Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831-6071, USA.
J Phys Condens Matter. 2012 Dec 12;24(49):496001. doi: 10.1088/0953-8984/24/49/496001. Epub 2012 Nov 12.
The diruthenium compound Ru(2)(O(2)CMe)(4)[Cr(CN)(6)] contains two weakly coupled, ferrimagnetically ordered sublattices occupying the same volume. Due to the weak, antiferromagnetic dipolar interaction K(c) ≈ 5 × 10(-3) meV between sublattices, a small magnetic field H(c) ∼ K(c)/μ(B) ≈ 800 Oe aligns the sublattice moments. Powder neutron-diffraction measurements on a deuterated sample confirm an earlier prediction that the sublattice moments are restricted by the anisotropy of the diruthenium 'paddle-wheels' to the cubic diagonals. Those measurements also suggest that quantum corrections to the ground state are significant.
该双钌化合物 Ru(2)(O(2)CM e)(4)[Cr(CN)(6)] 包含两个弱耦合的、铁磁有序的子晶格,它们占据相同的体积。由于子晶格之间的弱反铁磁偶极相互作用 K(c)≈5×10(-3)meV,一个小磁场 H(c)≈K(c)/μ(B)≈800 Oe 会使子晶格磁矩对齐。对氘代样品的粉末中子衍射测量证实了早先的预测,即子晶格磁矩受到双钌“桨轮”各向异性的限制,只能在立方对角线方向上运动。这些测量还表明,基态的量子修正非常显著。