{"title":"没有电离的成键。","authors":"E. N. Maslen, B. Etschmann","doi":"10.1071/PH99027","DOIUrl":null,"url":null,"abstract":"Charges are calculated for diatomic molecules by partitioning the promolecular density with projection operators derived from free atom potentials. The promolecular charges thus obtained have physically reasonable magnitudes, which are moderately sensitive to interatomic distances and thus to bond type. Their signs are negative for cations and positive for anions. Trends in these charges correlate with subshell structure. Due to the long range of their electrostatic potentials, the cations compete successfully for electrons at the expense of the anions in the density partitioning. This implies that the cation states become overfilled when the atoms overlap, favouring a flow of electrons away from the cation towards the vacant anion states. That accounts for the positive cations and negative anions observed when molecular densities are partitioned with projection operators based on free atom electron densities.","PeriodicalId":170873,"journal":{"name":"Australian Journal of Physics","volume":"37 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2000-04-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"5","resultStr":"{\"title\":\"Bonding without ionisation.\",\"authors\":\"E. N. Maslen, B. Etschmann\",\"doi\":\"10.1071/PH99027\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Charges are calculated for diatomic molecules by partitioning the promolecular density with projection operators derived from free atom potentials. The promolecular charges thus obtained have physically reasonable magnitudes, which are moderately sensitive to interatomic distances and thus to bond type. Their signs are negative for cations and positive for anions. Trends in these charges correlate with subshell structure. Due to the long range of their electrostatic potentials, the cations compete successfully for electrons at the expense of the anions in the density partitioning. This implies that the cation states become overfilled when the atoms overlap, favouring a flow of electrons away from the cation towards the vacant anion states. That accounts for the positive cations and negative anions observed when molecular densities are partitioned with projection operators based on free atom electron densities.\",\"PeriodicalId\":170873,\"journal\":{\"name\":\"Australian Journal of Physics\",\"volume\":\"37 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2000-04-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"5\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Australian Journal of Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1071/PH99027\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Australian Journal of Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1071/PH99027","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Charges are calculated for diatomic molecules by partitioning the promolecular density with projection operators derived from free atom potentials. The promolecular charges thus obtained have physically reasonable magnitudes, which are moderately sensitive to interatomic distances and thus to bond type. Their signs are negative for cations and positive for anions. Trends in these charges correlate with subshell structure. Due to the long range of their electrostatic potentials, the cations compete successfully for electrons at the expense of the anions in the density partitioning. This implies that the cation states become overfilled when the atoms overlap, favouring a flow of electrons away from the cation towards the vacant anion states. That accounts for the positive cations and negative anions observed when molecular densities are partitioned with projection operators based on free atom electron densities.