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Li<sub>12</sub>P<sub>3</sub>N<sub>9</sub> with Non‐Condensed [P<sub>3</sub>N<sub>9</sub>]<sup>12−</sup>‐Rings and its High‐Pressure Polymorph Li<sub>4</sub>PN<sub>3</sub> with Infinite Chains of PN<sub>4</sub>‐Tetrahedra

36

Citations

50

References

2017

Year

Abstract

Li<sub>12</sub> P<sub>3</sub> N<sub>9</sub> was synthesized by solid-state reaction of Li<sub>3</sub> N and P<sub>3</sub> N<sub>5</sub> at 790 °C. It is made up of non-condensed [P<sub>3</sub> N<sub>9</sub> ]<sup>12-</sup> dreier-rings of PN<sub>4</sub> -tetrahedra. The corresponding high-pressure polymorph, Li<sub>4</sub> PN<sub>3</sub> , was synthesized under high-pressure/high-temperature conditions from Li<sub>12</sub> P<sub>3</sub> N<sub>9</sub> or LiPN<sub>2</sub> and Li<sub>7</sub> PN<sub>4</sub> at 6 or 7 GPa, respectively, using the multianvil technique. Li<sub>4</sub> PN<sub>3</sub> is the first lithium catena-nitridophosphate and contains PN<sub>3</sub> zweier-chains of corner sharing PN<sub>4</sub> -tetrahedra. To confirm the structure elucidated from single-crystal X-ray data, Rietveld refinement, <sup>6</sup> Li, <sup>7</sup> Li, and <sup>31</sup> P solid-state NMR spectroscopy, FTIR spectroscopy and EDX measurements were carried out. To examine the phase transition of Li<sub>12</sub> P<sub>3</sub> N<sub>9</sub> to Li<sub>4</sub> PN<sub>3</sub> at 6 GPa and to corroborate the latter as the corresponding high-pressure polymorph, DFT calculations were conducted. Electronic band gap and electron localization function (ELF) calculations were carried out to elucidate the electronic properties and bonding behavior of both polymorphs.

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