量子点荧光探针的合成

量子点具有宽的激发光谱，窄的发射光谱，高的荧光量子产率，比有机染料寿命更长等优越的荧光特性，是一种理想的荧光探针，本文评述了量子点荧光探针合成的最新进展。     

一种频标变换的方法

对基准频率进行变换通常采用锁相环路或频率搬移电路，前者作为一个环路电路肯定复杂，调试难度增加，后者由于需要混频器或乘法器也存在类似问题．该文介绍的基准频率变换方法实质上是一种频率搬移法。采用MOTOROLA公司生产的MC14011、CMOS与门非电路及模块化晶体带通滤波器可使电路大大简化．调试十分方便。实验结果表明，具有工作可靠、稳定度高、体积小等特点。文中还讨论了工作原理和设计要点。     

定态量子流体动力学模型解的一些估计

有关量子流体动力学模型的研究成为了一个热点问题。研究了当电子密度为正,引入新的变换ω=ρ后,得到稳定态半导体量子流体动力系统的解的L∞估计、H1估计和H2估计。     

量子点中的磁极化子:压缩态变分法

采用基于逐次正则变换的变分方法研究了利用单模压缩态变换处理双线性项的情况下抛物量子点中磁极化子的基态能量．讨论了在弱耦合情况下，受限长度，回旋频率，电子一声子耦合常数与基态能量的依赖关系．     

电容耦合效应对介观LC电路量子效应的影响

将介观电容作为介观隧道结，提出电子波函数在介观电容两极板间有可能存在相互耦合的事实，从而给出介观LC电路的量子化方案。并讨论了电容耦合效应对介观LC电路中电荷和磁通量子涨落的影响。     

关于量子超光速通信的一个理论设想

本文深入分析了拟议中的量子超光速通信理论,提出了实现量子超光速通信的原理与技术方案。此外,本文还讨论了适用于量子超光速通信的新的时空变换,并提出了两种检测特惠Lorentz参照系的实验方法。     

"鹰鸽博弈"的量子分析

在经典的“鹰鸽博弈”中，纳什均衡为一方采取“鹰”策略，而另一方采取“鸽”策略。本文使用量子博弈的方法研究经典的“鹰鸽博弈”，通过量子策略给出了一个不同于经典博弈的新的纳什(Nash)均衡，即博弈双方均采取“鸽”策略，从而达到帕累托(Pareto)最优。     

人字门CAD集成系统的开发与研究

针对船闸人字门的结构形式，采用流行的开发工具和开发平台，引进先进的空间薄壁结构理论，运用面向对象和参数化编程的方法，开发了一套集平面结构初步设计、空间有限元分析优化、施工详图绘制于一体的船闸人字门CAD集成系统，有效提高了人字门的设计效率与设计质量．     

Synthesis and luminescence properties of Mn4+-dopant Ca14Zn6Ga10−xAlxO35 solid solution

Mn~(4+)-activated oxide phosphors,owing to their desirable spectral features,eco-friendly and low cost,are emerging as a new class of non-rare-earth red phosphors for warm white LEDs.However,these phosphors possess low photoluminescence quantum efficiency excited by blue chip currently.Herein we report an isostructural solid solution of Ca_(14)Zn_6Ga_(10-x)Al_xO_(35):0.15Mn~(4+)(0≤x≤10)synthesized by a traditional solidstate reaction route.The microstructure and luminescent performance of this red-emitting phosphor are investigated in detail with the aids of X-ray diffraction,diffuse reflection spectra,photoluminescence spectra/decay/QE,and temperature-dependent PL/QE measurements.Blue shift of energy peaks of~4A_2→~4T_1and~4A_2→~4T_2transition is illustrated by the Tanabe–Sugano diagram and the configurational coordinate diagram.The crystal field strength(Dq)and the Racah parameters(B and C)are carefully calculated to estimate the nephelauxetic effectβrespectively.Particularly we achieve external and internal quantum efficiencies as high as26.1%and 40.3%for Ca_(14)Zn_6Ga_6Al_4O_(35):0.15Mn~(4+)excited by 466 nm,the highest one ever reported in Mn~(4+)activated oxide phosphors under the similar condition.     

I ain’t afraid of no ghost

This paper criticizes the traditional philosophical account of the quantization of gauge theories and offers an alternative. On the received view, gauge theories resist quantization because they feature distinct mathematical representatives of the same physical state of affairs. This resistance is overcome by a sequence of ad hoc modifications, justified in part by reference to semiclassical electrodynamics. Among other things, these modifications introduce ”ghosts”: particles with unphysical properties which do not appear in asymptotic states and which are said to be purely a notational convenience. I argue that this sequence of modifications is unjustified and inadequate, making it a poor basis for the interpretation of ghosts. I then argue that gauge theories can be quantized by the same method as any other theory. On this account, ghosts are not purely notation: they are coordinates on the classical configuration space of the theory—specifically, on its gauge structure. This interpretation does not fall prey to the standard philosophical arguments against the significance of ghosts, due to Weingard. Weingard’s argumentative strategy, properly applied, in fact tells in favor of ghosts’ physical significance.