A new quantum optimal control formalism for stroboscopic steady states and limit cycles in dissipative systems, implemented in Spinach with GRAPE-like scaling and distinct from Floquet-Lindblad approaches.
G.; Chen, Z.; Weiner, J
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Asymmetry in bichromatic fields produces additional nonlinear error-signal frequency shifts in CPT spectroscopy at phase-jump modulation under unisotropic relaxation, while conventional harmonic modulation yields more linear shifts in the high-frequency regime for non-short integration times.
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Quantum optimal control of steady orbits
A new quantum optimal control formalism for stroboscopic steady states and limit cycles in dissipative systems, implemented in Spinach with GRAPE-like scaling and distinct from Floquet-Lindblad approaches.
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Analysis of the frequency shift in coherent population trapping resonance's dynamic continuous-wave spectroscopy at the phase-jump modulation and its comparison with the conventional approach
Asymmetry in bichromatic fields produces additional nonlinear error-signal frequency shifts in CPT spectroscopy at phase-jump modulation under unisotropic relaxation, while conventional harmonic modulation yields more linear shifts in the high-frequency regime for non-short integration times.