THE $4f-\Lambda^{2}\Sigma^{+}$ (1,1) BAND OF NO USING OPTICAL-OPTICAL DOUBLE RESONANCE MULTIPHOTON IONIZATION TECHNIQUE
dc.creator | Cheung, W. Y. | en_US |
dc.creator | Chupka, W. A. | en_US |
dc.creator | Colson, S. D. | en_US |
dc.creator | Gauyacq, D. | en_US |
dc.creator | Avouris, Ph. | en_US |
dc.creator | Wynne, J. J. | en_US |
dc.date.accessioned | 2007-08-31T14:10:43Z | |
dc.date.available | 2007-08-31T14:10:43Z | |
dc.date.issued | 1982 | en_US |
dc.identifier | 1982-FB-2 | en_US |
dc.identifier.uri | http://hdl.handle.net/1811/29128 | |
dc.description.abstract | The $4f-A^{2}\Sigma^{+} (3\delta\sigma)$ (1,1) band of $^{14}N^{16}O$ has been observed by the technique of optical-optical double resonance multiphoton ionization (OODR-MPI). Results confirm the pure case (d) nature of the $4f \upsilon=1$ level reported by previous workers. Analysis of our results yields values of $B_{\upsilon=1}=1.968 cm^{-1}$ and $\alpha_{c} = 0.020 cm^{-1}$ for the 4f state. Our observation of this transition suggests the presence of a significant amount of d character in the lowest member of the ns series, $(3\delta\sigma)\Lambda^{2}\Sigma^{+}$ state, of the NO molecule. Further theoretical and experimental work are necessary to access the importance of this d character in its contribution towards the intensity of this band. | en_US |
dc.format.extent | 74280 bytes | |
dc.format.mimetype | image/jpeg | |
dc.language.iso | English | en_US |
dc.publisher | Ohio State University | en_US |
dc.title | THE $4f-\Lambda^{2}\Sigma^{+}$ (1,1) BAND OF NO USING OPTICAL-OPTICAL DOUBLE RESONANCE MULTIPHOTON IONIZATION TECHNIQUE | en_US |
dc.type | article | en_US |
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