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Title: Materials Data on Rb2MnSO4F3 by Materials Project

Abstract

Rb2MnSO4F3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 9-coordinate geometry to five O2- and four F1- atoms. There are a spread of Rb–O bond distances ranging from 2.89–3.55 Å. There are a spread of Rb–F bond distances ranging from 2.94–3.08 Å. In the second Rb1+ site, Rb1+ is bonded in a 7-coordinate geometry to three O2- and four F1- atoms. There are a spread of Rb–O bond distances ranging from 2.87–3.06 Å. There are a spread of Rb–F bond distances ranging from 2.89–3.08 Å. There are two inequivalent Mn3+ sites. In the first Mn3+ site, Mn3+ is bonded to two equivalent O2- and four F1- atoms to form MnO2F4 octahedra that share corners with two equivalent MnO2F4 octahedra and corners with two equivalent SO4 tetrahedra. The corner-sharing octahedral tilt angles are 52°. Both Mn–O bond lengths are 2.20 Å. There is two shorter (1.87 Å) and two longer (1.95 Å) Mn–F bond length. In the second Mn3+ site, Mn3+ is bonded to two equivalent O2- and four F1- atoms to form MnO2F4 octahedra that share corners with two equivalent MnO2F4more » octahedra and corners with two equivalent SO4 tetrahedra. The corner-sharing octahedral tilt angles are 52°. Both Mn–O bond lengths are 1.98 Å. There are two shorter (1.88 Å) and two longer (2.21 Å) Mn–F bond lengths. S6+ is bonded to four O2- atoms to form SO4 tetrahedra that share corners with two MnO2F4 octahedra. The corner-sharing octahedral tilt angles are 49°. There are a spread of S–O bond distances ranging from 1.47–1.54 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to three Rb1+ and one S6+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to two Rb1+ and one S6+ atom. In the third O2- site, O2- is bonded in a 2-coordinate geometry to one Rb1+, one Mn3+, and one S6+ atom. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to two Rb1+, one Mn3+, and one S6+ atom. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted single-bond geometry to three Rb1+ and one Mn3+ atom. In the second F1- site, F1- is bonded in a distorted single-bond geometry to three Rb1+ and one Mn3+ atom. In the third F1- site, F1- is bonded in a 2-coordinate geometry to two Rb1+ and two Mn3+ atoms.« less

Authors:
Publication Date:
Other Number(s):
mp-19488
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; Rb2MnSO4F3; F-Mn-O-Rb-S
OSTI Identifier:
1194524
DOI:
https://doi.org/10.17188/1194524

Citation Formats

The Materials Project. Materials Data on Rb2MnSO4F3 by Materials Project. United States: N. p., 2019. Web. doi:10.17188/1194524.
The Materials Project. Materials Data on Rb2MnSO4F3 by Materials Project. United States. doi:https://doi.org/10.17188/1194524
The Materials Project. 2019. "Materials Data on Rb2MnSO4F3 by Materials Project". United States. doi:https://doi.org/10.17188/1194524. https://www.osti.gov/servlets/purl/1194524. Pub date:Sat Nov 16 00:00:00 EST 2019
@article{osti_1194524,
title = {Materials Data on Rb2MnSO4F3 by Materials Project},
author = {The Materials Project},
abstractNote = {Rb2MnSO4F3 crystallizes in the monoclinic P2_1/c space group. The structure is three-dimensional. there are two inequivalent Rb1+ sites. In the first Rb1+ site, Rb1+ is bonded in a 9-coordinate geometry to five O2- and four F1- atoms. There are a spread of Rb–O bond distances ranging from 2.89–3.55 Å. There are a spread of Rb–F bond distances ranging from 2.94–3.08 Å. In the second Rb1+ site, Rb1+ is bonded in a 7-coordinate geometry to three O2- and four F1- atoms. There are a spread of Rb–O bond distances ranging from 2.87–3.06 Å. There are a spread of Rb–F bond distances ranging from 2.89–3.08 Å. There are two inequivalent Mn3+ sites. In the first Mn3+ site, Mn3+ is bonded to two equivalent O2- and four F1- atoms to form MnO2F4 octahedra that share corners with two equivalent MnO2F4 octahedra and corners with two equivalent SO4 tetrahedra. The corner-sharing octahedral tilt angles are 52°. Both Mn–O bond lengths are 2.20 Å. There is two shorter (1.87 Å) and two longer (1.95 Å) Mn–F bond length. In the second Mn3+ site, Mn3+ is bonded to two equivalent O2- and four F1- atoms to form MnO2F4 octahedra that share corners with two equivalent MnO2F4 octahedra and corners with two equivalent SO4 tetrahedra. The corner-sharing octahedral tilt angles are 52°. Both Mn–O bond lengths are 1.98 Å. There are two shorter (1.88 Å) and two longer (2.21 Å) Mn–F bond lengths. S6+ is bonded to four O2- atoms to form SO4 tetrahedra that share corners with two MnO2F4 octahedra. The corner-sharing octahedral tilt angles are 49°. There are a spread of S–O bond distances ranging from 1.47–1.54 Å. There are four inequivalent O2- sites. In the first O2- site, O2- is bonded in a distorted single-bond geometry to three Rb1+ and one S6+ atom. In the second O2- site, O2- is bonded in a distorted single-bond geometry to two Rb1+ and one S6+ atom. In the third O2- site, O2- is bonded in a 2-coordinate geometry to one Rb1+, one Mn3+, and one S6+ atom. In the fourth O2- site, O2- is bonded in a 2-coordinate geometry to two Rb1+, one Mn3+, and one S6+ atom. There are three inequivalent F1- sites. In the first F1- site, F1- is bonded in a distorted single-bond geometry to three Rb1+ and one Mn3+ atom. In the second F1- site, F1- is bonded in a distorted single-bond geometry to three Rb1+ and one Mn3+ atom. In the third F1- site, F1- is bonded in a 2-coordinate geometry to two Rb1+ and two Mn3+ atoms.},
doi = {10.17188/1194524},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Sat Nov 16 00:00:00 EST 2019},
month = {Sat Nov 16 00:00:00 EST 2019}
}