2013
DOI: 10.1103/physreva.87.063406
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Quantitative rescattering theory of high-order harmonic generation for polyatomic molecules

Abstract: We report applications of the quantitative rescattering theory (QRS) for calculation of high-order-harmonic generation (HHG) from polyatomic molecules in ultrashort linearly polarized intense laser pulses, using the example of the CCl 4 molecule. In particular, we present a detailed analysis and a treatment for the phase of the electron returning wave packet, which recollides with the parent molecular ion to emit high-energy photons. Our results show that Cooper-type minimum structures in the molecular photoio… Show more

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Cited by 37 publications
(49 citation statements)
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“…For cis-DCE, the ionization yield is stronger when the field direction is closer to θ = 180 • , i.e., pointed away from the C-C center (or the electric force is closer to θ = 0 • , or pointed toward the C-C center). We comment that the angular dependence of the ionization rate looks very similar to that of the asymptotic wave function of the HOMO [21,28]. Overall, our angular dependence resembles the results of Spanner and Patchkovskii [29].…”
supporting
confidence: 75%
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“…For cis-DCE, the ionization yield is stronger when the field direction is closer to θ = 180 • , i.e., pointed away from the C-C center (or the electric force is closer to θ = 0 • , or pointed toward the C-C center). We comment that the angular dependence of the ionization rate looks very similar to that of the asymptotic wave function of the HOMO [21,28]. Overall, our angular dependence resembles the results of Spanner and Patchkovskii [29].…”
supporting
confidence: 75%
“…(2) needs to be averaged over the isotropic molecular distribution [19,21]. A major advantage of this approach over the more standard approach of calculating the electron wave packet directly for the target using the strong-field approximation (SFA) is that it avoids possible spurious spikes, which occur quite frequently for polyatomic targets.…”
mentioning
confidence: 99%
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