fig8

Towards practical all-solid-state batteries: structural engineering innovations for sulfide-based solid electrolytes

Figure 8. (A) (left) The crystal structure of Li6PS5I. (right) A face-shared S3I2 double tetrahedron with two distinct lithium-ion equivalent sites[23]. Reproduced with permission[23]. Copyright 2008, Wiley-VCH GmBH; (B) A simplified tetrahedron type in the argyrodite structure, where light gray represents PS4 groups (type 0) and dark gray indicates lithium-containing tetrahedron types (types 1-5)[131]. Reproduced with permission[131]. Copyright 2010, Wiley-VCH GmBH; (C) (upper left) Lattice parameters of Li6-xPS5-xCl1+x as a function of x. (upper right) Impedance plots at room temperature of Li6PS5Cl, Li5.75PS4.75Cl1.25, Li5.5PS4.5Cl1.5, and a sintered Li5.5PS4.5Cl1.5. (lower left) Nyquist and Arrhenius plots for Li5.5PS4.5Cl1.5. (lower right) Ionic conductivity and activation energy for Li6-xPS5-xCl1+x (x = 0, 0.25, 0.375, 0.5)[77]. Reproduced with permission[77]. Copyright 2019, Wiley-VCH GmBH; (D) (upper left) Crystal structure of Li6.7Si0.7Sb0.3S5I. (lower left) Three distinct lithium ion diffusion pathways: the doublet jump (blue arrow), the intra-cage jump (red arrow), and the inter-cage jump (orange arrow). (upper right and lower left) The crystal structure of Li6PS5I is shown for comparison, with no additional lithium ions in the structure[24]. Reproduced with permission[24]. Copyright 2019, American Chemical Society; (E) (left) Two distinct lithium-ion cages, defined by their radius from isolated S2- ions, are influenced by the Br-/S2-site disorder, and corresponding (right) lithium-ion diffusion pathways[133]. Reproduced with permission[133]. Copyright 2021, Wiley-VCH GmBH; (F) (left) The activation energy and Arrhenius prefactor as functions of X in Li6PS5X (X = Cl, Br, I). (right) The ionic conductivity as a function of X in Li6PS5X (X = Cl, Br, I)[36]. Reproduced with permission[36]. Copyright 2017, American Chemical Society.

Energy Materials
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