V型原子与光场拉曼相互作用传送未知原子态

未知量子态从一个地方到另一个地方的隐形传送在量子信息领域中有非常重要的作用,提出了一种利用简并V型三能级原子与振幅很大的单模相干态腔场的拉曼相互作用来传送未知原子态的方案。     

利用拉曼型的Jaynes-Cummings模型传送两比特的未知原子态

实现量子态的隐形传送、尤其是多比特量子态的隐形传送在量子信息领域中有非常重要的作用,提出了一种隐形传送两比特未知原子态的方案,在此方案中,用两个两粒子纠缠态代替一个三粒子纠缠态作为量子信道,而且此方案可推广到隐形传送N比特的未知原子态。     

Probabilistic teleportation of an arbitrary three-particle state

A scheme for teleporting an arbitrary and unknown three-particle state from a sender to either one of two receivers is proposed. The quantum channel is composed of a two-particle non-maximally entangled state and two three-particle non-maximally entangled W states. An arbitrary three-particle state can be perfectly teleported probabilistically if the sender performs three generalized Bell-state measurements and sends to the two receivers the classical result of these measurements, and either one of the two receivers adopts an appropriate unitary transformation conditioned on the suitable measurement outcomes of the other receiver. All kinds of unitary transformations are given in detail.     

利用Raman型的Jaynes-Cummings模型传送光场的福克叠加态

提出了一种利用Λ型三能级原子与光场Raman相互作用来传送光场的福克叠加态的方案.     

Scheme for the implementation of 1→3optimal phase-covariant quantum cloning in ion-trap systems

This paper proposes a scheme for the implementation of 1→ 3 optimal phase-covariant quantum cloning with trapped ions. In the present protocol, the required time for the whole procedure is short due to the resonant interaction, which is important in view of decoherence. Furthermore, the scheme is feasible based on current technologies.     

无标度神经元网络化学突触耦合诱导的依赖于时滞的同步转迁（摘要）

研究表明,神经元体系中化学突触耦合较电耦合更加普遍.本文研究了时滞无标度热敏神经元网络中化学耦合诱导的同步转迁现象.发现,不同延迟时间下有不同形式的同步转迁行为.无时滞情况下,出现从混沌簇放电到簇同步转变;对于较小的延迟时间,从混沌簇放电到峰放电同步;对于较大的延迟时间,则间歇性地出现从混沌簇放电到峰放电的多次同步转迁.这表明,化学突触耦合诱导的同步转迁行为强烈地依赖于时滞大小.这一发现可以帮助人们更好地了解时滞和化学耦合共同作用下神经元的放电活动.     

Implementing the Deutsch-Jozsa algorithm by using Schrodinger cat states in cavity QED

We propose a scheme to implement the Deutsch-Jozsa algorithm by using Schroedinger cat states in cavity quantum electron-dynamics （QED）. The scheme is based on the Raman interaction of a degenerate three-level A-type atom with a coherent state in a cavity. By using Schroedinger cat states, the atomic spontaneous emission can be minimized and the Hadamard transformation in our scheme is not needed.