<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Lu XQ</submitter><funding>National Natural Science Foundation of China</funding><pagination>12469-12474</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC9051253</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>10(21)</volume><pubmed_abstract>La-doped boron nanoclusters have received considerable attention due to their unique structures and bonding. Inspired by recent experimental observations of the inverse sandwich &lt;i>D&lt;/i> &lt;sub>8h&lt;/sub> La&lt;sub>2&lt;/sub>B&lt;sub>8&lt;/sub> (1) and triple-decker &lt;i>C&lt;/i> &lt;sub>2v&lt;/sub> La&lt;sub>3&lt;/sub>B&lt;sub>14&lt;/sub> &lt;sup>-&lt;/sup> (2) and based on extensive global searches and first-principles theory investigations, we present herein the possibility of the perfect cubic La-doped boron clusters &lt;i>O&lt;/i> &lt;sub>h&lt;/sub> La&lt;sub>6&lt;/sub>&amp;[La@B&lt;sub>24&lt;/sub>]&lt;sup>+&lt;/sup> (3, &lt;sup>1&lt;/sup>A&lt;sub>1g&lt;/sub>) and &lt;i>O&lt;/i> &lt;sub>h&lt;/sub> La&lt;sub>6&lt;/sub>&amp;[La@B&lt;sub>24&lt;/sub>] (4, &lt;sup>2&lt;/sup>A&lt;sub>2g&lt;/sub>) which appear to be the embryos of the metallic one-dimensional La&lt;sub>10&lt;/sub>B&lt;sub>32&lt;/sub> (5) nanowire, two-dimensional La&lt;sub>3&lt;/sub>B&lt;sub>10&lt;/sub> (6) nanosheet, and three-dimensional LaB&lt;sub>6&lt;/sub> (7) nanocrystal, facilitating a bottom-up approach to build cubic lanthanide boride nanostructures from gas-phase clusters. Detailed molecular orbital and bonding analyses indicate that effective (d-p)σ, (d-p)π and (d-p)δ covalent coordination interactions exist in La&lt;sub>6&lt;/sub>&amp;[La@B&lt;sub>24&lt;/sub>]&lt;sup>+/0&lt;/sup> (3/4) clusters, while the 1D La&lt;sub>10&lt;/sub>B&lt;sub>32&lt;/sub> (5), 2D La&lt;sub>3&lt;/sub>B&lt;sub>10&lt;/sub> (6), and 3D LaB&lt;sub>6&lt;/sub> (7) crystals exhibit mainly electrostatic interactions between the trivalent La centers and cubic B&lt;sub>24&lt;/sub> frameworks, with weak but discernible coordination contributions from La (5d) ← B (2p) back-donations. The IR and Raman spectra of La&lt;sub>6&lt;/sub>&amp;[La@B&lt;sub>24&lt;/sub>]&lt;sup>+/0&lt;/sup> (3/4) and band structures of La&lt;sub>10&lt;/sub>B&lt;sub>32&lt;/sub> (5) and La&lt;sub>3&lt;/sub>B&lt;sub>10&lt;/sub> (6) are computationally simulated to facilitate their future characterizations.</pubmed_abstract><journal>RSC advances</journal><pubmed_title>Perfect cubic La-doped boron clusters La&lt;sub>6&lt;/sub>&amp;[La@B&lt;sub>24&lt;/sub>]&lt;sup>+/0&lt;/sup> as the embryos of low-dimensional lanthanide boride nanomaterials.</pubmed_title><pmcid>PMC9051253</pmcid><funding_grant_id>11504213</funding_grant_id><funding_grant_id>21720102006</funding_grant_id><funding_grant_id>21803037</funding_grant_id><pubmed_authors>Lu XQ</pubmed_authors><pubmed_authors>Mu YW</pubmed_authors><pubmed_authors>Zan WY</pubmed_authors><pubmed_authors>Ao MZ</pubmed_authors><pubmed_authors>Li SD</pubmed_authors><pubmed_authors>Tian XX</pubmed_authors></additional><is_claimable>false</is_claimable><name>Perfect cubic La-doped boron clusters La&lt;sub>6&lt;/sub>&amp;[La@B&lt;sub>24&lt;/sub>]&lt;sup>+/0&lt;/sup> as the embryos of low-dimensional lanthanide boride nanomaterials.</name><description>La-doped boron nanoclusters have received considerable attention due to their unique structures and bonding. Inspired by recent experimental observations of the inverse sandwich &lt;i>D&lt;/i> &lt;sub>8h&lt;/sub> La&lt;sub>2&lt;/sub>B&lt;sub>8&lt;/sub> (1) and triple-decker &lt;i>C&lt;/i> &lt;sub>2v&lt;/sub> La&lt;sub>3&lt;/sub>B&lt;sub>14&lt;/sub> &lt;sup>-&lt;/sup> (2) and based on extensive global searches and first-principles theory investigations, we present herein the possibility of the perfect cubic La-doped boron clusters &lt;i>O&lt;/i> &lt;sub>h&lt;/sub> La&lt;sub>6&lt;/sub>&amp;[La@B&lt;sub>24&lt;/sub>]&lt;sup>+&lt;/sup> (3, &lt;sup>1&lt;/sup>A&lt;sub>1g&lt;/sub>) and &lt;i>O&lt;/i> &lt;sub>h&lt;/sub> La&lt;sub>6&lt;/sub>&amp;[La@B&lt;sub>24&lt;/sub>] (4, &lt;sup>2&lt;/sup>A&lt;sub>2g&lt;/sub>) which appear to be the embryos of the metallic one-dimensional La&lt;sub>10&lt;/sub>B&lt;sub>32&lt;/sub> (5) nanowire, two-dimensional La&lt;sub>3&lt;/sub>B&lt;sub>10&lt;/sub> (6) nanosheet, and three-dimensional LaB&lt;sub>6&lt;/sub> (7) nanocrystal, facilitating a bottom-up approach to build cubic lanthanide boride nanostructures from gas-phase clusters. Detailed molecular orbital and bonding analyses indicate that effective (d-p)σ, (d-p)π and (d-p)δ covalent coordination interactions exist in La&lt;sub>6&lt;/sub>&amp;[La@B&lt;sub>24&lt;/sub>]&lt;sup>+/0&lt;/sup> (3/4) clusters, while the 1D La&lt;sub>10&lt;/sub>B&lt;sub>32&lt;/sub> (5), 2D La&lt;sub>3&lt;/sub>B&lt;sub>10&lt;/sub> (6), and 3D LaB&lt;sub>6&lt;/sub> (7) crystals exhibit mainly electrostatic interactions between the trivalent La centers and cubic B&lt;sub>24&lt;/sub> frameworks, with weak but discernible coordination contributions from La (5d) ← B (2p) back-donations. The IR and Raman spectra of La&lt;sub>6&lt;/sub>&amp;[La@B&lt;sub>24&lt;/sub>]&lt;sup>+/0&lt;/sup> (3/4) and band structures of La&lt;sub>10&lt;/sub>B&lt;sub>32&lt;/sub> (5) and La&lt;sub>3&lt;/sub>B&lt;sub>10&lt;/sub> (6) are computationally simulated to facilitate their future characterizations.</description><dates><release>2020-01-01T00:00:00Z</release><publication>2020 Mar</publication><modification>2025-04-25T22:58:51.517Z</modification><creation>2025-04-06T09:12:19.418Z</creation></dates><accession>S-EPMC9051253</accession><cross_references><pubmed>35497573</pubmed><doi>10.1039/d0ra01616k</doi></cross_references></HashMap>