Materials Data on Li9(RuO3)10 by Materials Project

doi:10.17188/1282977

Title: Materials Data on Li9(RuO3)10 by Materials Project

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Abstract

Li9(RuO3)10 is beta indium sulfide-derived structured and crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are five inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with five LiO6 octahedra and edges with six RuO6 octahedra. The corner-sharing octahedra tilt angles range from 52–55°. There are a spread of Li–O bond distances ranging from 2.20–2.29 Å. In the second Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with five LiO6 octahedra and edges with six RuO6 octahedra. The corner-sharing octahedra tilt angles range from 52–55°. There are a spread of Li–O bond distances ranging from 2.19–2.34 Å. In the third Li1+ site, Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with six LiO6 octahedra, corners with six RuO6 octahedra, and faces with two RuO6 octahedra. The corner-sharing octahedra tilt angles range from 37–55°. There are a spread of Li–O bond distances ranging from 2.17–2.27 Å. In the fourth Li1+ site, Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with four LiO6more »« less

Authors:: The Materials Project

Publication Date:: 2020-06-05

Other Number(s):: mp-676252

DOE Contract Number:: AC02-05CH11231; EDCBEE

Research Org.:: Lawrence Berkeley National Lab. (LBNL), Berkeley, CA (United States). LBNL Materials Project

Sponsoring Org.:: USDOE Office of Science (SC), Basic Energy Sciences (BES)

Collaborations:: MIT; UC Berkeley; Duke; U Louvain

Subject:: 36 MATERIALS SCIENCE

Keywords:: crystal structure; Li9(RuO3)10; Li-O-Ru

OSTI Identifier:: 1282977

DOI:: https://doi.org/10.17188/1282977

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                    The Materials Project. Materials Data on Li9(RuO3)10 by Materials Project.  United States: N. p., 2020. 
        Web.  doi:10.17188/1282977.

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                    The Materials Project. Materials Data on Li9(RuO3)10 by Materials Project.  United States.  doi:https://doi.org/10.17188/1282977

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                    The Materials Project. 2020.  
"Materials Data on Li9(RuO3)10 by Materials Project".  United States.  doi:https://doi.org/10.17188/1282977.  https://www.osti.gov/servlets/purl/1282977. Pub date:Fri Jun 05 00:00:00 EDT 2020

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@article{osti_1282977,

  title        = {Materials Data on Li9(RuO3)10 by Materials Project},

  author       = {The Materials Project},

  abstractNote = {Li9(RuO3)10 is beta indium sulfide-derived structured and crystallizes in the triclinic P-1 space group. The structure is three-dimensional. there are five inequivalent Li1+ sites. In the first Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with five LiO6 octahedra and edges with six RuO6 octahedra. The corner-sharing octahedra tilt angles range from 52–55°. There are a spread of Li–O bond distances ranging from 2.20–2.29 Å. In the second Li1+ site, Li1+ is bonded to six O2- atoms to form LiO6 octahedra that share corners with five LiO6 octahedra and edges with six RuO6 octahedra. The corner-sharing octahedra tilt angles range from 52–55°. There are a spread of Li–O bond distances ranging from 2.19–2.34 Å. In the third Li1+ site, Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with six LiO6 octahedra, corners with six RuO6 octahedra, and faces with two RuO6 octahedra. The corner-sharing octahedra tilt angles range from 37–55°. There are a spread of Li–O bond distances ranging from 2.17–2.27 Å. In the fourth Li1+ site, Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with four LiO6 octahedra and edges with six RuO6 octahedra. The corner-sharing octahedra tilt angles range from 54–55°. There are a spread of Li–O bond distances ranging from 2.21–2.31 Å. In the fifth Li1+ site, Li1+ is bonded to six O2- atoms to form distorted LiO6 octahedra that share corners with six LiO6 octahedra, corners with six RuO6 octahedra, and faces with two RuO6 octahedra. The corner-sharing octahedra tilt angles range from 38–55°. There are a spread of Li–O bond distances ranging from 2.14–2.28 Å. There are five inequivalent Ru+5.10+ sites. In the first Ru+5.10+ site, Ru+5.10+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with two equivalent LiO6 octahedra, edges with three LiO6 octahedra, edges with three RuO6 octahedra, and a faceface with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 37–42°. There are a spread of Ru–O bond distances ranging from 1.92–2.00 Å. In the second Ru+5.10+ site, Ru+5.10+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three LiO6 octahedra, edges with three LiO6 octahedra, edges with three RuO6 octahedra, and a faceface with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 39–40°. There are a spread of Ru–O bond distances ranging from 1.95–2.01 Å. In the third Ru+5.10+ site, Ru+5.10+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with two LiO6 octahedra, edges with three LiO6 octahedra, edges with three RuO6 octahedra, and a faceface with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 39–40°. There are a spread of Ru–O bond distances ranging from 1.91–2.00 Å. In the fourth Ru+5.10+ site, Ru+5.10+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with two LiO6 octahedra, edges with three LiO6 octahedra, edges with three RuO6 octahedra, and a faceface with one LiO6 octahedra. The corner-sharing octahedra tilt angles range from 39–43°. There are a spread of Ru–O bond distances ranging from 1.92–2.02 Å. In the fifth Ru+5.10+ site, Ru+5.10+ is bonded to six O2- atoms to form RuO6 octahedra that share corners with three LiO6 octahedra, edges with three LiO6 octahedra, and edges with three RuO6 octahedra. The corner-sharing octahedra tilt angles range from 38–39°. There are a spread of Ru–O bond distances ranging from 1.94–1.99 Å. There are fifteen inequivalent O2- sites. In the first O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Ru+5.10+ atoms. In the second O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Ru+5.10+ atoms. In the third O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Ru+5.10+ atoms. In the fourth O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Ru+5.10+ atoms. In the fifth O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Ru+5.10+ atoms. In the sixth O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two equivalent Ru+5.10+ atoms. In the seventh O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Ru+5.10+ atoms. In the eighth O2- site, O2- is bonded in a distorted rectangular see-saw-like geometry to two Li1+ and two Ru+5.10+ atoms. In the ninth O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two equivalent Ru+5.10+ atoms. In the tenth O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two equivalent Ru+5.10+ atoms. In the eleventh O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Ru+5.10+ atoms. In the twelfth O2- site, O2- is bonded in a rectangular see-saw-like geometry to two Li1+ and two Ru+5.10+ atoms. In the thirteenth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one Li1+ and two Ru+5.10+ atoms. In the fourteenth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one Li1+ and two Ru+5.10+ atoms. In the fifteenth O2- site, O2- is bonded in a distorted trigonal non-coplanar geometry to one Li1+ and two Ru+5.10+ atoms.},

  doi          = {10.17188/1282977},

  journal      = {},

  number       = ,

  volume       = ,

  place        = {United States},

  year         = {2020},

  month        = {6}

}

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DOI: https://doi.org/10.17188/1282977

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