“薛定谔猫”—宏观量子叠加态

综述了近年来在量子光学方面关于“薛定谔猫”态的研究进展，包括其渊源，定义，制备，性质和可能的应用，“薛定谔猫”态本质上是两个宏观可区分的态相干叠加，它涉及量子力学的基本问题，对样一个问题进行研究，将有助于对量子力学的解释进行探讨。     

指向量子计算的约瑟夫森线路

在量子信息处理所涵盖的各分支领域中 ,尽管量子密钥分发的实验已经发展到了实际保密通信中可以利用的阶段 ,量子计算的真正实现仍是一个 10— 2 0年的远期目标 .已建成的核磁共振量子计算机 ,仅仅包括 7个量子位 (qubit) ,其体积却比真空管计算机还要大 .在这台计算机上 ,已经完成的“复杂”运算是 ,将合数 15分解为 3和 5两因子的乘积 .然而理论已经证明 :要想对一个十进制 6 0位数进行因子分解 ,用现行最快的电子计算机 (10 13 次 /s)需作 10 3 0 次运算 ,耗时10 17s(约等于宇宙年龄 ) .如若采用量子算法 ,在量子计算机(运算速度同样是 1…     

宏观量子叠加态（薛定谔猫态）特性

薛定谔猫态是宏观可区分的量子叠加态，本文推导两个成份的光学猫态的平均光子数，二阶相干度的表达式及猫态的光子数分布，揭示出猫态的某些性质。     

量子物理学百年回顾

简述了量子物理学诞生的背景。它的诞生,打开了人们认识微观物质世界运动规律的大门。物质属性及其微观结构问题,只有在量子物理的基础上才在原则上得以解决．量子力学提供了所有现代科学的基础支柱。在过去一百年中,量子物理不仅对于说明众多自然现象取得了无与伦比的成功,它还引发了大量的技术应用。由于量子物理学的基本概念与人们日常生活经验如此不同,诞生伊始至今,对于量子力学原理的诠释存在持续不断的争论。量子理论以前所未有的深度改变了人们的世界观。     

量子叠加态光场中广义电场的N次方H压缩效应

利用多模压缩态理论,研究了一种新型的三态叠加多模量子叠加态光场|Ψ(3)〉q中广义电场分量的等幂次N次方H压缩特性.结果发现,在一定条件下,态|Ψ(3)〉q的广义电场分量总可呈现出周期性变化的广义非线性等幂次N次方H压缩效应.     

量子计算与量子通信

介绍了量子计算的基本原理及量子通信的可行性 ,并对量子信息的表达方式及其实现方法、量子同调态等做了探讨     

量子信息与计算

量子信息与计算是物理学目前研究的热门领域,本文简要地介绍量子计算的一些基本概念：量子纠缠、量子位、量子寄存器、量子并行计算和量子纠错,并介绍两种典型的量子信息技术：量子密码和量子传物。     

量子Grover搜索在离子阱中的实现方案

本文在Cirac-Zoller模型的框架下,讨论在离子阱中如何实现多量子比特Grover搜索的方案。     

量子计算机理论中的量子叠加和量子纠缠

讨论了量子计算、量子通讯与量子计算机中的核心问题 量子叠加和量子纠缠. 从量子态表示量子信息为出发点, 指出有关量子信息的所有问题都可采用量子力学理论来处理. 其中信息的演变遵从薛定谔方程, 信息的传输就是量子态在量子通道中的传送, 信息处理就是量子态的幺正变换, 信息提取则是对量子系统实行量子测量.     

Quantum games via search algorithms

We build new quantum games, similar to the spin flip game, where as a novelty the players perform measurements on a quantum system associated to a continuous time search algorithm. The measurements collapse the wave function into one of the two possible states. These games are characterized by a continuous space of strategies and the selection of a particular strategy is determined by the moments when the players measure.     

Objective Probability and Quantum Fuzziness

This paper offers a critique of the Bayesian interpretation of quantum mechanics with particular focus on a paper by Caves, Fuchs, and Schack containing a critique of the “objective preparations view” or OPV. It also aims to carry the discussion beyond the hardened positions of Bayesians and proponents of the OPV. Several claims made by Caves et al. are rebutted, including the claim that different pure states may legitimately be assigned to the same system at the same time, and the claim that the quantum nature of a preparation device cannot legitimately be ignored. Both Bayesians and proponents of the OPV regard the time dependence of a quantum state as the continuous dependence on time of an evolving state of some kind. This leads to a false dilemma: quantum states are either objective states of nature or subjective states of belief. In reality they are neither. The present paper views the aforesaid dependence as a dependence on the time of the measurement to whose possible outcomes the quantum state serves to assign probabilities. This makes it possible to recognize the full implications of the only testable feature of the theory, viz., the probabilities it assigns to measurement outcomes. Most important among these are the objective fuzziness of all relative positions and momenta and the consequent incomplete spatiotemporal differentiation of the physical world. The latter makes it possible to draw a clear distinction between the macroscopic and the microscopic. This in turn makes it possible to understand the special status of measurements in all standard formulations of the theory. Whereas Bayesians have written contemptuously about the “folly” of conjoining “objective” to “probability,” there are various reasons why quantum-mechanical probabilities can be considered objective, not least the fact that they are needed to quantify an objective fuzziness. But this cannot be appreciated without giving thought to the makeup of the world, which Bayesians refuse to do. Doing this on the basis of how quantum mechanics assigns probabilities, one finds that what constitutes the macroworld is a single Ultimate Reality, about which we know nothing, except that it manifests the macroworld or manifests itself as the macroworld. The so-called microworld is neither a world nor a part of any world but instead is instrumental in the manifestation of the macroworld. Quantum mechanics affords us a glimpse “behind” the manifested world, at stages in the process of manifestation, but it does not allow us to describe what lies “behind” the manifested world except in terms of the finished product—the manifested world, for without the manifested world there is nothing in whose terms we could describe its manifestation.     

基于高维两粒子纠缠态的超密编码方案

基于通信双方预先共享d维二粒子最大纠缠态非定域相关性,信息发送方Bob只需要向信息接收者Alice传送一个粒子,就可以传送logd22比特经典信息,为保护信息的安全,方案采用诱骗光子技术,安全性等价于改进后的原始量子密钥分配方案（Bennett-Brassard 1984,BB84）.本文讨论了基于高维纯纠缠态超密编码方案.即通过引入一个附加量子比特,信息接收方对手中的纠缠粒子和附加粒子在执行相应的幺正演化,可以获取dαk2logd2+logd2（αk=minαj,j∈0,L,d－1）比特经典信息.通信双方采用诱骗光子技术确保量子信道的安全建立.与其他方案相比,该方案具有通信效率较高、实用性较强的优点.     

Generalized superposition of two squeezed states: generation and statistical properties

Superpositions of squeezed states were introduced by Sanders [Phys. Rev. A 39 (1998) 4284], Schleich et al. [Phys. Rev. A 38 (1988) 1177], Xin et al. [Phys. Rev. A 50 (1994) 2865], to investigate the occurrence of nonclassical properties of the quantized radiation field. In this report we present a generalized superposition state which interpolates between two arbitrary squeezed states. Nonclassical properties of this intermediate state as function of the interpolating parameters are studied, the previous results in the literature becoming a particularization of ours. An experimental proposal to generate this state is also presented.     

Quantum M-P Neural Network

Quantum Neural Network (QNN) is a young and outlying science built upon the combination of classical neural network and quantum computing. Making use of quantum linear superposition, this paper presents a quantum M-P neural network based on the analysis of the conventional M-P neural network. Moreover, the working principle of this proposed network and its corresponding weight updating algorithm are expatiated in the two cases of input state being in the orthogonal and non-orthogonal basic set, respectively. In addition, this paper not only validates that this quantum M-P network can realize some network functions, such as “XOR”, but also verifies the feasibility and validity of its weight learning algorithm by some simple examples.     

On Grover’s search algorithm from a quantum information geometry viewpoint

We present an information geometric characterization of Grover’s quantum search algorithm. First, we quantify the notion of quantum distinguishability between parametric density operators by means of the Wigner-Yanase quantum information metric. We then show that the quantum searching problem can be recast in an information geometric framework where Grover’s dynamics is characterized by a geodesic on the manifold of the parametric density operators of pure quantum states constructed from the continuous approximation of the parametric quantum output state in Grover’s algorithm. We also discuss possible deviations from Grover’s algorithm within this quantum information geometric setting.     

Quantum switch for coupling highly detuned superconducting qubits

We propose to implement a quantum switch scheme for coupling highly detuned superconducting qubits connected by a gap-tunable bridge qubit. By modulating the frequency of the bridge qubit, it can be used as a coupler to switch on/off and adjust the coupling strength between the initially non-interaction qubits. It is shown that the proposals of quantum information transfer and quantum entangled gate between two highly detuned qubits can be implemented with high fidelity. Moreover, we extend the case of coupling the switch to multiple qubits for the generation of W states. The advantages of our scheme are that it eliminates the need for tuning the gaps of the qubits and the cross-talk interaction is greatly suppressed. The influence of decoherence and parameter variation is also investigated by numerical simulation, which suggests that the present scheme is feasible in current experiment.