Department of Physics, Indian Institute of Technology Bombay, Mumbai 400076, India.
J Phys Condens Matter. 2010 Jan 27;22(3):035601. doi: 10.1088/0953-8984/22/3/035601. Epub 2009 Dec 21.
We report preparation, x-ray diffraction, magnetic susceptibility χ(T) and heat capacity C(p)(T) measurements on undoped samples as well as samples with Zn-doped (S = 0) at the Cu site BiCu(2(1-x))Zn(2x)PO(6), Ni-doped (S = 1) at the Cu site BiCu(2(1-y))Ni(2y)PO(6), and Ca doped (holes) at the Bi site Bi(1-z)Ca(z)Cu(2)PO(6) in the coupled two-leg spin ladder system BiCu(2)PO(6). While, Zn shows complete solid solubility, Ni could be doped to about 20% and Ca to about 15%. Magnetization and heat capacity data in the undoped compound point towards the existence of frustration effects. In all the samples, the χ(T) at low temperature increases with doping content. The Zn-induced susceptibility is smaller than that due to effective S = 1/2 moments, possibly due to frustrating next-nearest-neighbor interactions along the leg. For Zn content x>0.01, χ(T) deviates from the Curie law at low temperatures. The magnetic specific heat data C(m)(T) for the Zn-doped samples show weak anomalies at low temperature, in agreement with the χ(T) behavior. The anomalies are suggestive of spin freezing at low- T. In contrast, prominent effects are observed in χ(T) and C(m)(T) on Ni-doped samples. The zero-field-cooled (ZFC) and field-cooled (FC) χ(T) data are different from each other at low temperature, unlike that for Zn-doped samples, clearly indicating a transition to a spin-glass-like phase. No anomalies were found in Ca- or Pb-doped samples.
我们报告了未掺杂样品以及 Zn 掺杂(S = 0)在 Cu 位的 BiCu(2(1-x))Zn(2x)PO(6)、Ni 掺杂(S = 1)在 Cu 位的 BiCu(2(1-y))Ni(2y)PO(6)和 Ca 掺杂(空穴)在 Bi 位的 Bi(1-z)Ca(z)Cu(2)PO(6)中的 BiCu(2)PO(6)耦合双 leg 自旋梯系统中的制备、X 射线衍射、磁化率 χ(T)和比热 C(p)(T)测量。虽然 Zn 表现出完全的固溶度,但 Ni 可以掺杂到约 20%,Ca 可以掺杂到约 15%。未掺杂化合物的磁化和比热数据表明存在挫折效应。在所有样品中,低温下的 χ(T)随掺杂含量的增加而增加。Zn 诱导的磁化率小于有效 S = 1/2 矩的磁化率,这可能是由于沿腿的相邻近邻相互作用令人沮丧。对于 Zn 含量 x>0.01,χ(T)在低温下偏离居里定律。Zn 掺杂样品的磁比热数据 C(m)(T)在低温下表现出微弱的异常,与 χ(T)行为一致。这些异常表明在低温下自旋冻结。相比之下,在 Ni 掺杂样品中观察到 χ(T)和 C(m)(T)的显著影响。零场冷却(ZFC)和磁场冷却(FC)χ(T)数据在低温下彼此不同,与 Zn 掺杂样品不同,清楚地表明向自旋玻璃样相转变。在 Ca-或 Pb 掺杂样品中未发现异常。