posted on 2020-03-24, 19:36authored byXuyong Feng, Po-Hsiu Chien, Sawankumar Patel, Yan Wang, Yan-Yan Hu
Li<sub>1+2<i>x</i></sub>Zn<sub>1–<i>x</i></sub>PS<sub>4</sub> was computationally predicted to have superionic
conductivity of over 50 mS/cm. However, experimental efforts so far
have only yielded ionic conductivities on the order of 10<sup>–4</sup> S/cm, due to difficulty in producing phase-pure crystalline products.
Here, to improve phase purity and enhance ionic conductivity, Cl-
doping is employed to synthesize Li<sub>1+2<i>x</i>–<i>y</i></sub>Zn<sub>1–<i>x</i></sub>PS<sub>4–<i>y</i></sub>Cl<sub><i>y</i></sub>, which is shown to
stabilize Li<sub>1+2<i>x</i></sub>Zn<sub>1–<i>x</i></sub>PS<sub>4</sub> from decomposing to Li<sub>3</sub>PS<sub>4</sub>. Li<sub>2.5</sub>Zn<sub>0.25</sub>PS<sub>4</sub> which
shows the highest ionic conductivity among the Li<sub>1+2<i>x</i></sub>Zn<sub>1–<i>x</i></sub>PS<sub>4</sub> samples
is chosen as an example to study. After incorporating only a small
amount of Cl, the ionic conductivity increases from 0.6 mS/cm for
Li<sub>2.5</sub>Zn<sub>0.25</sub>PS<sub>4</sub> to 3.5 mS/cm for Li<sub>2.4</sub>Zn<sub>0.25</sub>PS<sub>3.9</sub>Cl<sub>0.1</sub> at 25
°C. In addition, the activation energy is reduced from 0.33 to
0.27 eV. The phase purity and fine structure of Li<sub>1+2<i>x</i>–<i>y</i></sub>Zn<sub>1–<i>x</i></sub>PS<sub>4–<i>y</i></sub>Cl<sub><i>y</i></sub> are determined with XRD, and <sup>7</sup>Li, <sup>31</sup>P, <sup>35</sup>Cl solid-state NMR characterizations. The
experimental data confirm the success of Cl<sup>–</sup> doping.
In addition, Li<sub>2.4</sub>Zn<sub>0.25</sub>PS<sub>3.9</sub>Cl<sub>0.1</sub> exhibits a low electronic conductivity of 1.21 × 10<sup>–9</sup> S/cm and a wide electrochemical stability window.