考虑渗透系数变化的地下结构温度-渗流耦合分析

地下岩体的温度随着深度的增加呈逐渐上升的趋势，在地下水的作用下，岩体温度-渗流耦合作用明显。分析了地下岩体温度场与渗流场间的相互作用效应，考虑流体渗流和岩体骨架本身的热传导作用以及温度梯度所产生的渗流作用，并计入温度对水体运动粘滞系数及岩体渗透率的影响，给出了完整的基于连续介质模型的地下岩体温度-渗流耦合数学模型。借助...     

Thermal Entanglement of an XY Two-Qutrit Spin Chain with Dzialoshinski-Moriya Interaction

The effect of Dzialoshinski-Moriya （DM） interaction on thermal entanglement of an XY two-qutrit spin chain is investigated. We find that DM interaction and the anisotropy parameter can enhance quantum thermal entanglement to a maximal value individually. However, when both of them take large values, the entanglement is not enhanced, but is destroyed. Our analysis will shed some light on the understanding of the effect of the DM interaction on thermal entanglement of an XY two-qutrit spin chain.     

All Pure Two-Qudit Entangled States Generated via a Universal Yang-Baxter Matrix Assisted by Local Unitary Transformations

We show that all pure entangled states of two d-dimensional quantum systems （i.e., two qudits） can be generated from an initial separable state via a universal Yang-Baxter matrix if one is assisted by local unitary transformations.     

Entanglement Purification for Mixed Entangled Quantum Dot States via Superconducing Transmission Line Resonators

An entanglement purification protocol for mixed entangled states is presented via double quantum dot molecules inside a superconducing transmission line resonator （TLR）. In the current scenario, coupling for arbitrary double quantum dot molecules can be tuned via the TLR in the large detuning region by controlling the qubit level splitting. The TLR is always empty and only virtually excited, so the interaction is insensitive to both the TLR decay and thermal field. Discussion about the feasibility of our scheme shows that the entanglement purification can be implemented with high fidelity and successful probability.     

基于极化-空间模超纠缠的量子网络多跳纠缠交换方法研究

基于纠缠交换方法进行多跳量子信息传输,是实现远距离量子网络通信的基本方式之一.传统的多跳量子网络通常使用单自由度极化光子纠缠态作为量子信道,信息传输容量较低且容易受到噪声的干扰.本文提出一种基于超纠缠的高效量子网络多跳纠缠交换方法,利用极化-空间模式两自由度的纠缠光子,建立超纠缠量子多跳信息传输通道.以远程超纠缠隐形传态的信道建立需求为例,首先给出了基础的逐跳超纠缠交换方案,为降低该方案的端到端超纠缠建立时延,提出在中间量子节点进行同时测量的并行超纠缠交换方案.在此基础上,为降低并行超纠缠交换的经典信息开销,进一步提出一种分级并行超纠缠交换方案.理论分析及仿真结果表明该方案的纠缠建立时延接近于并行超纠缠交换方案,但可以减少经典信息传输量,在一定程度上实现两者的平衡.相比传统的纠缠交换方法,本文方案有利于解决远程超纠缠通信的需求,对未来构建更高效率的量子网络有积极意义.     

Wigner function for the generalized excited pair coherent state

This paper introduces the generalized excited pair coherent state （GEPCS）. Using the entangled state 〈η〉 representation of Wigner operator, it obtains the Wigner function for the GEPCS. In the ρ-γ phase space, the variations of the Wigner function distributions with the parameters q, α, k and l are discussed. The tomogram of the GEPCS is calculated with the help of the Radon transform between the Wigner operator and the projection operator of the entangled state ｜η1, η2, τ1, τ2｜. The entangled states ｜η〉 and ｜η1, η2, τ1, τ2〉 provide two good representative space for studying the Wigner functions and tomograms of various two-mode correlated quantum states.     

Generation of four-photon W state via cavity QED

This paper proposes an alternative scheme for generating four-photon W state via cavity QED. The scheme bases on the resonant interaction of a A-type three level atom with two bimodal cavities. The detection of atom collapses the cavity to the desired state. Comparing with previous schemes, the advantage of this scheme is that the interaction time can be greatly shortened since it uses the resonant interaction between atom and cavities. Moreover, the proposed scheme is more experimentally feasible than the previous ones.     

Analytic solutions for degenerate Raman-coupled model

The Raman-coupled interaction between an atom and a single mode of a cavity field is studied. For the cases in which a light field is initially in a coherent state and in a thermal state separately, we have derived the analytic expressions for the time evolutions of atomic population difference W, modulus B of the Bloch vector, and entropy E. We find that the time evolutions of these quantities are periodic with a period of π. The maxima of W and B appear at the scaled interaction time points τ- = kπ（k = 0, 1, 2,...）. At these time points, E = 0, which shows that the atom and the field are not entangled. Between these time points, E ≠ 0, which means that the atom and the field are entangled. When the field is initially in a coherent state, near the maxima, the envelope of W is a Gaussian function with a variance of 1/（4n^-）（n^- is the mean number of photons）. Under the envelope, W oscillates at a frequency of n^-/π. When the field is initially in a thermal state, near the maxima, W is a Lorentz function with a width of 1/n^-.