Institute of Physics of Materials, Academy of Sciences of the Czech Republic, Žižkova 22, CZ-616 62 Brno, Czech Republic.
J Phys Condens Matter. 2010 Nov 3;22(43):435402. doi: 10.1088/0953-8984/22/43/435402. Epub 2010 Oct 7.
Lattice dynamics of the quasi-one-dimensional ferromagnetic chain-like structure of CsNiF(3) has been studied using density functional theory and the direct method. Investigations were limited to the harmonic approximation. Antiferromagnetic and ferromagnetic spin orderings on Ni atoms were considered. It is found that phonons remain practically insensitive to the type of magnetic arrangement. The difference in the calculated Helmholtz free energies between antiferro- and ferromagnetic ordering is too small to provide sufficient information on the preference of the type of magnetic ordering in CsNiF(3). Calculated acoustic phonons agree very well with the inelastic neutron scattering experiments, while the optical phonons remain in an acceptable agreement with Raman and infrared measurements. Comparison of the experimental heat capacity and the calculated lattice contribution to the heat capacity shows that the magnetic contribution is negligible above 20-30 K. Thermal motions of particular atoms in CsNiF(3) crystals are highly anisotropic with surprisingly high mean-squared vibrations of Cs ions which exceed thermal vibrations of very light F ions. Such a behavior could be explained by the difference of the force constants between the Cs and F sites which overcomes the effect associated with the difference between masses of Cs and F ions. Nickel cations reveal very high on-site force constants, i.e. very low amplitudes of thermal vibrations, as they form some kind of rigid rods in the CsNiF(3) lattice. Calculated elastic constants indicate CsNiF(3) to be rather a soft material.
采用密度泛函理论和直接法研究了 CsNiF(3)准一维的亚铁磁链状结构的晶格动力学。研究仅限于谐波近似。考虑了 Ni 原子上的反铁磁和铁磁自旋有序。结果表明,声子对磁排列类型几乎不敏感。反铁磁和铁磁有序之间计算出的亥姆霍兹自由能的差异太小,无法提供关于 CsNiF(3)中磁有序类型偏好的充分信息。计算出的声学声子与非弹性中子散射实验非常吻合,而光学声子与拉曼和红外测量仍保持可接受的一致性。实验热容与晶格对热容的贡献的比较表明,在 20-30 K 以上,磁贡献可以忽略不计。CsNiF(3)晶体中特定原子的热运动具有高度各向异性,Cs 离子的均方振动值出人意料地高,超过了非常轻的 F 离子的热振动。这种行为可以通过 Cs 和 F 位之间的力常数之间的差异来解释,这种差异克服了 Cs 和 F 离子质量差异所带来的影响。镍阳离子表现出非常高的局域力常数,即热振动的振幅非常低,因为它们在 CsNiF(3)晶格中形成某种刚性棒。计算出的弹性常数表明 CsNiF(3)是一种相当柔软的材料。