Fig. 2: Schematic illustrating the impact of FFM on Rydberg anti-blockade dynamics and the transition dynamics of the four ground states.
From: Quantum computation via Floquet tailored Rydberg interactions
a The time-average population of \(\left\vert rr\right\rangle\) varies as a function of the modulation index α and the normalized modulation frequency ω0/Ω. The red and green dashed curves correspond to J0(α) = 0 and J1(α) = 0, respectively. b Dynamics of transitions among the four ground states: the \(\left\vert 00\right\rangle\) state remains unaltered, transitions of the \(\left\vert 01\right\rangle\) and \(\left\vert 10\right\rangle\) states exhibit Rabi oscillations with the same Rabi frequency Ωa(t), while the \(\left\vert 11\right\rangle\) state is excited to the \(\left\vert rr\right\rangle\) state via the intermediate state \(\left\vert W\right\rangle\) with equivalent Rabi frequencies of \(\sqrt{2}{\Omega }_{a}(t)\) and \(\sqrt{2}{\Omega }_{b}(t)\), respectively.
