“…The suitable level structure is very helpful to implement the robust quantum manipulation. (iv) Different from the previous works [21,35,60], the present three-level system is selected at the magic point of n 0.5 d = , which contributes to remove the dephasing effect and then to prolong the system decoherence time greatly. (v) During the accelerated and reversible transfer process, the intermediate state añ | is almost not populated within the operation time, which makes the robust inversion insensitive to spontaneous emission caused by añ | .…”
Section: Discussionmentioning
confidence: 99%
“…Therefore, the realization of faster population transfer is highly sought after [22,[30][31][32] and from which the desired quantum operation can be performed within a shorter time and decoherence effects can be greatly reduced. Another key point related to optimal QPT is the reversible transferring quantum state [33][34][35], which is a requisite for the storage and retrieval of quantum information.…”
“…The suitable level structure is very helpful to implement the robust quantum manipulation. (iv) Different from the previous works [21,35,60], the present three-level system is selected at the magic point of n 0.5 d = , which contributes to remove the dephasing effect and then to prolong the system decoherence time greatly. (v) During the accelerated and reversible transfer process, the intermediate state añ | is almost not populated within the operation time, which makes the robust inversion insensitive to spontaneous emission caused by añ | .…”
Section: Discussionmentioning
confidence: 99%
“…Therefore, the realization of faster population transfer is highly sought after [22,[30][31][32] and from which the desired quantum operation can be performed within a shorter time and decoherence effects can be greatly reduced. Another key point related to optimal QPT is the reversible transferring quantum state [33][34][35], which is a requisite for the storage and retrieval of quantum information.…”
The present work investigates the entropy and the excitation inversion of a coupled system that consists of a qubit represented by a Cooper pair box (CPB) interacting with a transmission line working as a circuit quantum electrodynamics (CQED). The proposed scheme uses the Buck-Sukumar model with a time dependent frequency in the presence of losses to study the evolution of the entropy and the excitation inversion of the system. We have shown that the CQED is much more sensitive to the presence of losses than the CPB. The results also show that it is possible to monitor properties of the subsystems through appropriate choices of the time-dependent parameters.
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