2005
DOI: 10.1103/physreva.72.023420
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Dynamics of laser-induced molecular alignment in the impulsive and adiabatic regimes: A direct comparison

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Cited by 110 publications
(114 citation statements)
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“…2(d) and Fig. 2(e) show histograms of the FT of the calculation and the experimental data respectively, the peak positions corresponding to the dominant beat frequencies between [19] for an initially randomly aligned ensemble of room temperature D2 molecules. For a particular ∆t and θ, the false colour-scale indicates the wavepacket probability with a thermal average.…”
mentioning
confidence: 99%
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“…2(d) and Fig. 2(e) show histograms of the FT of the calculation and the experimental data respectively, the peak positions corresponding to the dominant beat frequencies between [19] for an initially randomly aligned ensemble of room temperature D2 molecules. For a particular ∆t and θ, the false colour-scale indicates the wavepacket probability with a thermal average.…”
mentioning
confidence: 99%
“…In the present work, the spatio-temporal evolution of the D 2 rotational wavepacket has been simulated following the procedure described in [19]. Briefly, a thermal ensemble of rigid rotors is considered, each of which gives rise to a superposition of rotational states, |Ψ Ji Mi = J≥|Mi| F JiJ (t)|JM i in which F JiJ (t ) are the timedependent complex coefficients (note that M i is conserved in a linearly polarized field).…”
mentioning
confidence: 99%
“…In a simple model, we may assume that it occurs when the internuclear separation of the expanding nuclear wavepacket passes through a value that matches the returning electron wavelength at that time. We therefore define a simple condition for suppression of harmonic emission in this dynamic system as 2R(t)cos(θ m ) = λ(t), where θ m is the modal value of the alignment distribution σ(θ) at the peak of the pulse, calculated by the method detailed in [20]. Here sech^2 pulses of FWHM 30 fs and peak intensities 3.0 x 10 14 Wcm -2 and 2.2 x 10 14 Wcm -2 are used to calculate the evolution of σ(θ) under the pulse envelope.…”
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confidence: 99%
“…This typically happens through collisions with other molecules and can be avoided by maintaining a low molecular density in the laser-molecule interaction region. Like in the case of adiabatic alignment, increasing degrees of impulsive alignment are achieved with increasing molecular polarisability and decreasing rotational temperature of the molecular ensemble [207]. However, in the impulsive regime the degree of rotational excitation solely depends on the total energy deposited in the molecular system.…”
Section: Impulsive Alignmentmentioning
confidence: 99%
“…In the impulsive regime, the laser pulse duration is much shorter than the characteristic rotational period of the molecule [207]. Here, the laser pulse coherently couples the rotational states of the molecule and thus creates a rotational wavepacket that is initially aligned along the laser pulse polarisation.…”
Section: Impulsive Alignmentmentioning
confidence: 99%