环境标准中pH值限值的合理性探讨

鉴于在不同的温度下水(或溶液)的pH值会有所不同,对环境标准中不规定pH值限值的温度条件是否合理进行了论证。通过分析各环境标准的特点、各环境标准中pH值参数的控制目的,结合各环境标准指定的监测方法的技术内容,得出以下结论:《海水水质标准》、《地表水环境质量标准》、《污水综合排放标准》和《土壤环境质量标准》中pH值限值不规定温度条件是合理、可操作的;《危险废物鉴别标准腐蚀性鉴别》pH值限值应该规定温度条件;对于《地下水质量标准》,有待于进一步实验验证温度对pH值的影响程度。     

Generation of four-atom cluster states in thermal cavity and implementing remote controlled not gate

We propose an experimentally feasible scheme for preparing a four-atom cluster state in a thermal cavity. In the scheme, the cavity field is only virtually excited and the photon-number-dependent part in the effective Hamiltonian is cancelled so that the system is insensitive to the cavity decay and the thermal field. At the same time, the scheme can be generalized to prepare n-atom cluster states with the success probability 100\%. In addition, using the four-atom cluster state, we also propose a simpler scheme for implementing a remote--controlled not gate (CNOT) without the Bell states measurement.     

A scheme for conditional quantum phase gate viabimodal cavity and a Λ-type three-level atom

We propose a scheme to implement a two-qubit conditional quantum phase gatefor the intracavity field viaa single three-level $\Lambda$-type atom driven by two modes in a high-Q cavity. The quantum information is encoded on the Fock states of the bimodal cavity. The gate's averaged fidelity is expected to reach $99.8\%$.     

Unconventional Geometric Phase-Shift Gates Based on Superconducting Quantum Interference Devices Coupled to a Single-Mode Cavity

We present a scheme to realize geometric phase-shift gate for two superconducting quantum interference device （SQUID） qubits coupled to a single-mode microwave field. The geometric phase-shift gate operation is performed in two lower flux states, and the excited state [2〉 would not participate in the procedure. The SQUIDs undergo no transitions during the gate operation. Thus, the docoherence due to energy spontaneous emission based on the levels of SQUIDs are suppressed. The gate is insensitive to the cavity decay throughout the operation since the cavity mode is displaced along a circle in the phase space, acquiring a phase conditional upon the two lower flux states of the SQUID qubits, and the cavity mode is still in the original vacuum state. Based on the SQUID qubits interacting with the cavity mode, our proposed approach may open promising prospects for quantum iogic in SQUID-system.     

The non—local implementation of a CNOT gate and single—qubit rotation

We show how a CNOT gate and single-qubit rotation can be implemented non-locally,We also report on the quantitative relations between these quantum actions,entanglement and classical communication resources required in the implementation.     

Preparation of arbitrary n-particle d-dimensional superposition states using only single qubit operations and CNOT gates

In this article, using only single qubit operation and a CNOT gate, we propose a scheme for creating arbitrary n-particle d-dimensional superposition states including entangled states and give the relevant circuits for realizing this scheme.     

Implementation of non-local multiple qubits controlled-not operation via partially entangled channels

We propose two different schemes for probabilistic implementing a non-local multiple qubits controlled-not operation via partially entangled quantum channels. The overall physical resources required for accomplishing these schemes are different, and the successful implementation probabilities are also different.     

细菌视紫红质用于光子逻辑门的研究

本文对基于细菌视紫红质变种材料D96N的三种基本光逻辑操作进行了研究.随着入射黄光强度的增加,菌紫质对黄光的吸收呈饱和吸收特性,此时紫光的照射将会使此饱和吸收阈值增加.在黄光和紫光对样品的共同作用下,透射光强度会被调制,调制的程度取决于这两束光的相对强度以及被调制光波长.通过观测被调制的525nm检测光强度,我们模拟了几种基本的光子逻辑运算:“非”、“或”和“与”运算.     

辐射俘获反应中门态过程的干涉现象

主要计算中子能量为5—25MeV ¹²C(n,γ)反应截面,计算结果表明,在Ex=13MeV处有矮共振存在,同时,也计算了质子能量为8—35MeV ¹²C(p,γ)反应截面.计算表明对应13N激发能量为11.74MeV和14.06MeV处反应截面有谷点存在.这是因为半直接俘获与门态过程中的共振俘获之间有相消干涉效应,计算结果与实验值符合较好.     

散射介质成像中的时间门研究

研究了用蒙特卡罗方法模拟均匀散射介质中含有光学性质不同的小球时,漫反射信号随时间的变化,当小球和激励源的相对位置不同时随时间变化的漫反射曲线也不同,利用这种漫反射信号的差异同时结合时间门技术可以对散射介质中一定浓度的物体成像。结论表明成像对比度与时间门的开始时刻和时间门宽度有直接关系。针对小球投影位置漫反射信号的强和弱,分别用半宽度点和最大强度的80％点作为小球办界位置的判断。