V. A. Alekseev, T. A. Vartanyan, A. S. Pazgalev, P. Yu. Serdobintsev
{"title":"含CF4气相混合物光谱中K、Rb和Cs原子向低位2S1/2和2D3/2,5/2激发态的偶极禁止跃迁的卫星","authors":"V. A. Alekseev, T. A. Vartanyan, A. S. Pazgalev, P. Yu. Serdobintsev","doi":"10.1134/S1063776123090029","DOIUrl":null,"url":null,"abstract":"<p>The luminescence excitation spectra of the <i>D</i><sub>1</sub> resonance line of atoms K, Rb, and Cs in gas mixtures with CF<sub>4</sub> are found to contain satellite transitions, which correspond to the transition of an atom to the states (<i>n</i> – 1)<i>d</i> <sup>2</sup><i>D</i><sub>3/2,5/2</sub> and (<i>n</i> + 1)<i>s</i> <sup>2</sup><i>S</i><sub>1/2</sub>, where <i>n</i> = 4, 5, and 6 for K, Rb, and Cs, respectively, with the simultaneous excitation of CF<sub>4</sub> molecule vibrations at the IR active mode frequency ν<sub>3</sub> with a quantum energy of 1283 cm<sup>–1</sup>. These satellite transitions are A(<i>ns</i> <sup>2</sup><i>S</i><sub>1/2</sub>) + CF<sub>4</sub>(ν<sub>3</sub> = 0) + <i>h</i>ν → A((<i>n</i> – 1)<i>d</i> <sup>2</sup><i>D</i><sub>3/2,5/2</sub>) + CF<sub>4</sub>(ν<sub>3</sub> = 1) and A(<i>ns</i> <sup>2</sup><i>S</i><sub>1/2</sub>) + CF<sub>4</sub>(ν<sub>3</sub> = 0) + <i>h</i>ν → A((<i>n</i> + 1)<i>s</i> <sup>2</sup><i>S</i><sub>1/2</sub>) + CF<sub>4</sub>(ν<sub>3</sub> = 1), where A = K, Rb, and Cs. The appearance of an optical coupling between the upper and lower states of these asymptotically (at <span>\\({{R}_{{{\\text{A}} - {\\text{C}}{{{\\text{F}}}_{4}}}}}\\)</span> → ∞) forbidden transitions is shown to be caused by the interaction of the dipole moment of the ν<sub>3</sub> = 1 ↔ ν<sub>3</sub> = 0 vibrational transition in the CF<sub>4</sub> molecule with the dipole moments of the electronic transitions <i>np</i> <sup>2</sup><i>P</i><sub>1/2,3/2</sub> ↔ (<i>n</i> – 1)<i>d</i> <sup>2</sup><i>D</i><sub>3/2,5/2</sub> and <i>np</i> <sup>2</sup><i>P</i><sub>1/2,3/2</sub> ↔ (<i>n</i> + 1)<i>s</i> <sup>2</sup><i>S</i><sub>1/2</sub> in an alkali metal atom; as a result of this interaction, the upper state of the satellite transition acquires admixtures of the A(<i>np</i> <sup>2</sup><i>P</i><sub>1/2,3/2</sub>)CF<sub>4</sub>(ν<sub>3</sub> = 0) resonance states.</p>","PeriodicalId":629,"journal":{"name":"Journal of Experimental and Theoretical Physics","volume":"137 3","pages":"283 - 293"},"PeriodicalIF":1.0000,"publicationDate":"2023-10-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Satellites of the Dipole-Forbidden Transitions to the Low-Lying 2S1/2 and 2D3/2,5/2 Excited States of K, Rb, and Cs Atoms in the Spectra of Gas-Phase Mixtures with CF4\",\"authors\":\"V. A. Alekseev, T. A. Vartanyan, A. S. Pazgalev, P. Yu. Serdobintsev\",\"doi\":\"10.1134/S1063776123090029\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>The luminescence excitation spectra of the <i>D</i><sub>1</sub> resonance line of atoms K, Rb, and Cs in gas mixtures with CF<sub>4</sub> are found to contain satellite transitions, which correspond to the transition of an atom to the states (<i>n</i> – 1)<i>d</i> <sup>2</sup><i>D</i><sub>3/2,5/2</sub> and (<i>n</i> + 1)<i>s</i> <sup>2</sup><i>S</i><sub>1/2</sub>, where <i>n</i> = 4, 5, and 6 for K, Rb, and Cs, respectively, with the simultaneous excitation of CF<sub>4</sub> molecule vibrations at the IR active mode frequency ν<sub>3</sub> with a quantum energy of 1283 cm<sup>–1</sup>. These satellite transitions are A(<i>ns</i> <sup>2</sup><i>S</i><sub>1/2</sub>) + CF<sub>4</sub>(ν<sub>3</sub> = 0) + <i>h</i>ν → A((<i>n</i> – 1)<i>d</i> <sup>2</sup><i>D</i><sub>3/2,5/2</sub>) + CF<sub>4</sub>(ν<sub>3</sub> = 1) and A(<i>ns</i> <sup>2</sup><i>S</i><sub>1/2</sub>) + CF<sub>4</sub>(ν<sub>3</sub> = 0) + <i>h</i>ν → A((<i>n</i> + 1)<i>s</i> <sup>2</sup><i>S</i><sub>1/2</sub>) + CF<sub>4</sub>(ν<sub>3</sub> = 1), where A = K, Rb, and Cs. The appearance of an optical coupling between the upper and lower states of these asymptotically (at <span>\\\\({{R}_{{{\\\\text{A}} - {\\\\text{C}}{{{\\\\text{F}}}_{4}}}}}\\\\)</span> → ∞) forbidden transitions is shown to be caused by the interaction of the dipole moment of the ν<sub>3</sub> = 1 ↔ ν<sub>3</sub> = 0 vibrational transition in the CF<sub>4</sub> molecule with the dipole moments of the electronic transitions <i>np</i> <sup>2</sup><i>P</i><sub>1/2,3/2</sub> ↔ (<i>n</i> – 1)<i>d</i> <sup>2</sup><i>D</i><sub>3/2,5/2</sub> and <i>np</i> <sup>2</sup><i>P</i><sub>1/2,3/2</sub> ↔ (<i>n</i> + 1)<i>s</i> <sup>2</sup><i>S</i><sub>1/2</sub> in an alkali metal atom; as a result of this interaction, the upper state of the satellite transition acquires admixtures of the A(<i>np</i> <sup>2</sup><i>P</i><sub>1/2,3/2</sub>)CF<sub>4</sub>(ν<sub>3</sub> = 0) resonance states.</p>\",\"PeriodicalId\":629,\"journal\":{\"name\":\"Journal of Experimental and Theoretical Physics\",\"volume\":\"137 3\",\"pages\":\"283 - 293\"},\"PeriodicalIF\":1.0000,\"publicationDate\":\"2023-10-26\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Experimental and Theoretical Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://link.springer.com/article/10.1134/S1063776123090029\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Experimental and Theoretical Physics","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1134/S1063776123090029","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
Satellites of the Dipole-Forbidden Transitions to the Low-Lying 2S1/2 and 2D3/2,5/2 Excited States of K, Rb, and Cs Atoms in the Spectra of Gas-Phase Mixtures with CF4
The luminescence excitation spectra of the D1 resonance line of atoms K, Rb, and Cs in gas mixtures with CF4 are found to contain satellite transitions, which correspond to the transition of an atom to the states (n – 1)d2D3/2,5/2 and (n + 1)s2S1/2, where n = 4, 5, and 6 for K, Rb, and Cs, respectively, with the simultaneous excitation of CF4 molecule vibrations at the IR active mode frequency ν3 with a quantum energy of 1283 cm–1. These satellite transitions are A(ns2S1/2) + CF4(ν3 = 0) + hν → A((n – 1)d2D3/2,5/2) + CF4(ν3 = 1) and A(ns2S1/2) + CF4(ν3 = 0) + hν → A((n + 1)s2S1/2) + CF4(ν3 = 1), where A = K, Rb, and Cs. The appearance of an optical coupling between the upper and lower states of these asymptotically (at \({{R}_{{{\text{A}} - {\text{C}}{{{\text{F}}}_{4}}}}}\) → ∞) forbidden transitions is shown to be caused by the interaction of the dipole moment of the ν3 = 1 ↔ ν3 = 0 vibrational transition in the CF4 molecule with the dipole moments of the electronic transitions np2P1/2,3/2 ↔ (n – 1)d2D3/2,5/2 and np2P1/2,3/2 ↔ (n + 1)s2S1/2 in an alkali metal atom; as a result of this interaction, the upper state of the satellite transition acquires admixtures of the A(np2P1/2,3/2)CF4(ν3 = 0) resonance states.
期刊介绍:
Journal of Experimental and Theoretical Physics is one of the most influential physics research journals. Originally based on Russia, this international journal now welcomes manuscripts from all countries in the English or Russian language. It publishes original papers on fundamental theoretical and experimental research in all fields of physics: from solids and liquids to elementary particles and astrophysics.