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arXiv 0812.4540cond-mat.str-elcond-mat.mtrl-sci
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反铁磁性S = 1链状化合物CaV2O4的单晶生长、结晶学、磁化率、Heat Capacity和热膨胀

Single Crystal Growth, Crystallography, Magnetic Susceptibility, Heat Capacity, and Thermal Expansion of the Antiferromagnetic S = 1 Chain Compound CaV2O4

A. Niazi, S. L. Bud'ko, D. L. Schlagel, J. Q. Yan, T. A. Lograsso, A. Kreyssig, S. Das, S. Nandi, A. I. Goldman, A. Honecker, R. W. McCallum, M. Reehuis, O. Pie… 展开作者

A. Niazi, S. L. Bud'ko, D. L. Schlagel, J. Q. Yan, T. A. Lograsso, A. Kreyssig, S. Das, S. Nandi, A. I. Goldman, A. Honecker, R. W. McCallum, M. Reehuis, O. Pieper, B. Lake, D. C. Johnston

摘要:

化合物CaV 2 O 4含有自旋S = 1的V^{+3}阳离子,并且在室温下具有正交结构,含有沿c轴延伸的V原子的Z字形链。我们生长了CaV_2O_4单晶,并报道了单晶和多晶样品在1.8-350 K温度范围内的晶体学、静态磁化强度、磁化率χ、交流磁化率、热容Cp和热膨胀测量。在T_S \approx 108-145 K和T_N \approx 51-76 K的温度范围内发现了从正交到单斜的结构畸变和长程反铁磁(AF)转变。在两个退火的单晶中,在\approx 200 K发现了另一个转变.在其中一个晶体中,这种转变主要是由于退火期间晶体中相干生长的V2 O3杂质相。然而,在另一种晶体中,这种在200 K的转变的起源是未知的。χ(T)在\approx 300 K时有一个宽的最大值,与短程AF有序有关,而在T_N以上χ的各向异性很小。T_N以下的各向异性χ(T \to 0)数据表明AF磁结构的(平均)易磁化轴是b轴。Cp(T)数据表明T_N以上存在较强的短程AF有序,与χ(T)数据一致。我们用J1-J2 S = 1海森堡链模型拟合了室温附近的χ(T)数据,其中J1(J2)是(次)近邻交换相互作用。我们发现J1 \approx 230 K,令人惊讶的是,J2/J1 \approx 0(或J1/J2 \approx 0)。这些S = 1链之间的相互作用J_ \perp导致T_N处的长程AF有序,估计为J_ \perp /J_1 \gtrsim 0.04。

英文摘要:

The compound CaV2O4 contains V^{+3} cations with spin S = 1 and has an orthorhombic structure at room temperature containing zigzag chains of V atoms running along the c-axis. We have grown single crystals of CaV2O4 and report crystallography, static magnetization, magnetic susceptibility χ, ac magnetic susceptibility, heat capacity Cp, and thermal expansion measurements in the temperature T range of 1.8-350 K on the single crystals and on polycrystalline samples. An orthorhombic to monoclinic structural distortion and a long-range antiferromagnetic (AF) transition were found at sample-dependent temperatures T_S \approx 108-145 K and T_N \approx 51-76 K, respectively. In two annealed single crystals, another transition was found at \approx 200 K. In one of the crystals, this transition is mostly due to V2O3 impurity phase that grows coherently in the crystals during annealing. However, in the other crystal the origin of this transition at 200 K is unknown. The χ(T) shows a broad maximum at \approx 300 K associated with short-range AF ordering and the anisotropy of χabove T_N is small. The anisotropic χ(T \to 0) data below T_N show that the (average) easy axis of the AF magnetic structure is the b-axis. The Cp(T) data indicate strong short-range AF ordering above T_N, consistent with the χ(T) data. We fitted our χ(T) data near room temperature by a J1-J2 S = 1 Heisenberg chain model, where J1(J2) is the (next)-nearest-neighbor exchange interaction. We find J1 \approx 230 K, and surprisingly, J2/J1 \approx 0 (or J1/J2 \approx 0). The interaction J_\perp between these S = 1 chains leading to long-range AF ordering at T_N is estimated to be J_\perp/J_1 \gtrsim 0.04.

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