A quantum approach and classical molecular dynamics simulations (CMDS) are proposed for the modeling of rotational relaxation and of the nonadiabatic alignment of gaseous linear molecules by a nonresonant laser field under dissipative conditions. They are applied to pure CO2 and compared by looking at state-to-state collisional rates and at the value of ⟨cos2[θz(t)]⟩ induced by a 100 fs laser pulse linearly polarized along |$\vec z$|. The main results are: (i) When properly requantized, the classical model leads to very satisfactory predictions of the permanent and transient alignments under non-dissipative conditions. (ii) The CMDS calculations of collisional-broadening coefficients and rotational state-to-state rates are in very good agreement with those of a quantum model based on the energy corrected sudden (ECS) approximation. (iii) Both approaches show a strong propensity of collisions, while they change the rotational energy (i.e., J), to conserve the angular momentum orientation (i.e., M/J). (iv) Under dissipative conditions, CMDS and quantum-ECS calculations lead to very consistent decays with time of the “permanent” and transient components of the laser-induced alignment. This result, expected from (i) and (ii), is obtained only if a properly J- and M-dependent ECS model is used. Indeed, rotational state-to-state rates and the decay of the “permanent” alignment demonstrate, for pure CO2, the limits of a M-independent collisional model proposed previously. Furthermore, computations show that collisions induce a decay of the “permanent” alignment about twice slower than that of the transient revivals amplitudes, a direct consequence of (iii). (v) The analysis of the effects of reorienting and dephasing elastic collisions shows that the latter have a very small influence but that the former play a non-negligible role in the alignment dynamics. (vi) Rotation-translation collisionally induced transfers have also been studied, demonstrating that they only slightly change the alignment dissipation for the considered laser energy conditions.
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14 May 2012
Research Article|
May 09 2012
Quantum and classical approaches for rotational relaxation and nonresonant laser alignment of linear molecules: A comparison for CO2 gas in the nonadiabatic regime
J.-M. Hartmann;
J.-M. Hartmann
a)
1Laboratoire Interuniversitaire des Systèmes Atmosphériques (LISA) CNRS (UMR 7583), Université Paris Est Créteil, Université Paris Diderot,
Institut Pierre-Simon Laplace, Université Paris Est Créteil
, 94010 Créteil Cedex, France
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C. Boulet
C. Boulet
2Institut des Sciences Moléculaires d’Orsay (ISMO) CNRS (UMR 8214),
Université Paris-Sud
, Bât. 350, Orsay F-91405, France
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a)
Author to whom correspondence should be addressed. Electronic mail: jean-michel.hartmann@lisa.u-pec.fr. Tel.: 33 (0)145176542. FAX: 33 (0)145171564.
J. Chem. Phys. 136, 184302 (2012)
Article history
Received:
January 09 2012
Accepted:
April 06 2012
Citation
J.-M. Hartmann, C. Boulet; Quantum and classical approaches for rotational relaxation and nonresonant laser alignment of linear molecules: A comparison for CO2 gas in the nonadiabatic regime. J. Chem. Phys. 14 May 2012; 136 (18): 184302. https://doi.org/10.1063/1.4705264
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