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2014
DOI: 10.1364/optica.1.000323
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Metastable electronic states and nonlinear response for high-intensity optical pulses

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Cited by 38 publications
(30 citation statements)
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“…This form of the post-adiabatic correction was shown to work reasonably well in simple model systems [5]. However, given the number of approximations adopted in the above derivations, it is necessary to test this result against numerically exact solutions for the same atom models used to obtain all MESA-related characteristics.…”
Section: B Further Memory-function Approximationsmentioning
confidence: 90%
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“…This form of the post-adiabatic correction was shown to work reasonably well in simple model systems [5]. However, given the number of approximations adopted in the above derivations, it is necessary to test this result against numerically exact solutions for the same atom models used to obtain all MESA-related characteristics.…”
Section: B Further Memory-function Approximationsmentioning
confidence: 90%
“…For completeness, we begin with a recapitulation of the MESA [5]. Consider a Hamiltonian for a single-active-electron model of an atom exposed to a time-dependent electric field F (t) (optical pulse) polarized along x (in atomic units):…”
Section: Stark Resonant State Expansionmentioning
confidence: 99%
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“…The model we test here is the metastable-electronic-state approach (MESA) [13]. This method is sufficiently fast to allow spatially resolved simulation of optical pulses on scales relevant to experiments while, at the same time, drawing from first-principle calculations, it captures both the nonlinear polarization and plasma generation [14].…”
Section: Introductionmentioning
confidence: 99%