JOURNAL ARTICLE

Photoluminescence and Magnetism in the New Magnetic\nSemiconductors:  K<sub>2</sub>Cd<sub>3(1</sub><sub>-</sub><i><sub>x</sub></i><sub>)</sub>Mn<sub>3</sub><i><sub>x</sub></i>S<sub>4</sub>

Abstract

A new family of magnetic semiconductors, K<sub>2</sub>Cd<sub>3(1</sub><sub>-</sub><i><sub>x</sub></i><sub>)</sub>Mn<sub>3</sub><i><sub>x</sub></i>S<sub>4</sub>, prepared from molten K<sub>2</sub>S<i><sub>x</sub></i>\nis reported. For <i>x</i> ≤ 0.6, the compounds crystallize in the K<sub>2</sub>Cd<sub>3</sub>S<sub>4</sub> structure type. The cell\nvolumes of the series obey Vegard's Law for solid solutions. The compounds range in color\nfrom yellow through orange brown to red and possess platelike morphologies. A structural\ntransformation occurs between <i>x</i> = 0.7 and <i>x</i> = 0.9. Red plates of K<sub>2</sub>Cd<sub>0.4</sub>Mn<sub>2.6</sub>S<sub>4</sub> (<i>x</i> = 0.87)\ncrystallize in the space group <i>Ccca</i> with <i>a </i>= 5.9217(8) Å, <i>b </i>= 13.531(1) Å, <i>c</i> = 11.0696(8) Å,\nand <i>V</i> = 887.0(1) Å<sup>3</sup>. The end member, K<sub>2</sub>Mn<sub>3</sub>S<sub>4</sub>, crystallizes in the space group <i>Ccca</i> with\n<i>a</i> = 11.0637(7) Å, <i>b </i>= 26.830(2) Å <i>c </i>= 5.8180(4) Å, and <i>V</i> = 1727 Å<sup>3</sup>. For <i>x</i> ≤ 0.6, the\ncompounds form as (M<sub>3</sub>S<sub>4</sub>)<i><sub>n</sub></i><sup>2</sup><i><sup>n</sup></i><sup>-</sup> layers, interspersed by K<sup>+</sup> cations. These layers are composed\nonly of M<sub>3</sub>S<sub>4</sub><sup>2-</sup> units shaped like truncated cubes. When <i>x</i> = 0.87, a new structure related to\nthat of Cs<sub>2</sub>Mn<sub>3</sub>S<sub>4</sub> is observed. The end member of the series (i.e., <i>x</i> = 1) K<sub>2</sub>Mn<sub>3</sub>S<sub>4</sub> is revealed\nto have a related yet surprising structure. The compounds display room-temperature band\ngaps ranging from 2.79 to 2.92 eV. Absorptions in the mid-gap region, due to Mn<sup>2+</sup>-based\nd−d transitions, are also observed. The compounds are strongly emissive in the visible\nspectrum at room temperature, with the light emission shifted to the red immediately upon\nthe introduction of small amounts of manganese. The magnetic properties of these compounds\nevolve from classical paramagnetic to spin glass as a function of <i>x</i>. For <i>x</i> ≥ 0.05, the\ncompounds deviate from Curie−Weiss behavior. Antiferromagnetic coupling is observed in\nall cases. With very high Mn content transitions to magnetically complex phases are observed\nwith possible spin-glass-like behavior.

Keywords:
Magnetism Antiferromagnetism Photoluminescence Paramagnetism Solid solution Magnetic structure Spin glass Crystal structure

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