We extend study of the Jaynes-Cummings model involving a pair of identical
two-level atoms (or qubits) interacting with a single mode quantized field. We
investigate the effects of replacing the radiation field mode with a composite
spin, comprising qubits, or spin-1/2 particles. This model is relevant for
physical implementations in superconducting circuit QED, ion trap and molecular
systems. For the case of the composite spin prepared in a spin coherent state,
we demonstrate the similarities of this set-up to the qubits-field model in
terms of the time evolution, attractor states and in particular the collapse
and revival of the entanglement between the two qubits. We extend our analysis
by taking into account an effect due to qubit imperfections. We consider a
difference (or mismatch') in the dipole interaction strengths of the two qubits, for both the field mode and composite spin cases. To address decoherence due to this mismatch, we then average over this coupling strength difference with distributions of varying width. We demonstrate in both the field mode and the composite spin scenarios that increasing the width of the error’ distribution increases suppression of the coherent dynamics of the
coupled system, including the collapse and revival of the entanglement between
the qubits.

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