Role of Na<sup>+</sup> Interstitials and Dopants in Enhancing the Na<sup>+</sup> Conductivity of the Cubic Na<sub>3</sub>PS<sub>4</sub> Superionic Conductor

Abstract

In this work, we performed a first-principles investigation of the phase stability, dopant formation energy and Na<sup>+</sup> conductivity of pristine and doped cubic Na<sub>3</sub>PS<sub>4</sub> (c-Na<sub>3</sub>PS<sub>4</sub>). We show that pristine c-Na<sub>3</sub>PS<sub>4</sub> is an extremely poor Na ionic conductor, and the introduction of Na<sup>+</sup> excess is the key to achieving reasonable Na<sup>+</sup> conductivities. We studied the effect of aliovalent doping of M<sup>4+</sup> for P<sup>5+</sup> in c-Na<sub>3</sub>PS<sub>4</sub>, yielding Na<sub>3+<i>x</i></sub>M<sub><i>x</i></sub>P<sub>1–<i>x</i></sub>S<sub>4</sub> (M = Si, Ge, and Sn with <i>x</i> = 0.0625; M = Si with <i>x</i> = 0.125). The formation energies in all the doped structures with dopant concentration of <i>x</i> = 0.0625 are found to be relatively low. Using <i>ab initio</i> molecular dynamics simulations, we predict that 6.25% Si-doped c-Na<sub>3</sub>PS<sub>4</sub> has a Na<sup>+</sup> conductivity of 1.66 mS/cm, in excellent agreement with previous experimental results. Remarkably, we find that Sn<sup>4+</sup> doping at the same concentration yields a much higher predicted Na<sup>+</sup> conductivity of 10.7 mS/cm, though with a higher dopant formation energy. A higher Si<sup>4+</sup> doping concentration of <i>x</i> = 0.125 also yields a significant increase in Na<sup>+</sup> conductivity with an even higher dopant formation energy. Finally, topological and van Hove correlation function analyses suggest that the channel volume and correlation in Na<sup>+</sup> motions may play important roles in enhancing Na<sup>+</sup> conductivity in this structure

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