1977
DOI: 10.1063/1.89481
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Photoionization cross sections for excited states of argon and krypton

Abstract: Calculations have been carried out for the photoionization cross sections of excited states of atomic argon and krypton, relevant to the KrF laser. At λ=2486 Å, it is found that photoabsorption due to the 3P0,2 metastable states is relatively unimportant, while the cross sections for the first excited p states are large (∼4.5 ×10−18 cm2).

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Cited by 46 publications
(11 citation statements)
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“…In the circumstances prevailing in this experiment, the photo-ionization rate from the metastable state is negligible [31], and the low gas pressures (0.05 mbar) mean that the collisional rates are negligible in comparison to optical transition rates [16]. In those conditions, the 760 nm LIF is directly proportional to the total metastable population produced by a laser pulse.…”
Section: Apparatus and Proceduresmentioning
confidence: 91%
See 1 more Smart Citation
“…In the circumstances prevailing in this experiment, the photo-ionization rate from the metastable state is negligible [31], and the low gas pressures (0.05 mbar) mean that the collisional rates are negligible in comparison to optical transition rates [16]. In those conditions, the 760 nm LIF is directly proportional to the total metastable population produced by a laser pulse.…”
Section: Apparatus and Proceduresmentioning
confidence: 91%
“…where we note that the photo-ionization cross-section from the 1s 5 state σ mi is less than 3 % of that from the 2p 6 state σ ei [31]. We have thus neglected the former in the calculation as it does not significantly modify the metastable population.…”
Section: Theory and Analysismentioning
confidence: 99%
“…electrons in excited rare-gas atoms with those in the respective alkali atoms has been reproduced in calculations of excited states with = 0[261,262,[326][327][328][329][330]], = 1[261,296,326,[331][332][333], and = 2[261]. In many of these calculations, however, electron correlation, relativistic effects and the open-shell structure of the rare gas ion core were ignored.In a single configuration description, photoionization from the metastable (m+1)s J = 2 level (J + = 3/2 core) and from the (m + 1)s J = 0 level (J + = 1/2) only involve the respective core-conserving "major" transitions, i.e., those leading to the formation of only Rg + ( 2 P 3/2 ) ions from J = 2 and only Rg + ( 2 P 1/2 ) ions from J = 0.Correlation effects in the initial and final states, however, modify this simple picture considerably and result in the observation of the core-changing "minor" transitions.…”
mentioning
confidence: 99%
“…is the rate of 1-photon ionization of excited Kr atoms, σ a ≈4.5x10 −22 m 2 is 1-photon ionization cross section of excited Kr, 33 W Σ = W i is the summarized effect given by Eq. (5) and N Kr−0 = P Kr /k B T is the initial density of Kr.…”
Section: Aip Advances 6 095018 (2016)mentioning
confidence: 99%