ABSTRACT
Optimal control theory in the Liouville space is used to perform rovibrational control by means of a laser pulse in a polyad of acetylene in order to populate a dark vibrational state. The initial mixed state is a truncated Boltzmann distribution of rotational levels from J=27 to J=31 of the ground vibrational state. The target state is a rotational equidistribution of levels ranging from J=28 to J=32 of the first excited vibrational dark state including quanta of energy in each bending modes, with positive vibrational angular momenta. The simulation is performed by using a manifold of eigenstates of a full-dimensional Hamiltonian calibrated by high precision spectroscopy known as the global acetylene Hamiltonian [B. Amyay et al., J. Chem. Phys. 131, 114301 (2009)]. The control is successful as an Uhlmann's fidelity of 0.98 is reached.
GRAPHICAL ABSTRACT
![](/cms/asset/1cca4fb9-a3bd-4bc2-89ff-dddd6e6b8159/tmph_a_1469797_uf0001_c.jpg)
Acknowledgements
L.S. is grateful to M. Godefroid for helpful suggestions and S. Gorza for helpful discussions. We also thank the COST XLIC and MOLIM actions. This work has been performed within the French GDR 3575 THEMS.
Disclosure statement
No potential conflict of interest was reported by the authors.
ORCID
L. Santos http://orcid.org/0000-0003-2484-9503
M. Desouter-Lecomte http://orcid.org/0000-0002-6199-7401
N. Vaeck http://orcid.org/0000-0003-0590-9646