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Springer eBooks

Spectroscopy of highly excited S and D states of potassium by two photon absorption

M. D. Levenson, C. D. Harper, G. L. Eesley

Published Apr 6, 2008• 0 citations
Publisher
DOI
10.1007/3-540-07411-2_298

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Highly excited S and D states of potassium were studied by two-photon absorption using a tuneable dye laser and fluorescence detection. Measurements were made of the term values, relative fluorescence signal levels, and fluorescence decay profiles. Using matrix elements determined from quantum defect wave functions, theoretical two-photon absorption cross sections were calculated.

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Three-photon absorption spectroscopy allows determination of the $\mathrm{nf}^{2}F_{\frac{5}{2},\frac{7}{2}}^{0}$ energy levels of alkali metals ($\ensuremath{\Delta}L=+3$). The $3d^{2}D_{\frac{3}{2},\frac{5}{2}}$ levels of KI were selectively excited using a narrow-band dye laser. The $3d^{2}D_{\frac{3}{2},\frac{5}{2}}\ensuremath{\rightarrow}\mathrm{nf}^{2}F_{\frac{5}{2},\frac{7}{2}}^{0}$ absorption lines were observed in the background spectrum of another dye laser, and the $\mathrm{nf}^{2}F_{\frac{5}{2},\frac{7}{2}}^{0}$ energy levels were deduced, from $n=10$ to $n=14$ inclusive, with an accuracy better than 0.1 ${\mathrm{cm}}^{\ensuremath{-}1}$. Previously, an experiment was performed for the $7f^{2}F_{\frac{5}{2},\frac{7}{2}}^{0}$ levels in order to verify the method. Shifts and systematic errors were entirely negligible. For all lines, the relative intensities of the absorbed doublet peaks are in good agreement with the estimates of the $4s^{2}S_{\frac{1}{2}}\ensuremath{\rightarrow}3d^{2}D_{\frac{3}{2},\frac{5}{2}}$ probabilities.

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Three-photon absorption spectroscopy allows determination of the nf2F52,720\mathrm{nf}^{2}F_{\frac{5}{2},\frac{7}{2}}^{0}nf2F25​,27​0​ energy levels of alkali metals ($\ensuremath{\Delta}L=+3$). The 3d2D32,523d^{2}D_{\frac{3}{2},\frac{5}{2}}3d2D23​,25​​ levels of KI were selectively excited using a narrow-band dye laser. The $3d^{2}D_{\frac{3}{2},\frac{5}{2}}\ensuremath{\rightarrow}\mathrm{nf}^{2}F_{\frac{5}{2},\frac{7}{2}}^{0}$ absorption lines were observed in the background spectrum of another dye laser, and the nf2F52,720\mathrm{nf}^{2}F_{\frac{5}{2},\frac{7}{2}}^{0}nf2F25​,27​0​ energy levels were deduced, from n=10n=10n=10 to n=14n=14n=14 inclusive, with an accuracy better than 0.1 ${\mathrm{cm}}^{\ensuremath{-}1}$. Previously, an experiment was performed for the 7f2F52,7207f^{2}F_{\frac{5}{2},\frac{7}{2}}^{0}7f2F25​,27​0​ levels in order to verify the method. Shifts and systematic errors were entirely negligible. For all lines, the relative intensities of the absorbed doublet peaks are in good agreement with the estimates of the $4s^{2}S_{\frac{1}{2}}\ensuremath{\rightarrow}3d^{2}D_{\frac{3}{2},\frac{5}{2}}$ probabilities.