(a) Electric field (solid line) used for the exact TDSE and RRA calculations, and kicked field (dashed lines) consisting of seven consecutive kicks used for the IA. (b) Fourier transforms of pulse in frequency domain. , , , , , , and .
The evolution of the degree of orientation for LiH by using the three levels of approximations, where the rotational temperature is .
The final rotational populations calculated by the RRA and the IA for LiH.
The evolution of the degree of orientation for LiCl as a function of laser frequency , where the intensity of electric fields are and , and the other pulse parameters are the same as those in Fig. 1.
The evolutions of the degree of orientation obtained by using the exact TDSE calculation and the RRA for LiCl.
Time-dependent rotational populations of in the vibrational state for LiCl.
The evolutions of the degree of orientation calculated by using the RRA and the IA for LiCl. The letter marks indicate the short instants.
Polar plots of angular distributions at different times marked in Fig. 7 for LiCl.
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