Materials Department and Materials Research Laboratory, University of California, Santa Barbara, CA 93106, USA.
J Phys Condens Matter. 2012 Jan 11;24(1):016002. doi: 10.1088/0953-8984/24/1/016002. Epub 2011 Dec 2.
We have prepared the complete delafossite solid solution series between diamagnetic CuAlO(2) and the t(2g)(3)frustrated antiferromagnet CuCrO(2). The evolution with composition x in CuAl(1-x)Cr(x)O(2) of the crystal structure and magnetic properties has been studied and is reported here. The room-temperature unit cell parameters follow the Végard law and increase with x as expected. The μ(eff) is equal to the Cr(3+) spin-only S = 3/2 value throughout the entire solid solution. Θ(CW) is negative, indicating that the dominant interactions are antiferromagnetic, and its magnitude increases with Cr substitution. For dilute Cr compositions, the nearest-neighbor exchange coupling constant J(BB) was estimated by mean-field theory to be 3.0 meV. Despite the sizable Θ(CW), long-range antiferromagnetic order does not develop until x is almost 1, and is preceded by glassy behavior. The data presented here, and those on dilute Al substitution from Okuda et al, suggest that the reduction in magnetic frustration due to the presence of non-magnetic Al does not have as dominant an effect on magnetism as chemical disorder and dilution of the magnetic exchange. For all samples, the 5 K isothermal magnetization does not saturate in fields up to 5 T and minimal hysteresis is observed. The presence of antiferromagnetic interactions is clearly evident in the sub-Brillouin behavior with a reduced magnetization per Cr atom. An inspection of the scaled Curie plot reveals that significant short-range antiferromagnetic interactions occur in CuCrO(2) above its Néel temperature, consistent with its magnetic frustration. Uncompensated short-range behavior is present in the Al-substituted samples and is likely a result of chemical disorder.
我们已经制备了完全的反铁磁体 CuCrO(2) 和顺磁体 CuAlO(2) 之间的反铁磁体 CuAl(1-x)Cr(x)O(2) 固溶体系列。本文报道了 CuAl(1-x)Cr(x)O(2) 中随组成 x 变化的晶体结构和磁性能的演变。室温下的晶胞参数遵循 Vegard 定律,与预期的 x 增加。μ(eff) 在整个固溶体中等于 Cr(3+) 的自旋单态 S = 3/2 值。Θ(CW) 为负,表明主导相互作用是反铁磁的,其大小随 Cr 取代而增加。对于稀 Cr 组成,用平均场理论估计最近邻交换耦合常数 J(BB) 为 3.0 meV。尽管 Θ(CW) 很大,但直到 x 几乎为 1 时才会出现长程反铁磁序,并且在此之前存在玻璃行为。这里提出的数据,以及 Okuda 等人关于稀 Al 取代的数据,表明由于非磁性 Al 的存在导致磁各向异性的减少对磁性的影响不如化学无序和磁性交换的稀释大。对于所有样品,在高达 5 T 的磁场下,5 K 的等温磁化强度不会饱和,并且观察到最小的磁滞。反铁磁相互作用的存在在每个 Cr 原子的磁矩减少的亚布里渊行为中明显可见。对比例居里图的检查表明,在其奈尔温度以上的 CuCrO(2)中存在显著的短程反铁磁相互作用,这与磁各向异性一致。在 Al 取代的样品中存在未补偿的短程行为,这可能是化学无序的结果。