U.S. Department of EnergyOffice of Scientific and Technical Information
Materials Data on FeTe6O13 (SG:148) 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-565337
- 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; Fe1 O13 Te6; Fe-O-Te; ICSD-417293; electronic bandstructure
- OSTI Identifier:
- 1272472
- DOI:
- https://doi.org/10.17188/1272472
Citation Formats
The Materials Project. Materials Data on FeTe6O13 (SG:148) by Materials Project. United States: N. p., 2014.
Web. doi:10.17188/1272472.
The Materials Project. Materials Data on FeTe6O13 (SG:148) by Materials Project. United States. doi:https://doi.org/10.17188/1272472
The Materials Project. 2014.
"Materials Data on FeTe6O13 (SG:148) by Materials Project". United States. doi:https://doi.org/10.17188/1272472. https://www.osti.gov/servlets/purl/1272472. Pub date:Wed Jul 09 00:00:00 EDT 2014
@article{osti_1272472,
title = {Materials Data on FeTe6O13 (SG:148) 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 = {10.17188/1272472},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Wed Jul 09 00:00:00 EDT 2014},
month = {Wed Jul 09 00:00:00 EDT 2014}
}
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