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理论物理通讯：英文版

Selective Atom-Cavity Interaction Scheme for Quantum Controlled-NOT Gate Using Four-Level Atoms in Cavity QED System

Tang, Shiqing, Zhang, Deng-Yu, Xie, Lijun, Zhan Zhan, Xiao-Gui, Gao Gao, Feng

Published Jan 1, 2009• 2 citations
OpenAlex

Abstract

我们为实现建议一个计划量用通过在洞量 electrodynamics 的一个选择原子洞相互作用的二个四水平的原子的控制不的门操作系统。在我们的协议，量信息在二个原子的稳定的地面状态上被编码。在在原子和单个模式的真空洞地之间的相互作用期间，当大原子洞 detuning 有效地压制原子的自发的腐烂，原子自发的排放是可以忽略的。驱散的影响和控制不的门和我们的建议的试验性的可行性也被讨论的忠实和量的相应成功概率上的相互作用时间的偏差。

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我们为实现建议一个计划量用通过在洞量 electrodynamics 的一个选择原子洞相互作用的二个四水平的原子的控制不的门操作系统。在我们的协议，量信息在二个原子的稳定的地面状态上被编码。在在原子和单个模式的真空洞地之间的相互作用期间，当大原子洞 detuning 有效地压制原子的自发的腐烂，原子自发的排放是可以忽略的。驱散的影响和控制不的门和我们的建议的试验性的可行性也被讨论的忠实和量的相应成功概率上的相互作用时间的偏差。
We propose a scheme for realization a quantum Controlled-NOT gate operation using two four-level atoms through a selective atom–cavity interaction in cavity quantum electrodynamics system. In our protocol, the quantum information is encoded on the stable ground states of the two atoms. During the interaction between atoms and single-mode vacuum cavity-field, the atomic spontaneous emission is negligible as the large atom–cavity detuning effectively suppresses the spontaneous decay of the atoms. The influences of the dissipation and the deviation of interaction time on fidelity and corresponding success probability of the quantum Controlled-NOT gate and the experimental feasibility of our proposal are also discussed.
This paper proposes a scheme for realization of a three-qubit Toffoli gate operation using three four-level atoms by a selective atom-field interaction in a cavity quantum electrodynamics system. In the proposed protocol, the quantum information is encoded on the stable ground states of atoms, and atomic spontaneous emission is negligible as the large atom-cavity detuning effectively suppresses the spontaneous decay of the atoms. The influence of the dissipation on fidelity and success probability of the three-qubit Toffoli gate is also discussed. The scheme can also be applied to realize an N -qubit Toffoli gate and the interaction time required does not rise with increasing the number of qubits.
Cavity quantum electrodynamics (QED) offers powerful possibilities for the deterministic control of atom-photon interactions quantum by quantum [1]. Indeed, modern experiments in cavity QED have achieved the exceptional circumstance of strong coupling, for which single quanta can profoundly impact the dynamics of the atom-cavity system. The diverse accomplishments of this field set the stage for advances into yet broader frontiers in quantum information science for which cavity QED offers unique advantages, such as the realization of quantum networks by way of multiple atom-cavity systems linked by optical interconnects [2,3].