3G博弈

信息产业部电信研究院主办,中国泰尔网承办的“2006中国通信产业发展形势报告会———暨‘2005年中国通信产业十大关键词活动’评选发布会”具体内容,本刊已在2005年第6期上报道。本期刊登“2005年通信产业十大关键词”:电信普遍服务、IPTV、网络融合、电信转型、3G博弈、电信资费、TD-SCDMA测试、互联网治理、下一代网络、Wi MAX部分点评文章,与读者共同回顾2005年我国通信产业发展的热点和焦点,探讨我国通信产业各个相关领域的发展现状及前景。———编者的话     

基于时频分布的信号相位跳变检测与估计方法

本文提出了利用时频分布的信号相位跳变检测方法,对由相位跳变而引起的时频分布峰值的变化规律进行了讨论。分析表明信号时频表示的幅度能够直观地反映出其相位的变化,因此通过对时频分布峰值特征的检测可以准确定位频率跳变时刻,并能够定量的了解这些参数的变化,从而为信号的相位调制类型识别提供帮助。相应的仿真实验证明了这一分析结论。     

MIMO-OFDM系统Turbo接收机中的限幅非线性失真迭代对消法

在多入多出的正交频分复用系统中,常采用Turbo接收以保证系统性能。在正交频分复用系统中,限幅技术是常见的峰值平均功率比抑制技术,但限幅带来的非线性失真会造成带内失真和带外辐射,从而恶化系统性能。本文提出可以利用Turho接收机的先验信息进行限幅非线性失真的迭代对消,从而在引入少量复杂度的基础上,对抗限幅带来的影响。仿真结果表明,引入限幅非线性失真迭代对消算法可以有效提高系统性能,限幅门限越低效果越明显。     

双光子B-J模型中类克尔介质对量子态保真度的影响

研究了充满类克尔介质的高 Q腔中二能级原子与单模相干光场发生双光子相互作用 (双光子 B- J模型 )时 ,类克尔介质对该体系量子态保真度的影响。结果表明 :当类克尔介质与光场耦合较强时 ,原子的量子态保真度为 1,即原子处于退纠缠状态 ,此时光场对原子的作用被类克尔介质所屏蔽。     

Flat panel detector-based cone-beam volume CT angiography imaging: system evaluation

Preliminary evaluation of recently developed large-area flat panel detectors (FPDs) indicates that FPDs have some potential advantages: compactness, absence of geometric distortion and veiling glare with the benefits of high resolution, high detective quantum efficiency (DQE), high frame rate and high dynamic range, small image lag (< 1%), and excellent linearity (approximately 1%). The advantages of the new FPD make it a promising candidate for cone-beam volume computed tomography (CT) angiography (CBVCTA) imaging. The purpose of this study is to characterize a prototype FPD-based imaging system for CBVCTA applications. A prototype FPD-based CBVCTA imaging system has been designed and constructed around a modified GE 8800 CT scanner. This system is evaluated for a CBVCTA imaging task in the head and neck using four phantoms and a frozen rat. The system is first characterized in terms of linearity and dynamic range of the detector. Then, the optimal selection of kVps for CBVCTA is determined and the effect of image lag and scatter on the image quality of the CBVCTA system is evaluated. Next, low-contrast resolution and high-contrast spatial resolution are measured. Finally, the example reconstruction images of a frozen rat are presented. The results indicate that the FPD-based CBVCT can achieve 2.75-lp/mm spatial resolution at 0% modulation transfer function (MTF) and provide more than enough low-contrast resolution for intravenous CBVCTA imaging in the head and neck with clinically acceptable entrance exposure level. The results also suggest that to use an FPD for large cone-angle applications, such as body angiography, further investigations are required.     

Structural features of toxic chemicals for specific toxicity

We have studied the structural features of toxic chemicals from the RTECS database associated with specific toxicity. The frameworks, functional groups, and structure patterns of molecules are taken into account. Potential active frameworks, groups, and structure patterns for specific toxicity are gained by computational chemistry approaches. These structural features of toxic chemicals will be helpful in understanding activities of toxic chemicals and useful in predicting the toxicity of chemicals, especially in the early stage of drug design.     

带模糊约束的最小费用流问题

本文首次提出了带模糊约束的最小费用流问题,建立了相应的数学模型并给出了求解这一模型的有关算法。最后,给出了一个具体实例。     

一阶时滞微分方程解的零点分布

Abstract. The paper gives two estimates of the distance between adjacent zeros of solutions     

磁通钉扎液体的动力学特性

依据Ｍａｌｏｚｅｍｏｆｆ和Ｇｒｉｅｓｓｅｎ等建议的表征高温超导体有效钉扎势的唯象表式Ｕ（Ｔ,Ｂ,Ｊ）＝Ｕｏ（Ｔ,Ｂ）／μ（Ｔ,Ｂ）［Ｊｃ（Ｔ,Ｂ）／Ｊ）＾μ（Ｔ,Ｂ）－１］和热激活涡旋运动模型,并通过ＹＢａ２Ｃｕ３Ｏ７－δ薄膜直流传输特性的测量结果,利用“函数唯一性”数据处理方法,研究了钉扎液体的玻璃态指数μ（Ｔ,Ｂ）随温度与外磁场的负值函数形式。以及钉扎势垒Ｕｏ（Ｔ,Ｂ）和Ｊｃ（Ｔ,Ｂ）随外场与     

Design criteria of a chemical reactor based on a chaotic flow

We consider the design criteria of a chemical mixing device based on a chaotic flow, with an emphasis on the steady-state devices. The merit of a reactor, defined as the Q-factor, is related to the physical dimension of the device and the molecular diffusivity of the reactants through the local Lyapunov exponents of the flow. The local Lyapunov exponent can be calculated for any given flow field and it can also be measured in experimental situations. Easy-to-compute formulae are provided to estimate the Q-factor given either the exact spatial dependence of the local Lyapunov exponent or its probability distribution function. The requirements for optimization are made precise in the context of local Lyapunov exponents. (c) 1999 American Institute of Physics.