<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Ovchinnikov A</submitter><funding>U.S. Department of Energy</funding><funding>Basic Energy Sciences</funding><funding>Office of Science</funding><pagination>446-450</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC6312832</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>22</volume><pubmed_abstract>Electronic band structures of the following compounds - Cs&lt;sub>4&lt;/sub>Cd(As&lt;sub>7&lt;/sub>)&lt;sub>2&lt;/sub>, K&lt;sub>2&lt;/sub>PdP&lt;sub>2&lt;/sub>, K&lt;sub>5&lt;/sub>CuAs&lt;sub>2&lt;/sub>, Na&lt;sub>2&lt;/sub>CuP and K&lt;sub>3&lt;/sub>Cu&lt;sub>3&lt;/sub>P&lt;sub>2&lt;/sub> - all computed by means of the TB-LMTO-ASA code. The calculations show that for all compounds, the bonding states are occupied, while the antibonding orbitals are vacant. This confirms the partitioning of the valence electrons according to the Zintl-Klemm formalism. &lt;i>The data is related to&lt;/i>doi.org/10.1016/j.jssc.2018.11.029 (Ovchinnikov and Bobev, 2019) [1].</pubmed_abstract><journal>Data in brief</journal><pubmed_title>Data from the electronic band structures of several Zintl phases with group 15 elements and the transition metals.</pubmed_title><pmcid>PMC6312832</pmcid><funding_grant_id>DE-SC0008885</funding_grant_id><pubmed_authors>Bobev S</pubmed_authors><pubmed_authors>Ovchinnikov A</pubmed_authors></additional><is_claimable>false</is_claimable><name>Data from the electronic band structures of several Zintl phases with group 15 elements and the transition metals.</name><description>Electronic band structures of the following compounds - Cs&lt;sub>4&lt;/sub>Cd(As&lt;sub>7&lt;/sub>)&lt;sub>2&lt;/sub>, K&lt;sub>2&lt;/sub>PdP&lt;sub>2&lt;/sub>, K&lt;sub>5&lt;/sub>CuAs&lt;sub>2&lt;/sub>, Na&lt;sub>2&lt;/sub>CuP and K&lt;sub>3&lt;/sub>Cu&lt;sub>3&lt;/sub>P&lt;sub>2&lt;/sub> - all computed by means of the TB-LMTO-ASA code. The calculations show that for all compounds, the bonding states are occupied, while the antibonding orbitals are vacant. This confirms the partitioning of the valence electrons according to the Zintl-Klemm formalism. &lt;i>The data is related to&lt;/i>doi.org/10.1016/j.jssc.2018.11.029 (Ovchinnikov and Bobev, 2019) [1].</description><dates><release>2019-01-01T00:00:00Z</release><publication>2019 Feb</publication><modification>2025-04-19T22:52:36.25Z</modification><creation>2019-03-26T22:55:09Z</creation></dates><accession>S-EPMC6312832</accession><cross_references><pubmed>30619921</pubmed><doi>10.1016/j.dib.2018.12.040</doi></cross_references></HashMap>