中心化开放式大学物理实验教学管理系统的设计

研究型大学建设背景下,农林院校大学物理实验实行中心化开放式教学,有效发挥公共基础课教学的基础性作用,具有十分重要的意义.根据高等农林院校中心化开放式教学的特点,采用B/S和C/S混合模式,设计了中心化开放式大学物理实验教学管理系统.该系统的使用保证了中心化开放式大学物理实验教学体系的运行,实现了多元化的考核方式,使物理实验教学中心资源发挥了最大效益,在提高学生的综合素质、培养学生的创新精神与实践能力方面发挥重要作用.     

500—4250eV电子对CO2的散射全截面绝对测量

对中能电子与二氧化碳分子碰撞的散射全截面测量，给出５００－４２５０ｅＶ电子对ＣＯ２的绝对散射全截面。对测量结果作了曲线拟合，并与已有的实验和理论结果进行了比较     

发挥科技创新支撑作用进一步提高企业自主创新能力——来自上海市青浦区科技管理工作的思考

进入2009以来，随着国家和各级政府相继出台了一系列信贷、税收、物价、产业规划等政策，“经济寒冬”开始慢慢回暖。 在应对危机过程中，不管从国家发展战略、应对金融危机、建设“绿色青浦”的高度出发，还是从解决企业实际困难、帮助大学生创业就业等具体实践来看，越来越多的现实使我们更加深刻地认识到，提高创新能力，是推动经济平稳较快发展、增强综合竞争力的核心工程；是做大做强企业、解决群众就业问题的民心工程；是调整产品结构、提高产品技术含量和附加值的重点工程；是扩大开放、加强国际间交流与合作、赢得良好外部发展环境的纽带工程。     

浅谈铁路客车电气化厨房系统设计

本文从当前实际运营的铁路客车电气化厨房系统分析，简要阐述了铁路客车电气化厨房系统设计特点和基本要素.     

浙江大学青年创业俱乐部：大学生创业的源头活水

2009年11月25日，浙江大学国家大学科技园的“杭州市大学生创业园（西湖·浙大科技园）”大楼内，许多年轻人聚集在一起，热烈地讨论着关于“教育培训和高校服务类企业”的话题。原来，他们正在参加浙大科技园创业青年交流活动中心举办的定期沙龙活动。     

基于腔辅助相互作用的远距离信息传递

提出了一种基于腔辅助相互作用的远距离信息传递的方案.在该方案中,通过让一束相干光和一个囚禁在腔里面的原子进行相互作用,可以使相干光产生一个可控的相位偏移.用这种腔辅助相互作用完成了原子态和光场态之间信息的相互转移.最后我们演示了远距离信息传递方案,该方案在当前实验条件下是可行的,并且在理想条件下,成功的概率几乎为1.     

基于D2shepp统计法的非序列局部比对

两条生物序列间的相似性比对是计算生物学探讨的主要问题之一,一种快速的依赖于k-元组的D2shepp统计法目前已被应用到非序列比对中.文中在零模型的基础上产生两条相互独立的随机序列,基于D2shepp统计法进行了两条序列的局部比对,找到局部比对的最优值并求和.在此基础上模拟了Power值的分布情况,并分析了不同k参数下的Power值分布.在相同参数下将文中提出的局部比对与已有的D2shepp统计的全局比对进行比较,发现局部比对D2shepp统计的Power值随着序列长度的增大而快速地接近于1,比全局比对更加快速、准确.     

Entanglement control in one-dimensional s= 1/2 random XY spin chain

The entanglement in one-dimensional random XY spin systems where the impurities of exchange couplings and the external magnetic fields are considered as random variables is investigated by solving the different spin-spin correlation functions and the average magnetization per spin. The entanglement dynamics near particular locations of the system is also studied when the exchange couplings （or the external magnetic fields） satisfy three different distributions （the Gaussian distribution, double-Gaussian distribution, and bimodal distribution）. We find that the entanglement can be controlled by varying the strength of external magnetic field and the distributions of impurities. Moreover, the entanglement of some nearest-neighbouring qubits can be increased for certain parameter values of the three different distributions.     

Self-organization effect in poly（3-hexylthiophene）： methanofullerenes solar cells

This paper studies the self-organization of the polymer in solar cells based on poly（3-hexylthiophene）： [6, 6]-phenyl C61-butyric acid methyl ester by controlling the growth rate of active layer. These blend films are characterized by UV-vis absorption spectroscopy, charge-transport dark J - V curve, x-ray diffraction pattern curve, and atomic force microscopy. The results indicate that slowing down the drying process of the wet films leads to an enhanced selforganization, which causes an increased hole transport. Increased incident light absorption, higher carrier mobility, and balanced carrier transport in the active layer explain the enhancement in the device performance, the power conversion efficiency of 3.43% and fill factor up to 64.6% are achieved under Air Mass 1.5, 100 mW/cm^2.     

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^-.