posted on 2014-08-18, 00:00authored byJian Lin, Kariem Diefenbach, Naoki Kikugawa, Ryan E. Baumbach, Thomas E. Albrecht-Schmitt
Twenty-two new lanthanide tellurite
sulfates with five distinct structures, Ln<sub>2</sub>(Te<sub>2</sub>O<sub>5</sub>)(SO<sub>4</sub>)<sub>2</sub> (Ln = La, Ce, Pr, Nd,
Sm, Eu, Gd, Tb; <b>LnTeSO-1</b>), Ho<sub>3</sub>(TeO<sub>3</sub>)<sub>2</sub>(SO<sub>4</sub>)<sub>2</sub>(OH)(H<sub>2</sub>O) (<b>LnTeSO-2</b>), Ln<sub>2</sub>TeO<sub>3</sub>(SO<sub>4</sub>)<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub> (Ln = Dy, Ho, Er; <b>LnTeSO-3</b>), Ln<sub>2</sub>(Te<sub>2</sub>O<sub>5</sub>)(SO<sub>4</sub>)<sub>2</sub> (Ln = Er, Tm, Yb, Lu; <b>LnTeSO-4</b>), and Ln<sub>2</sub>(Te<sub>4</sub>O<sub>10</sub>)(SO<sub>4</sub>) (Ln = Gd, Dy,
Ho, Er, Tm, Yb; <b>LnTeSO-5</b>), have been prepared and characterized.
The topologies of <b>LnTeSO-1</b>, <b>LnTeSO-2</b>, <b>LnTeSO-3</b>, <b>LnTeSO-4</b>, and <b>LnTeSO-5</b> are substantially different with respect to the connectivity between
Ln polyhedra and the coordination environments of the lanthanide ions.
For the first four topologies, the dimensionality changes from layered
(<b>LnTeSO-1</b>) to chains (<b>LnTeSO-2</b>) to tetramers
(<b>LnTeSO-3</b>) and finally to a monomer (<b>LnTeSO-4</b>). The coordination numbers of lanthanides decrease from nine (<b>LnTeSO-1</b>) to eight (<b>LnTeSO-2</b> and <b>LnTeSO-3</b>) to seven and six (<b>LnTeSO-4</b>). We attribute the transitions
to a decrease in the ionic radii of the 4f ions. Magnetic susceptibility
measurements reveal no evidence for long-range magnetic ordering in
these materials. However, diverse short-range magnetic correlations
were observed within <b>LnTeSO-1</b>.