X-ray and Neutron Diffraction Studies of SrTe2FeO6Cl, an Oxide Chloride with Rare Anion Ordering
Open Access
- 2 August 2023
- journal article
- research article
- Published by American Chemical Society (ACS) in Inorganic Chemistry
- Vol. 62 (32) , 13081-13088
Abstract
The oxychloride SrTe2FeO6Cl is obtained by high-temperature solid-state synthesis under inert conditions in closed reaction vessels. The compound crystallizes in a novel monoclinic crystal structure that is described in the space group P121/n1 (No. 14). The unit cell parameters, a = 10.2604(1) Å, b = 5.34556(5) Å, c = 26.6851(3) Å, and β = 93.6853(4)°, and atomic parameters were determined from synchrotron diffraction data, starting from a model that was obtained from single-crystal X-ray diffraction data. The anion lattice exhibits a rare ordering of oxide and chloride ions: one-dimensional zig-zag ladders of chlorine (squarelike motif) are surrounded by an oxygen matrix. Two different iron sites coordinated solely to oxygen are present in the structure, one octahedral and one square pyramidal, both distorted. Similarly, two different strontium coordinations are present; the first homoleptic coordinated to eight oxygen atoms and the second heteroleptic coordinated to four oxygen and four chlorine atoms in a fac-like manner. The lone pair of Te(IV) is directed toward the larger chlorine atoms. Magnetic susceptibility measurements confirm that Fe is +3 (d5) in the high-spin electronic configuration, exhibiting an almost ideal spin-only moment, μeff = 5.65 μB Fe-1. The slightly negative Weiss constant (θCW = -39 K) suggests dominating antiparallel spin-to-spin coupling in the paramagnetic temperature range, agreeing with an observed long-range antiferromagnetic spin ordering below Néel temperature, TN ∼ 13 K, and a broad second order-like anomaly in the specific heat measurement data. Low-temperature neutron diffraction data reveal that the antiferromagnetic ordered phase is C-type, with a k-vector (1/2, 1/2, 0) and ordered moment of 4.14(7) μB. The spin structure can be described as antiferromagnetic ordered layers stacked along the a-axis, forming layers of squares that alternate along the c-axis.Keywords
Funding Information
- Norges Forskningsråd (245942, 301711, 325345)
This publication has 27 references indexed in Scilit:
- Crystal structure and magnetic properties of Co2TeO3Cl2 and Co2TeO3Br2Journal of Solid State Chemistry, 2006
- WinPLOTR: A Windows Tool for Powder Diffraction Pattern AnalysisMaterials Science Forum, 2001
- Dielectric properties and structure of Bi4NbO8Cl and Bi4TaO8ClJournal of Materials Chemistry, 2001
- Tetrahedral Clusters of Copper(II): Crystal Structures and Magnetic Properties of Cu2Te2O5X2 (X = Cl, Br)Chemistry of Materials, 2000
- Superconductivity and Antiferromagnetism in High- T c CupratesScience, 1997
- E.s.d.'s and estimated probable error obtained in Rietveld refinements with local correlationsJournal of Applied Crystallography, 1991
- Structure refinement of an FeCl3 crystal using a thin plate sampleJournal of Applied Crystallography, 1989
- Structure and luminescence of some rare earth halotungstates of the type Ln3WO6Cl3Journal of Solid State Chemistry, 1982
- Crystal structures of caesium and rubidium chlorochromates, CsCrO3Cl and RbCrO3ClJournal of Chemical Crystallography, 1974
- Structure cristalline de l'oxychlorure de baryum, Ba4OCl6Acta Crystallographica Section B: Structural Science, Crystal Engineering and Materials, 1970