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Physical Review A

Absolute photoionization cross sections of the Cs 7 D3/2 level measured by use of fluorescence reduction

Keith Bonin, M. Gatzke, Charles L. Collins, Michael A. Kadar-Kallen

Published Jun 1, 1989• 19 citations
Publisher

Abstract

A simple technique for measuring absolute photoionization cross sections \ensuremath{\sigma} of excited atoms has been applied to the 7${D}_{3/2}$ level in Cs. Past experiments on excited-state cross sections have relied on measurements of the total number of ions or photoelectrons produced by photoionization to deduce \ensuremath{\sigma}. Our technique is novel in that it utilizes the simple measurement of the reduction in the excited-atom fluorescence due to photoionization to find \ensuremath{\sigma}. We report measurements of cross sections at six different photon energies.

DOI
10.1103/physreva.39.5624

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A simple technique for measuring absolute photoionization cross sections \ensuremath{\sigma} of excited atoms has been applied to the 7D3/2{D}_{3/2}D3/2​ level in Cs. Past experiments on excited-state cross sections have relied on measurements of the total number of ions or photoelectrons produced by photoionization to deduce \ensuremath{\sigma}. Our technique is novel in that it utilizes the simple measurement of the reduction in the excited-atom fluorescence due to photoionization to find \ensuremath{\sigma}. We report measurements of cross sections at six different photon energies.
We report the first measurement of the absolute cross section for photoionization of the 7S7S7S state of cesium. The measurement employed a new technique in which the density of the excited-state atoms was determined by the amount of fluorescence. The cross section for photoionization by 540-nm light is 1.14(10)\ifmmode\times\else\texttimes\fi{}${10}^{\ensuremath{-}19}$ cm2{\mathrm{cm}}^{2}cm2. We also propose a second new technique for the absolute measurement of photoionization cross sections which is based on modulated fluorescence.
An atom trapping technique for determining absolute, total ionization cross sections (TICS) out of an excited atom is presented. The unique feature of our method is in utilizing Doppler cooling of neutral atoms to determine ionization cross sections. This fluorescence-monitoring experiment, which is a variant of the ``trap loss'' technique, has enabled us to obtain the experimental electron impact ionization cross sections out of the Cs 62P3∕26\phantom{\rule{0.2em}{0ex}}^{2}{P}_{3∕2}62P3∕2​ state between 7eV7\phantom{\rule{0.3em}{0ex}}\mathrm{eV}7eV and 400eV400\phantom{\rule{0.3em}{0ex}}\mathrm{eV}400eV. CCC, RMPS, and Born theoretical results are also presented for both the ground and excited states of cesium and rubidium. In the low energy region (<11eV)(<11\phantom{\rule{0.3em}{0ex}}\mathrm{eV})(<11eV) where best agreement between these excited state measurements and theory might be expected, a discrepancy of approximately a factor of five is observed. Above this energy there are significant contributions to the TICS from both autoionization and multiple ionization.
An atom trapping technique for determining absolute, total ionization cross sections (TICS) out of an excited atom is presented. The unique feature of our method is in utilizing Doppler cooling of neutral atoms to determine ionization cross sections. This fluorescence-monitoring experiment, which is a variant of the “trap loss” technique, has enabled us to obtain the experimental electron impact ionization cross sections out of the Cs 6 2P3∕2 state between 7 eV and 400 eV. CCC, RMPS, and Born theoretical results are also presented for both the ground and excited states of cesium and rubidium. In the low energy region (<11 eV) where best agreement between these excited state measurements and theory might be expected, a discrepancy of approximately a factor of five is observed. Above this energy there are significant contributions to the TICS from both autoionization and multiple ionization.
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We describe a new technique for accurate measurement of absolute photoionization cross sections. By measuring the loss rateof atoms from a laser trap in the presence of ionizing light, we directly measure the photoionization rate. The only quantities requiring absolute calibration are the ionizing laser intensity and the fractional population in the relevant state. Our technique is capable of detecting extremely small ionization rates, which means that low-power cw sources can be used. We have applied this method to photoionization from the 5P(3/2) state of rubidium at wavelengths of 413 and 407 nm.The cross sections are 1.36(12) x 10(-17) and 1.25(11) x 10(-17) cm(2) , respectively.
We report the measurement of the absolute photoionization cross section for the 6P3/2{6P}_{3/2}6P3/2​ state of cesium. Cross sections were determined by measuring the photoionization rate of cesium atoms confined in a magneto-optical trap. The photoionization rate was measured by monitoring the decay of trap fluorescence during exposure to ionizing laser radiation. The measurements were made in the wavelength range 457.9 to 501.7 nm using several lines from an Ar-ion laser. Our results are compared to other experimental measurements as well as to existing theories.