ordering of Fe and the structural change from the TT to the OT phase. The linewidth roughly measures the internal field in the ordered state and the transition is most likely first order. The small and nearly constant shift from (31)P and (75)As NMR suggests the presence of competing hyperfine interactions between the nuclear spins and the 4f and 3d ions of Ce and Fe. (2) For the x = 0.3 alloy, the evolution of the Fe-SDW type of order takes place at around 70 K corroborating the results of bulk measurement and μSR. Here we found evidence for phase separation of paramagnetic and magnetic SDW phases. (3) In contrast to the heavy fermion CeFePO for the x = 0.9 alloy a phase transition is found at 2 K. The field-dependent NMR shift gives evidence of FM ordering. Above the ordering the spin-lattice relaxation rate (31)(1/T(1)) shows unconventional, non-Korringa-like behaviour which indicates a complex interplay of Kondo and FM fluctuations.
本文对多晶 CeFeAs(1-x)P(x)O 合金进行了详细的 (31)P(I=1/2)和 (75)As(I=3/2)NMR 研究。CeFeAsO 的磁性在 As 位被 P 取代后发生了剧烈变化。CeFePO 是一个没有长程有序的重费米子体系,而 CeFeAsO 则表现出 Fe 3d SDW 型有序,同时伴随着从四方(TT)到正交(OT)结构的转变。此外,Ce 4f(1)在低温下反铁磁(AFM)有序。在铁磁有序消失的临界浓度处,Ce-Ce 相互作用转变为铁磁(FM)有序。本文系统研究了 CeFeAs(1-x)P(x)O(x=0.05、0.3 和 0.9)系列的三个代表性样品。(1)对于 x=0.05 的合金,在 130 K 时线宽的急剧变化表明 Fe 的 AFM-SDW 型有序和从 TT 到 OT 相的结构变化。线宽大致衡量了有序态中的内场,而且转变很可能是一级相变。(31)P 和 (75)As NMR 的微小且几乎恒定的位移表明,核自旋与 Ce 和 Fe 的 4f 和 3d 离子之间存在竞争的超精细相互作用。(2)对于 x=0.3 的合金,Fe-SDW 型有序的演化发生在 70 K 左右,这与体测量和 μSR 的结果一致。在这里,我们发现了顺磁和磁性 SDW 相分离的证据。(3)与重费米子 CeFePO 不同,对于 x=0.9 的合金,在 2 K 时发现了一个相变。场依赖的 NMR 位移证明了 FM 有序。在有序相上方,自旋晶格弛豫率 (31)(1/T(1))表现出非传统的、非 Korringa 行为,这表明 Kondo 和 FM 涨落之间存在复杂的相互作用。