Antiferromagnetic Order and Spin-Canting Transition in the Corrugated Square Net Compound Cu3(TeO4)(SO4)•H2O

被引:4
|
作者
Wang, Zhi-Cheng [2 ]
Thanabalasingam, Kulatheepan [1 ]
Scheifers, Jan P. [1 ]
Streeter, Alenna [2 ]
McCandless, Gregory T. [1 ]
Gaudet, Jonathan [3 ,4 ]
Brown, Craig M. [4 ]
Segre, Carlo U. [5 ,6 ]
Chan, Julia Y. [1 ]
Tafti, Fazel [2 ]
机构
[1] Univ Texas Dallas, Dept Chem & Biochem, Richardson, TX 75080 USA
[2] Boston Coll, Dept Phys, Chestnut Hill, MA 02467 USA
[3] Maryland Univ, Dept Mat Sci & Engn, College Pk, MD 20942 USA
[4] NIST, Ctr Neutron Res, Gaithersburg, MD 20899 USA
[5] IIT, Dept Phys, Chicago, IL 60616 USA
[6] IIT, CSRRI, Chicago, IL 60616 USA
基金
美国国家科学基金会;
关键词
CRYSTAL-STRUCTURE; ELECTRONIC-STRUCTURE; OXIDES;
D O I
10.1021/acs.inorgchem.1c01220
中图分类号
O61 [无机化学];
学科分类号
070301 ; 081704 ;
摘要
Strongly correlated electrons in layered perovskite structures have been the birthplace of high-temperature superconductivity, spin liquids, and quantum criticality. Specifically, the cuprate materials with layered structures made of cornersharing square-planar CuO4 units have been intensely studied due to their Mott insulating ground state, which leads to high-temperature superconductivity upon doping. Identifying new compounds with similar lattice and electronic structures has become a challenge in solid-state chemistry. Here, we report the hydrothermal crystal growth of a new copper tellurite sulfate, Cu-3(TeO4)(SO4)center dot H2O, a promising alternative to layered perovskites. The orthorhombic phase (space group Pnma) is made of corrugated layers of corner-sharing CuO4 square-planar units that are edge-shared with TeO4 units. The layers are linked by slabs of corner-sharing CuO4 and SO4. Using both the bond valence sum analysis and magnetization data, we find purely Cu2+ ions within the layers but a mixed valence of Cu2+/Cu+ between the layers. Cu-3(TeO4)(SO4)center dot H2O undergoes an antiferromagnetic transition at TN = 67 K marked by a peak in the magnetic susceptibility. Upon further cooling, a spin-canting transition occurs at T* = 12 K, evidenced by a kink in the heat capacity. The spin-canting transition is explained on the basis of a J(1)-J(2) model of magnetic interactions, which is consistent with the slightly different in-plane superexchange paths. We present Cu-3(TeO4)(SO4)center dot H2O as a promising platform for the future doping and strain experiments that could tune the Mott insulating ground state into superconducting or spin liquid states.
引用
收藏
页码:10565 / 10571
页数:7
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