Nucleon structure functions from ν_µ-Fe interactions and a study of the valence quark distribution

Data were taken in 1979-80 by the CCFRR high energy neutrino experiment at Fermilab. A total of 150,000 neutrino and 23,000 antineutrino charged current events in the approximate energy range 25 < E_v < 250GeV are measured and analyzed. The structure functions F2 and xF_3 are extracted for three assumptions about σ_L/σ_T:R=0., R=0.1 and R= a QCD based expression. Systematic errors are estimated and their significance is discussed. Comparisons or the X and Q^2 behaviour or the structure functions with results from other experiments are made.

We find that statistical errors currently dominate our knowledge of the valence quark distribution, which is studied in this thesis. xF_3 from different experiments has, within errors and apart from level differences, the same dependence on x and Q^2, except for the HPWF results. The CDHS F_2 shows a clear fall-off at low-x from the CCFRR and EMC results, again apart from level differences which are calculable from cross-sections.

The result for the the GLS rule is found to be 2.83±.15±.09±.10 where the first error is statistical, the second is an overall level error and the third covers the rest of the systematic errors. QCD studies of xF_3 to leading and second order have been done. The QCD evolution of xF_3, which is independent of R and the strange sea, does not depend on the gluon distribution and fits yield

ʌ_(LO) = 88^(+163)_(-78) ^(+113)_(-70) MeV

The systematic errors are smaller than the statistical errors. Second order fits give somewhat different values of ʌ, although α_s (at Q^2_0 = 12.6 GeV^2) is not so different.

A fit using the better determined F_2 in place of xF_3 for x > 0.4 i.e., assuming q = 0 in that region, gives

ʌ_(LO) = 266^(+114)_(-104) ^(+85)_(-79) MeV

Again, the statistical errors are larger than the systematic errors. An attempt to measure R was made and the measurements are described. Utilizing the inequality q(x)≥0 we find that in the region x > .4 R is less than 0.55 at the 90% confidence level.

Investigação do efeito magnetocalórico convencional e anisotrópico no sistema Er(1-y)Ho(y)N

O efeito magnetocalórico, base da refrigeração magnética, é caracterizado por duas quantidades: a variação isotérmica da entropia (ΔST) e a variação adiabática da temperatura (ΔTad) as quais podem ser obtidas sob variações na intensidade de um campo magnético aplicado. Em sistemas que apresentam anisotropia magnética, pode‐se definir o efeito magnetocalórico anisotrópico, o qual, por definição, é calculado através da variação na direção de aplicação de um campo magnético cuja intensidade se mantém fixa. Nos materiais de nosso interesse, o efeito magnetocalórico é estudado teoricamente partindo de um hamiltoniano modelo que leva em conta a rede magnética (que pode ser composta por diversas sub-redes magnéticas acopladas), rede cristalina e a dinâmica dos elétrons de condução. No hamiltoniano magnético são consideradas as interações de troca, Zeeman e campo cristalino (esta ultima responsável pela anisotropia magnética). Recentemente, estudamos o efeito magnetocalórico convencional e o efeito magnetocalórico anisotrópico nos compostos mononitretos com terras-raras, a saber: Ho(y)Er(1-y)N para as concentrações y= 0,1,0.5 e 0.75. Comparações entre nossos resultados teóricos e os dados experimentais para o EMC foram bastante satisfatórias [3,9]. Além disso, diversas predições teóricas como a existência de uma fase ferrimagnética no sistema Ho(y)Er(1-y)N (para a concentração y=0.5) e reorientações de spin nas sub-redes do Ho e Er foram feitas [25].

O efeito magnetocalórico na série Gd(1-y)Pr(y)Ni2

Em geral, o efeito magnetocalórico (EMC) é caracterizado pela variação adiabática da temperatura (ΔTad) e a variação isotérmica da entropia (ΔST) sob variações do campo magnético. Devido as aplicações tecnológicas do EMC na refrigeração magnética, que não apresentam efeitos perigosos para o meio ambiente e tem o potencial para reduzir o consumo de energia, os estudos sobre o EMC tem crescido ao longo dos anos . Neste trabalho, estudamos as propriedades magnéticas e magnetocalóricos da série Gd (1-Y) Pr (Y) Ni2 com Y = 0; 0,25; 0,5; 0,75 e 1 A série dos compostos RNi2 compostos cristalizam na fase de Laves cúbico C15, o que torna o Campo Elétrico Cristalino cúbico um quadro adequado para descrever a anisotropia magnética sobre estes compostos . Além do modelo hamiltoniano inclui contribuições do efeito Zeeman e as interações de troca indireta entre Gd-Gd, Gd-Pr e íons Pr-Pr. Vale a pena notar que o GdNi2 apresenta um arranjo ferromagnético com temperatura de transição de cerca de 78 K e o composto PrNi2 é paramagnético. Os potenciais magnetocalóricos foram calculados e comparados com os dados experimentais. Além disso, investigamos a influência da direção do campo magnético sobre as quantidades magnéticas e no EMC investigada.

Efficient statistical electromagnetic analysis in reverberant environments

This paper presents a statistical approach to the electromagnetic analysis of a system that lies within a reverberant cavity that has random or uncertain properties. The need to solve Maxwell's equations within the cavity is avoided by employing a relation known as the diffuse field reciprocity principle, which leads directly to the ensemble mean squared response of the system; all that is required is the impedance matrix of the system associated with radiation into infinite space. The general theoretical approach is presented, and the analysis is then applied to a five-cable bundle in a reverberation room © 2013 EMC Europe Foundation.

Highly efficient and tunable microlasers on photonic crystal slab

zhangdi于2010-03-09批量导入

Experimental investigation of slow light phenomenon in photonic crystal waveguide line defect laser

The guide mode whose frequency locates in the band edge in photonic crystal single line defect waveguide has very low group velocity. So the confinement and gain of electromagnetic field in the band edge are strongly enhanced. Photonic crystal waveguide laser is fabricated and the slow light phenomenon is investigated. The laser is pumped by pulsed pumping light at 980nm whose duty ratio is 0.05%. The active layer in photonic crystal slab is InGaAsP multiple quantum well. Light is transimited by a photonic crystal chirp waveguide in one facet of the laser. Then the output light is coupled to a fiber and the character of laser is analysis by an optical spectrometer. It is found that single mode and multimode happens with different power of pumping light. Meanwhile the plane wave expansion and finite-difference time-domain methods are used to simulate the phenomenon of slow light. And the result of the experiment is compared with the theory which proves the slow light results in lasing oscillation.

Magnetic resonant cavity composing of a three layered plasmonic nanostructure

The magnetic-type plasmon resonant of a metal-dielectric-metal nanocavity working at the wavelength of 1.55 mu m is explored, in which the upper layer is periodically patterned with metallic nanostrip arrays. In the dielectric film layer, the magnetic energy intensity is enhanced about 1700 times when irradiated with a p-polarized plane wave. We numerically studied the dispersion of the modes and the Q-value of this periodic cavity arrays. Q value is estimated about 18 and still has room for further improvement. It provides a new type of nanocavity that exhibits a strong magnetic response.

6H-SiC高场输运特性的多粒子蒙特卡罗研究

采用非抛物性能带模型，对6H-SiC高场电子输运特性进行了多粒子蒙特卡罗(Ensemble Monte Carlo)研究．研究表明：温度为296 K时，电子横向漂移速度在电场为2．0×104 V／cm处偏离线性区，5．O×10~5V／cm处达到饱和．由EMC方法得到的电子横向饱和漂移速度为1．95×10~7cm／s，纵向为6．0×10~6cm／s，各向异性较为显著．当电场小于1．0×10~6 V／cm时，碰撞电离效应对高场电子漂移速度影响较小．另一方面，高场下电子平均能量的各向异性非常明显．电场大于2．O×10~5V／cm时，极化光学声子散射对电子横向能量驰豫时间影响较大．当电场一定时，c轴方向的电子碰撞电离率随着温度的上升而增大．对非稳态高场输运特性的分析表明：阶跃电场强度为1．0×10~6 V／cm时，电子横向瞬态速度峰值接近3．O×10~7cm／s，反应时间仅为百分之几皮秒量级．

Quasi-3D Cytoskeletal Dynamics of Osteocytes under Fluid Flow

Osteocytes respond to dynamic fluid shear loading by activating various biochemical pathways, mediating a dynamic process of bone formation and resorption. Whole-cell deformation and regional deformation of the cytoskeleton may be able to directly regulate this process. Attempts to image cellular deformation by conventional microscopy techniques have been hindered by low temporal or spatial resolution. In this study, we developed a quasi-three-dimensional microscopy technique that enabled us to simultaneously visualize an osteocyte's traditional bottom-view profile and a side-view profile at high temporal resolution. Quantitative analysis of the plasma membrane and either the intracellular actin or microtubule (MT) cytoskeletal networks provided characterization of their deformations over time. Although no volumetric dilatation of the whole cell was observed under flow, both the actin and MT networks experienced primarily tensile strains in all measured strain components. Regional heterogeneity in the strain field of normal strains was observed in the actin networks, especially in the leading edge to flow, but not in the MT networks. In contrast, side-view shear strains exhibited similar subcellular distribution patterns in both networks. Disruption of MT networks caused actin normal strains to decrease, whereas actin disruption had little effect on the MT network strains, highlighting the networks' mechanical interactions in osteocytes.

高稳定度大功率开关电源性能参数测量

介绍了重离子加速器磁场系统中高稳定度大功率稳流电源的电流稳定度、电流纹波、效率、EMC等参数的测量方法和仪器 ,并给出了部分电源的测试结果

高品质CsI晶体研制及HPLUS谱仪中电磁量能器模拟

在HIRFL-CSRm的强子物理谱仪(HPLUS)中，电磁量能器(EMC)是其非常重要的组成部分之一。计划中的电磁量能器将使用CsI(Tl)晶体搭建，主要用于高能γ射线和电子的探测，共需要约1020根晶体单元探测器，总重量约3500～5000公斤。另外，我们还计划在CSRm的外靶实验终端建造一个可测量单个射线、所有射线的能量求和以及多重性的γ球探测器，该探测器预计使用CsI(Tl)晶体，总重量约1700公斤。鉴于近代物理所对CsI晶体的大量需求，我们启动了自行研制大尺寸CsI晶体的计划。目前，我们已经掌握了利用Bridgman晶体生长技术，生长出高品质、大尺寸CsI晶体（~100mm×350mm）的工艺。同时我们也掌握了各种不同尺寸和形状的CsI晶体加工工艺。测试结果表明，自行研制的CsI(Tl)晶体的多项指标均好于其他厂家的同类产品。本论文工作的主要内容有：（1）高品质、大尺寸CsI晶体生长工艺的摸索；（2）自制CsI晶体性能的系统测试，包括：光产额的温度效应、PD/APD读出时的能量分辨(源测试)、表面处理和光输出的关系、包装材料的选择、光输出非均匀性、辐照硬度等，以及自制CsI(Tl)晶体在重离子物理实验中的应用等；（3）基于GEANT4软件包，建立了CsI(Tl)晶体探测器的模拟程序，模拟主要集中在对影响单元探测器性能的因素进行分析，包括：侧面泄露、尾部泄露、包装材料的类型和厚度、提前簇射、晶体光输出非均匀性等。建立了EMC探测器的模拟框架，并通过模拟初步确定了HPLUS中EMC探测单元尺寸和和探测单元数目，为EMC设计的优化以及HPLUS的整体模拟打下了重要的基础

HPLUS电磁郎能器的初步设计

在HIRFL-CSRm的强子物理谱仪(HPLUS)中，电磁量能器(EMC)是其非常重要的组成部分之一，其性能将直接影响CSR上强子物理实验的水平。计划中的电磁量能器将使用CsI(Tl)晶体搭建，主要用于探测来自于强子碰撞中的高能光子和电子。中科院近代物理研究所已经完全掌握了高品质、大尺寸(~F100mm×350mm) CsI(Tl)晶体的生长和加工工艺。测试结果表明，近代物理所自行生长的CsI(Tl)晶体的多项指标都明显优于其他厂家的同类产品。目前，使用自行生长的CsI(Tl)晶体制作的探测器在实验中已得到很好的应用，表现出优良的性能。为优化HPLUS的设计，需要进行大量的Monte Carlo模拟计算，包括物理事例产生器的建立、子探测器的设计及其响应、数据的输出等。目前基于GEANT4的HPLUS模拟软件包正在建立中。EMC是HPLUS的子探测器之一，相应的模拟模拟程序也在建立中。本论文的工作的主要内容包含两个方面： (1)自行生长的CsI(Tl)晶体性能系统测试。包括：能量分辨水平、光输出对温度的依赖关系、辐照硬度以及大尺寸晶体的光输出均匀性等。 (2)为HPLUS的EMC探测器搭建了初步的模拟框架。基于GEANT4软件包，建立了EMC的模拟程序，并对EMC prototype探测器的设计进行了初步模拟，如：侧面泄露、尾部泄露、包装材料的类型、提前簇射等，确定了prototype探测器的尺寸和阵列数，为prototype探测器的设计提供参考依据；对CsI(Tl)晶体单元探测器的光学效应也做了相应的模拟，包括晶体的表面处理和几何形状对闪烁光收集的影响等，并在实际工作中指导了晶体的表面处理

宽频带地震数据采集系统的研制

The seismic data acquisition system is the most important equipment for seismic prospecting. The geophysicists have been paying high attention to the specification of the equipment used in seismic prospecting. Its specification and performance are of great concerned to acquire precisely and accurately seismic data, which show us stratum frame. But, by this time, limited by the technology, most of the Broad-band Seismic Recorder (BSR) for lithosphere research of our country were bought from fremdness which were very costliness and maintained discommodiously. So it is very important to study the seismic data acquisition system.The subject of the thesis is the research of the BSR, several items were included, such as: seismic data digitizer and its condition monitor design.In the first chapter, the author explained the significance of the implement of BSR, expatiated the requirement to the device and introduced the actuality of the BSR in our country.In the second chapter, the collectivity architecture of the BSR system was illustrated. Whereafter, the collectivity target and guideline of the performance of the system design were introduced. The difficulty of the system design and some key technology were analyzed, such as the Electro Magnetic Compatibility (EMC), system reliability technology and so on.In the third chapter, some design details of BSR were introduced. In the recorder, the former analog to digital converter (ADC) was separated from the later data transition module. According to the characteristic of seismic data acquisition system, a set high-resolution 24-bit ADC chip was chosen to the recorder design scheme. As the following part, the noise performance of the seismic data channel was analyzed.In the fourth chapter, the embedded software design of each board and the software design of the workstation were introduced. At the same time the communication protocol of the each module was recommendedAt the last part of this thesis, the advantages and the practicability of the BSR system design were summarized, and the next development items were suggested.

基于GIS 的乌江流域（ 贵州境内）非点源污染评价

　　水是人类生存不可或缺的资源，水环境污染问题愈来愈受到人们的重视。随着对点源污染控制能力的提高，非点源污染问题成为当前研究中的热点，而对非点源污染进行定量化研究的最直接、最有效的途径就是建立模拟模型。基于此热点问题，本文选择乌江流域（贵州境内）作为研究区，在ArcGIS 平台上建立了一个简单、快速评价流域非点源污染的方法，它考虑流域的空间异质性，且只需很少的参数。该方法用一个分辨率较高的栅格数字高程模型（DEM）将整个流域划分成100 m×100 m 的格网，计算每个栅格里产生的地表径流量和非点源污染负荷。通过模拟流域地表水流，追踪每个栅格中的水流流向，模拟非点源污染物在流域河网中的运动过程。该方法能计算一个区域水文系统年均非点源污染物的负荷，并能估算出由非点源污染在河网中产生的各污染物浓度值。 　　通过本项研究，能识别出流域内非点源污染严重区域，还可以快速模拟土地利用变化对流域非点源污染的影响，从而为流域今后的规划和综合治理提供科学依据。通过系统的研究，本文主要研究成果如下： 　　1. 建立了乌江流域（贵州境内）非点源污染数据库（空间数据库和属性数据库），这不仅有力地支撑了研究区非点源污染评价研究，同时对于在研究区开展其它方面的研究也是一个有力的支撑。 　　2. 基于Arc Hydro Tools 和DEM 自动提取的流域河网与1:25 万数字水系相比较，两者在总体上吻合较好，特别是两者的主干河道基本重合，这正是在DEM基于GIS 的乌江流域（ 贵州境内） 非点源污染评价预处理中用AGREE 算法将主干河网与DEM 融合的效果；但也有少部分地区（地形平坦处，地形坡度≤3°或受人类活动影响较大的区域）两者存在较大差异，如将红枫湖、百花水库等湖泊水库区描述成河道了，在东干渠和西干渠处，由于人工河渠改变了水流的自然方向，使得提取河网与实际河网差别很大。 　　3. 以流域内的5 个水文站为子流域出口，分别描绘相应子流域，比较自动提取流域面积与实际量测结果，结果表明自动提取的子流域面积与实际量测子流域面积非常接近，相对误差在9％以内，能达到1:25 万数据的精度要求。 　　4. 以流域内5 个子流域的地表径流量，降雨量和土地利用百分比为输入参数，利用多元回归分析工具建立流域降雨径流模型，结果表明模拟相对误差在7%以内，证明所建降雨径流模型能满足模拟需要，模拟精度较高。 　　5. 流域出口处的年均非点源总氮（TN）和总磷（TP）输出通量分别为40309 ton 和2607 ton。从流域内各大支流控制的子流域来看，野济河流域由于其中的耕地面积大（占流域面积的51.21％），以3.03％的流域面积分别贡献了4.08％和3.95％的非点源总氮（TN）和总磷（TP）负荷；而湘江流域，由于其中的林地面积占主导地位（占流域面积的68.94％），以8.45％的流域面积只分别输出了6.40％和6.06％的非点源总氮（TN）和总磷（TP）负荷。因此，对非点源污染的控制要从耕地和草地着手，需要优先治理的流域为野济河流域、三岔河流域、猫跳河流域、偏岩河流域、乌江下干流流域。 　　6. 模拟的非点源总氮（TN）和总磷（TP）浓度值在流域上游明显大于下游。比较水质监测点浓度值与对应的模拟浓度值，可以发现在贵阳站和湘江站的观测值大大超过模拟值：贵阳站的总氮（TN）浓度观测值为9.37 mg/l，模拟值为2.94mg/l，总磷（TP）浓度观测值为0.68 mg/l，模拟值为0.19 mg/l；湘江站的总氮（TN）浓度观测值为5.77 mg/l，模拟值为1.98 mg/l，总磷（TP）浓度观测值为0.27 mg/l，模拟值为0.13 mg/l。另外在思南站的总磷（TP）的观测值也大大超过模拟值，观测值为0.44 mg/l，模拟值为0.14 mg/l。观测值与模拟值之间这种巨大的差异可能暗示在这两处存在明显的总氮（TN）点源污染。而贵阳站和湘江站刚好分别位于贵阳市和遵义市市区的下游，贵阳市和遵义市是流域内最大的两个工业城市。对于观测值小于模拟值的情况，主要有两种可能的原因：①某种土地利用类型的EMC 平均值赋得过高了，或②非点源污染物在随水流运动过程中损失了一部分，如沉淀或分解等。

Multiphysics modelling for electronics design

The future of many companies will depend to a large extent on their ability to initiate techniques that bring schedules, performance, tests, support, production, life-cycle-costs, reliability prediction and quality control into the earliest stages of the product creation process. Important questions for an engineer who is responsible for the quality of electronic parts such as printed circuit boards (PCBs) during design, production, assembly and after-sales support are: What is the impact of temperature? What is the impact of this temperature on the stress produced in the components? What is the electromagnetic compatibility (EMC) associated with such a design? At present, thermal, stress and EMC calculations are undertaken using different software tools that each require model build and meshing. This leads to a large investment in time, and hence cost, to undertake each of these simulations. This paper discusses the progression towards a fully integrated software environment, based on a common data model and user interface, having the capability to predict temperature, stress and EMC fields in a coupled manner. Such a modelling environment used early within the design stage of an electronic product will provide engineers with fast solutions to questions regarding thermal, stress and EMC issues. The paper concentrates on recent developments in creating such an integrated modeling environment with preliminary results from the analyses conducted. Further research into the thermal and stress related aspects of the paper is being conducted under a nationally funded project, while their application in reliability prediction will be addressed in a new European project called PROFIT.