“…As we will show in the following sections, in the case of a qubit and a single harmonic oscillator, this translates into a state that is a superposition of a deexcited qubit and a vacuum, with other states in which the qubit, the oscillator, or both are populated with excitations and photons, respectively. 10,12,13 This is a completely non-RWA effect, which requires large values of the coupling to be observed. More precisely, the excitation probability grows approximately as p e ∝ (g/ω) 2 , and g has to become comparable to the energies of photonhω or of qubithω 0 , making the interaction dynamics both very strong and very fast.…”