{"title":"化学位移张量作为硫键探针:碲二唑- xcn−(X = O, S, Se)盐共晶的固态核磁共振研究","authors":"Carina Almario, Tamali Nag, David L. Bryce","doi":"10.1139/facets-2023-0082","DOIUrl":null,"url":null,"abstract":"We report experimental 125 Te magic-angle spinning solid-state nuclear magnetic resonance (MAS NMR) measurements of the tellurium chemical shift (CS) tensors in three [K(18-crown-6)] + 3,4-dicyano-1,2,5-telluradiazole-XCN − (X = O, S, Se) salt cocrystals featuring chalcogen bonds. These data are compared to those for pure 3,4-dicyano-1,2,5-telluradiazole (1). A reduction in the span of the 125 Te CS tensor is consistently noted in the salt cocrystals compared to pure 1. Isotopically 15 N-labelled [K(18-crown-6)] + [1-OC 15 N] − , which features a chalcogen bond between Te and the cyanate nitrogen atom, is synthesized using KOC 15 N, and the nitrogen CS tensors are measured for both samples via 15 N slow MAS NMR spectroscopy. Possible dynamic disorder of the cyanate ions in KOCN is ruled out. Two crystallographically distinct nitrogen sites are resolved for the salt cocrystal. Upon formation of [K(18-crown-6)] + [1-OC 15 N] − , the 15 N isotropic CS and CS tensor span both decrease relative to the values for pure KOC 15 N, and the axial symmetry of this tensor is lost. These findings are supplemented with a series of density functional theory calculations of magnetic shielding tensors using cluster models or periodic boundary conditions. Inclusion of spin–orbit relativistic effects in the calculation of tellurium shielding tensors is particularly important in achieving agreement with experiment.","PeriodicalId":48511,"journal":{"name":"Facets","volume":"78 1","pages":"0"},"PeriodicalIF":2.9000,"publicationDate":"2023-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Chemical shift tensors as probes of chalcogen bonds: solid-state NMR study of telluradiazole-XCN<sup>−</sup> (X = O, S, Se) salt cocrystals\",\"authors\":\"Carina Almario, Tamali Nag, David L. Bryce\",\"doi\":\"10.1139/facets-2023-0082\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We report experimental 125 Te magic-angle spinning solid-state nuclear magnetic resonance (MAS NMR) measurements of the tellurium chemical shift (CS) tensors in three [K(18-crown-6)] + 3,4-dicyano-1,2,5-telluradiazole-XCN − (X = O, S, Se) salt cocrystals featuring chalcogen bonds. These data are compared to those for pure 3,4-dicyano-1,2,5-telluradiazole (1). A reduction in the span of the 125 Te CS tensor is consistently noted in the salt cocrystals compared to pure 1. Isotopically 15 N-labelled [K(18-crown-6)] + [1-OC 15 N] − , which features a chalcogen bond between Te and the cyanate nitrogen atom, is synthesized using KOC 15 N, and the nitrogen CS tensors are measured for both samples via 15 N slow MAS NMR spectroscopy. Possible dynamic disorder of the cyanate ions in KOCN is ruled out. Two crystallographically distinct nitrogen sites are resolved for the salt cocrystal. Upon formation of [K(18-crown-6)] + [1-OC 15 N] − , the 15 N isotropic CS and CS tensor span both decrease relative to the values for pure KOC 15 N, and the axial symmetry of this tensor is lost. These findings are supplemented with a series of density functional theory calculations of magnetic shielding tensors using cluster models or periodic boundary conditions. Inclusion of spin–orbit relativistic effects in the calculation of tellurium shielding tensors is particularly important in achieving agreement with experiment.\",\"PeriodicalId\":48511,\"journal\":{\"name\":\"Facets\",\"volume\":\"78 1\",\"pages\":\"0\"},\"PeriodicalIF\":2.9000,\"publicationDate\":\"2023-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Facets\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1139/facets-2023-0082\",\"RegionNum\":3,\"RegionCategory\":\"综合性期刊\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"MULTIDISCIPLINARY SCIENCES\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Facets","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1139/facets-2023-0082","RegionNum":3,"RegionCategory":"综合性期刊","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MULTIDISCIPLINARY SCIENCES","Score":null,"Total":0}
Chemical shift tensors as probes of chalcogen bonds: solid-state NMR study of telluradiazole-XCN− (X = O, S, Se) salt cocrystals
We report experimental 125 Te magic-angle spinning solid-state nuclear magnetic resonance (MAS NMR) measurements of the tellurium chemical shift (CS) tensors in three [K(18-crown-6)] + 3,4-dicyano-1,2,5-telluradiazole-XCN − (X = O, S, Se) salt cocrystals featuring chalcogen bonds. These data are compared to those for pure 3,4-dicyano-1,2,5-telluradiazole (1). A reduction in the span of the 125 Te CS tensor is consistently noted in the salt cocrystals compared to pure 1. Isotopically 15 N-labelled [K(18-crown-6)] + [1-OC 15 N] − , which features a chalcogen bond between Te and the cyanate nitrogen atom, is synthesized using KOC 15 N, and the nitrogen CS tensors are measured for both samples via 15 N slow MAS NMR spectroscopy. Possible dynamic disorder of the cyanate ions in KOCN is ruled out. Two crystallographically distinct nitrogen sites are resolved for the salt cocrystal. Upon formation of [K(18-crown-6)] + [1-OC 15 N] − , the 15 N isotropic CS and CS tensor span both decrease relative to the values for pure KOC 15 N, and the axial symmetry of this tensor is lost. These findings are supplemented with a series of density functional theory calculations of magnetic shielding tensors using cluster models or periodic boundary conditions. Inclusion of spin–orbit relativistic effects in the calculation of tellurium shielding tensors is particularly important in achieving agreement with experiment.