{"title":"CO2的c1s→nsσg Rydberg激发态中的振动耦合","authors":"Jun-ichi Adachi, Nobuhiro Kosugi, Eiji Shigemasa, Akira Yagishita","doi":"10.1021/jp962025j","DOIUrl":null,"url":null,"abstract":"<p >Fragment ion yields in the C 1s → Rydberg excitation region of CO<sub>2</sub> were measured in the 90° and 0° directions relative to the electric vector of the linearly polarized light. The C 1s → <i>ns</i> (<i>n</i> = 3, 4), <i>n</i>pπ and <i>n</i>pσ (<i>n</i> = 3?7), and <i>n</i>d (<i>n</i> = 3, 4) Rydberg transitions are clearly observed and show some vibrational structures. The dipole-forbidden C 1s(σ<sub>g</sub>) → 3sσ<sub>g</sub> Rydberg transition is the strongest of all the Rydberg transitions, and the ion yield in the 90° direction is dominant. This indicates that the bending vibration is predominantly coupled with the 3sσ<sub>g</sub> Rydberg state and the intensity-lending dipole-allowed state is a very strong π* resonance, only 2 eV lower than the 3sσ<sub>g</sub> state. On the other hand, in the 4sσ<sub>g</sub> Rydberg state the vibronic coupling through the antisymmetric stretching mode is strongly observed in the 0° direction. This is probably because the 4sσ<sub>g</sub> state approaches another intensity-lending state with Σ<sub>u</sub><sup>+</sup> symmetry and goes away from the π* resonance. The angle-resolved ion-yield technique is very powerful for elucidating the vibronic coupling mechanism. </p>","PeriodicalId":58,"journal":{"name":"The Journal of Physical Chemistry ","volume":"100 51","pages":"19783–19788"},"PeriodicalIF":2.7810,"publicationDate":"1996-12-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1021/jp962025j","citationCount":"30","resultStr":"{\"title\":\"Vibronic Couplings in the C 1s → nsσg Rydberg Excited States of CO2\",\"authors\":\"Jun-ichi Adachi, Nobuhiro Kosugi, Eiji Shigemasa, Akira Yagishita\",\"doi\":\"10.1021/jp962025j\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >Fragment ion yields in the C 1s → Rydberg excitation region of CO<sub>2</sub> were measured in the 90° and 0° directions relative to the electric vector of the linearly polarized light. The C 1s → <i>ns</i> (<i>n</i> = 3, 4), <i>n</i>pπ and <i>n</i>pσ (<i>n</i> = 3?7), and <i>n</i>d (<i>n</i> = 3, 4) Rydberg transitions are clearly observed and show some vibrational structures. The dipole-forbidden C 1s(σ<sub>g</sub>) → 3sσ<sub>g</sub> Rydberg transition is the strongest of all the Rydberg transitions, and the ion yield in the 90° direction is dominant. This indicates that the bending vibration is predominantly coupled with the 3sσ<sub>g</sub> Rydberg state and the intensity-lending dipole-allowed state is a very strong π* resonance, only 2 eV lower than the 3sσ<sub>g</sub> state. On the other hand, in the 4sσ<sub>g</sub> Rydberg state the vibronic coupling through the antisymmetric stretching mode is strongly observed in the 0° direction. This is probably because the 4sσ<sub>g</sub> state approaches another intensity-lending state with Σ<sub>u</sub><sup>+</sup> symmetry and goes away from the π* resonance. The angle-resolved ion-yield technique is very powerful for elucidating the vibronic coupling mechanism. </p>\",\"PeriodicalId\":58,\"journal\":{\"name\":\"The Journal of Physical Chemistry \",\"volume\":\"100 51\",\"pages\":\"19783–19788\"},\"PeriodicalIF\":2.7810,\"publicationDate\":\"1996-12-19\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1021/jp962025j\",\"citationCount\":\"30\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The Journal of Physical Chemistry \",\"FirstCategoryId\":\"1\",\"ListUrlMain\":\"https://pubs.acs.org/doi/10.1021/jp962025j\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Journal of Physical Chemistry ","FirstCategoryId":"1","ListUrlMain":"https://pubs.acs.org/doi/10.1021/jp962025j","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Vibronic Couplings in the C 1s → nsσg Rydberg Excited States of CO2
Fragment ion yields in the C 1s → Rydberg excitation region of CO2 were measured in the 90° and 0° directions relative to the electric vector of the linearly polarized light. The C 1s → ns (n = 3, 4), npπ and npσ (n = 3?7), and nd (n = 3, 4) Rydberg transitions are clearly observed and show some vibrational structures. The dipole-forbidden C 1s(σg) → 3sσg Rydberg transition is the strongest of all the Rydberg transitions, and the ion yield in the 90° direction is dominant. This indicates that the bending vibration is predominantly coupled with the 3sσg Rydberg state and the intensity-lending dipole-allowed state is a very strong π* resonance, only 2 eV lower than the 3sσg state. On the other hand, in the 4sσg Rydberg state the vibronic coupling through the antisymmetric stretching mode is strongly observed in the 0° direction. This is probably because the 4sσg state approaches another intensity-lending state with Σu+ symmetry and goes away from the π* resonance. The angle-resolved ion-yield technique is very powerful for elucidating the vibronic coupling mechanism.