TY - JOUR
T1 - Three-dimensional alignment of asymmetric-top molecules induced by polarization-shaped optimal laser pulses
AU - Yoshida, Masataka
AU - Takemoto, Norio
AU - Ohtsuki, Yukiyoshi
N1 - Funding Information:
One of the authors (Y.O.) acknowledges support from a Grant-in-Aid for Scientific Research (C) (Grant No. 15K05373) and partly from the Joint Usage/Research Program on Zero-Emission Energy Research, Institute of Advanced Energy, Kyoto University (Grant No. ZE30B-16). This work was also partly supported by a Grant-in-Aid for JSPS Fellows (Grant No. 17J02010). N.T. acknowledges support from the Israel Science Foundation (Grant No. 1094/16) and the German-Israeli Foundation for Scientific Research and Development (GIF) for the main part of the work at Department of Chemical Physics, Weizmann Institute of Science. N.T. further acknowledges the Chemical Sciences, Geosciences, and Biosciences Division, Office of Basic Energy Sciences, Office of Science, U.S. Department of Energy, under Award No. DE-FG02-86ER13491 for support during the preparation of the manuscript.
Publisher Copyright:
© 2018 American Physical Society.
PY - 2018/11/26
Y1 - 2018/11/26
N2 - Optimal control simulation is applied to numerically design nonresonant laser pulses that maximize the degrees of three-dimensional (3D) alignment of SO2 using the lowest-order induced-dipole interaction. In our trials, combinations of more than two mutually orthogonal, linearly polarized subpulses are always obtained as the optimal solutions. Each subpulse in the optimal pulses impulsively excites the rotational wave packet. The optimal pulses effectively cooperate with the rotational dynamics up to only a few partial revival timings owing to the rotational dephasing that determines the effective control periods. The control mechanisms are interpreted in terms of the time derivatives of the expectation values of the squares of the direction cosines, that of the rotational energy, and the interplay between them. We find a special and important role of the last subpulses as they align the molecular axes using the interaction through the two smallest polarizability components, while the other subpulses excite the rotational wave packet mainly through the largest polarizability component. The control pulses composed of the specified number of subpulses are also numerically optimized by actively utilizing the instantaneous penalty to systematically show the superiority of the use of more than two subpulses over that of two subpulses, the latter of which leads to the saturation of the degree of 3D alignment as a function of total fluence.
AB - Optimal control simulation is applied to numerically design nonresonant laser pulses that maximize the degrees of three-dimensional (3D) alignment of SO2 using the lowest-order induced-dipole interaction. In our trials, combinations of more than two mutually orthogonal, linearly polarized subpulses are always obtained as the optimal solutions. Each subpulse in the optimal pulses impulsively excites the rotational wave packet. The optimal pulses effectively cooperate with the rotational dynamics up to only a few partial revival timings owing to the rotational dephasing that determines the effective control periods. The control mechanisms are interpreted in terms of the time derivatives of the expectation values of the squares of the direction cosines, that of the rotational energy, and the interplay between them. We find a special and important role of the last subpulses as they align the molecular axes using the interaction through the two smallest polarizability components, while the other subpulses excite the rotational wave packet mainly through the largest polarizability component. The control pulses composed of the specified number of subpulses are also numerically optimized by actively utilizing the instantaneous penalty to systematically show the superiority of the use of more than two subpulses over that of two subpulses, the latter of which leads to the saturation of the degree of 3D alignment as a function of total fluence.
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U2 - 10.1103/PhysRevA.98.053434
DO - 10.1103/PhysRevA.98.053434
M3 - Article
AN - SCOPUS:85057543174
SN - 2469-9926
VL - 98
JO - Physical Review A
JF - Physical Review A
IS - 5
M1 - 053434
ER -