At resonance (omega_d = 2*omega_f), the rotating-frame Hamiltonian is:
H_rot=eps2(t)*(a_dag^2+a^2)
The drive maps the delivered in-phase signal to a^2+a_dag^2. A carrier
frequency of 2*omega_f makes the weight-two operator bands resonant in the
corresponding rotating frame.
The real-field projection halves the scheduled amplitude, so an envelope of
amplitude A(t) scheduled on this drive contributes
A(t)/2*(a_dag^2+a^2) to H_rot, not A(t)*(a_dag^2+a^2). A
schedule of amplitude=2*eps2(t) realizes the eps2(t) coefficient
shown in H_rot above.
Parametric two-photon drive for Kerr-cat qubit stabilisation.
Coupling operator: a^2+a_dag^2
Schedule the drive at twice the cavity frequency
(freq=2*cavity.freq) so the rotating-frame interaction is static:
eps2(t)*(a_dag^2+a^2). Kerr nonlinearity combined with the
two-photon drive creates and stabilises cat states.
The engine band-decomposes a^2+a_dag^2 into excitation weights
Delta_n = +2 and Delta_n = -2 and combines them with the delivered
signal’s carrier.
The real-field projection contributes only half the scheduled envelope
amplitude to each band. The coefficient on a_dag^2+a^2 in the
rotating frame is A(t)/2, where A(t) is the amplitude scheduled on
this drive’s envelope. Schedule amplitude=2*eps2(t) to realize the
target two-photon drive strength eps2(t) used above and in
alpha^2=eps2/K.
Parameters:
target (BaseDevice | None) – Device to connect this drive to. None means unconnected.