U.S. Department of EnergyOffice of Scientific and Technical Information
Materials Data on Li4Ti2Mn3Nb3O16 (SG:8) by Materials Project
Abstract
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
- Authors:
- Publication Date:
- Other Number(s):
- mp-762518
- 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; Li4 Mn3 Nb3 O16 Ti2; Li-Mn-Nb-O-Ti;
- OSTI Identifier:
- 1292695
- DOI:
- https://doi.org/10.17188/1292695
Citation Formats
The Materials Project. Materials Data on Li4Ti2Mn3Nb3O16 (SG:8) by Materials Project. United States: N. p., 2016.
Web. doi:10.17188/1292695.
The Materials Project. Materials Data on Li4Ti2Mn3Nb3O16 (SG:8) by Materials Project. United States. doi:https://doi.org/10.17188/1292695
The Materials Project. 2016.
"Materials Data on Li4Ti2Mn3Nb3O16 (SG:8) by Materials Project". United States. doi:https://doi.org/10.17188/1292695. https://www.osti.gov/servlets/purl/1292695. Pub date:Fri Apr 22 00:00:00 EDT 2016
@article{osti_1292695,
title = {Materials Data on Li4Ti2Mn3Nb3O16 (SG:8) by Materials Project},
author = {The Materials Project},
abstractNote = {Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations},
doi = {10.17188/1292695},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Fri Apr 22 00:00:00 EDT 2016},
month = {Fri Apr 22 00:00:00 EDT 2016}
}
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