2016
DOI: 10.1103/physreva.94.053411
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Wavelength- and alignment-dependent photoionization ofN2andO2

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Cited by 5 publications
(2 citation statements)
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“…The deconvoluted MF ionization probability distributions I(θ) of N 2 are shown in green using q á ¢ñ = cos 0.55 2 (dashed), 0.60 (solid) and 0.65 (dotted). With a 800nm probe and I probe =1.0× 10 14 W cm −2 , the ∼3:1 ratio between parallel to perpendicular alignment is consistent with previous studies and reflects the σ g symmetry of the highest occupied molecular orbital (HOMO) of N 2  [27,[36][37][38]. The small local maximum of ionization featured at θ=90°is real as it was also reported elsewhere at lower intensity (I probe =3.0×10 13 W cm −2 ) via COLTRIMS measurements [39].…”
Section: Strong Field Ionization In Aligned Moleculessupporting
confidence: 89%
“…The deconvoluted MF ionization probability distributions I(θ) of N 2 are shown in green using q á ¢ñ = cos 0.55 2 (dashed), 0.60 (solid) and 0.65 (dotted). With a 800nm probe and I probe =1.0× 10 14 W cm −2 , the ∼3:1 ratio between parallel to perpendicular alignment is consistent with previous studies and reflects the σ g symmetry of the highest occupied molecular orbital (HOMO) of N 2  [27,[36][37][38]. The small local maximum of ionization featured at θ=90°is real as it was also reported elsewhere at lower intensity (I probe =3.0×10 13 W cm −2 ) via COLTRIMS measurements [39].…”
Section: Strong Field Ionization In Aligned Moleculessupporting
confidence: 89%
“…An increase of the HOMO ionization probability for the wavelength change from 500 to 600 nm is also displayed. This irregular behaviour of the HOMO ionization probability will be analyzed in figure 2.The TDSE simulations for the intense-field ionization spectrum of N 2 and O 2 [44] have emphasized an overall decrease of the ionization yields with increasing laser wavelength. Figure 2 displays the time dependence of the laser electric field given by equations ( 11) and (12) in upper panels and the corresponding orbital populations in lower panels, for the three wavelengths for which the HOMO ionization probability presents an irregular behaviour for short laser pulses, as can be seen from figure 1(a).…”
Section: Resultsmentioning
confidence: 94%