<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Cui S</submitter><funding>Natural Science Foundation of Tianjin City</funding><funding>National Natural Science Foundation of China</funding><funding>Natural Science Foundation of Tianjin</funding><pagination>e2204755</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC9896038</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>10(4)</volume><pubmed_abstract>Oxychalcogenides capable of exhibiting excellent balance among large second-harmonic generation (SHG) response, wide band gap (E&lt;sub>g&lt;/sub> ), and suitable birefringence (Δn) are ideal materials class for infrared nonlinear optical (IR NLO) crystals. However, rationally designing a new high-performance oxychalcogenide IR NLO crystal still faces a huge challenge because it requires the optimal orientations of the heteroanionic groups in oxychalcogenide. Herein, a series of antiperovskite-type oxychalcogenides, Ae&lt;sub>3&lt;/sub> Q[GeOQ&lt;sub>3&lt;/sub> ] (Ae = Ba, Sr; Q = S, Se), which were synthesized by employing the antiperovskite-type Ba&lt;sub>3&lt;/sub> S[GeS&lt;sub>4&lt;/sub> ] as the structure template. Their structures feature novel three-dimensinoal frameworks constructed by distorted [QAe&lt;sub>6&lt;/sub> ] octahedra, which are further filled by [GeOQ&lt;sub>3&lt;/sub> ] tetrahedra to form antiperovskite-type structures. Based on the unique antiperovskite-type structures, the favorable alignment of the polarizable [GeOQ&lt;sub>3&lt;/sub> ] tetrahedra and distorted [QAe&lt;sub>6&lt;/sub> ] octahedra have been achieved. These contribute the ideal combination of large SHG response (0.7-1.5 times that of AgGaS&lt;sub>2&lt;/sub> ), wide E&lt;sub>g&lt;/sub> (3.52-4.10 eV), and appropriate Δn (0.017-0.035) in Ae&lt;sub>3&lt;/sub> Q[GeOQ&lt;sub>3&lt;/sub> ]. Theoretical calculations and crystal structure analyses revealed that the strong SHG and wide E&lt;sub>g&lt;/sub> could be attributed to the polarizable [GeOQ&lt;sub>3&lt;/sub> ] tetrahedra and distorted [QAe&lt;sub>6&lt;/sub> ] octahedra. This research provides a new exemplification for the design of high-performance IR NLO materials.</pubmed_abstract><journal>Advanced science (Weinheim, Baden-Wurttemberg, Germany)</journal><pubmed_title>The Antiperovskite-Type Oxychalcogenides Ae&lt;sub>3&lt;/sub> Q[GeOQ&lt;sub>3&lt;/sub> ] (Ae = Ba, Sr; Q = S, Se) with Large Second Harmonic Generation Responses and Wide Band Gaps.</pubmed_title><pmcid>PMC9896038</pmcid><funding_grant_id>22071179</funding_grant_id><funding_grant_id>51972230</funding_grant_id><funding_grant_id>52172006</funding_grant_id><funding_grant_id>51890864</funding_grant_id><funding_grant_id>51890865</funding_grant_id><funding_grant_id>20JCJQJC00060</funding_grant_id><funding_grant_id>21JCJQJC00090</funding_grant_id><pubmed_authors>Hu Z</pubmed_authors><pubmed_authors>Cui S</pubmed_authors><pubmed_authors>Wang J</pubmed_authors><pubmed_authors>Wu Y</pubmed_authors><pubmed_authors>Yu H</pubmed_authors><pubmed_authors>Wu H</pubmed_authors></additional><is_claimable>false</is_claimable><name>The Antiperovskite-Type Oxychalcogenides Ae&lt;sub>3&lt;/sub> Q[GeOQ&lt;sub>3&lt;/sub> ] (Ae = Ba, Sr; Q = S, Se) with Large Second Harmonic Generation Responses and Wide Band Gaps.</name><description>Oxychalcogenides capable of exhibiting excellent balance among large second-harmonic generation (SHG) response, wide band gap (E&lt;sub>g&lt;/sub> ), and suitable birefringence (Δn) are ideal materials class for infrared nonlinear optical (IR NLO) crystals. However, rationally designing a new high-performance oxychalcogenide IR NLO crystal still faces a huge challenge because it requires the optimal orientations of the heteroanionic groups in oxychalcogenide. Herein, a series of antiperovskite-type oxychalcogenides, Ae&lt;sub>3&lt;/sub> Q[GeOQ&lt;sub>3&lt;/sub> ] (Ae = Ba, Sr; Q = S, Se), which were synthesized by employing the antiperovskite-type Ba&lt;sub>3&lt;/sub> S[GeS&lt;sub>4&lt;/sub> ] as the structure template. Their structures feature novel three-dimensinoal frameworks constructed by distorted [QAe&lt;sub>6&lt;/sub> ] octahedra, which are further filled by [GeOQ&lt;sub>3&lt;/sub> ] tetrahedra to form antiperovskite-type structures. Based on the unique antiperovskite-type structures, the favorable alignment of the polarizable [GeOQ&lt;sub>3&lt;/sub> ] tetrahedra and distorted [QAe&lt;sub>6&lt;/sub> ] octahedra have been achieved. These contribute the ideal combination of large SHG response (0.7-1.5 times that of AgGaS&lt;sub>2&lt;/sub> ), wide E&lt;sub>g&lt;/sub> (3.52-4.10 eV), and appropriate Δn (0.017-0.035) in Ae&lt;sub>3&lt;/sub> Q[GeOQ&lt;sub>3&lt;/sub> ]. Theoretical calculations and crystal structure analyses revealed that the strong SHG and wide E&lt;sub>g&lt;/sub> could be attributed to the polarizable [GeOQ&lt;sub>3&lt;/sub> ] tetrahedra and distorted [QAe&lt;sub>6&lt;/sub> ] octahedra. This research provides a new exemplification for the design of high-performance IR NLO materials.</description><dates><release>2023-01-01T00:00:00Z</release><publication>2023 Feb</publication><modification>2026-03-27T16:48:23.168Z</modification><creation>2025-04-05T17:07:26.708Z</creation></dates><accession>S-EPMC9896038</accession><cross_references><pubmed>36470657</pubmed><doi>10.1002/advs.202204755</doi></cross_references></HashMap>