非晶态Ni-Si-B合金薄膜的霍耳效应和磁阻效应

本文对非晶态Ni-Si-B合金薄膜的霍耳效应和磁阻随磁场变化等电磁性能进行了实验研究。在室温条件下,测量了非晶态Ni-Si-B合金薄膜的霍耳电势差,得出了该薄膜的霍耳系数和相应的每个原子的有效传导电子数Z≈0.3。结果表明,非晶态Ni-S-i-B合金薄膜具有正常的霍耳效应,可用自由电子模型的观点进行(?)述,本文还对非晶态Ni-Si-B合金薄膜的磁阻作了简要讨论。     

直流磁控溅射ZnO:Al薄膜的光电和红外发射特性

以锌、铝合金(ω(Al)=3%)为靶材,利用直流反应磁控溅射法制备了系列掺铝氧化锌ZnO:Al(ZAO)薄膜样品,通过X射线衍射(XRD)、扫描电子显微镜(SEM)、分光光度计、霍耳效应及红外发射率测量仪等测试仪器或方法表征了样品的结构、形貌、光学、电学及红外发射特性.测得样品最低电阻率达到1.8×10^-6(Ω·m),最大禁带宽度为3.47?eV,可见光区平均透过率达到90%,8~14?μm波段平均红外发射率在0.26~0.9之间.上述特性均随衬底温度和溅射功率的变化有着规律的变化.当方块电阻小于45?Ω时,薄膜在8~14?μm波段平均红外发射率与方块电阻遵循二阶函数变化规律.     

航天器可展开薄膜遮光罩的构型设计与优化

针对当前航天器遮光罩轻量化的需求，在保证薄膜遮光罩有效面积不变的前提下，根据质量和有效面积占比设计了一款柔性平面薄膜遮光罩。以提高薄膜边缘应力的同时尽量避免有效圆面积占比减少为优化目标，对薄膜遮光罩的边缘做弧边优化设计。结果表明，当薄膜遮光罩为正六边形时，既能保证结构对称性，又能获得较低的单位有效面积占比对应质量。通过应力叠加法建立了薄膜遮光罩的应力分布模型，求出薄膜边缘应力的理论计算值。探究了弧边拱高的增加对薄膜边缘应力和有效圆面积占比的影响规律，当二者的函数曲线相交于一点时，可取为薄膜弧边的最优拱高。根据设计的薄膜遮光罩参数，搭建薄膜遮光罩的试验样机并进行展开试验。薄膜遮光罩可完全展开，薄膜边缘张紧度高，证明了薄膜遮光罩系统方案设计的可靠性，弧边设计可有效提高薄膜边缘的应力水平。     

基于电子束蒸发沉积的曲面纳米薄膜均匀性研究

半球谐振子金属化是半球谐振陀螺研制过程中的重要环节，针对半球表面薄膜制备均匀性难以实现的问题，提出了一种将薄膜沉积实验和光学模拟相结合的方法。本文采用电子束蒸发技术在半球上沉积Au薄膜，利用台阶仪测量球面上不同位点的薄膜厚度，将平面上的膜厚等效为半球曲面上的膜厚，研究球面薄膜的均匀性，得出了在半球内外表面上薄膜的膜厚分布；同时对薄膜沉积均匀性进行光学模拟，将半球探测器上辐照度等效为实验中沉积所得到的薄膜厚度，计算得出的半球探测器上辐照度分布与实验测量结果一致性较好，可为半球谐振子纳米薄膜的均匀性制备提供理论基础。     

基于ANCF的挠性太阳翼动力学建模及模态辨识研究

可展薄膜结构平面太阳翼由于极具纤薄和轻柔的特性,导致其动力学性能参数显得相当复杂.为全面、准确地明晰大挠性太阳翼动力学特征对新型百公斤级低轨卫星姿态控制性能的影响,采用ANCF(absolute node coordinate formulation)索梁模型和ANCF薄膜单元构建主要挠性附件,基于索梁预应力建立大型空间可展结构的动力学模型.通过建立的动力学模型,综合考虑太阳光压力、气动阻力、重力梯度力矩和地磁力矩在内的复杂空间环境干扰,采用复模态指示函数(complex mode indication function, CMIF)进行薄膜结构平面太阳翼模态参数在轨辨识的研究.辨识结果与仿真分析结果的对比表明,CMIF方法能够有效地识别可展薄膜结构平面太阳翼的低阶固有模态,为该技术的工程实施提供了坚实的理论研究基础.     

紧缩平面场扫描架系统研制

紧缩平面场(CATR)是在较小的微波暗室里模拟远场的电磁环境,以行进各种天线的测量和研究.其最终性能指标要由紧缩平面场扫描架评定.根据紧缩平面场扫描测量原理,及其对扫描架平面度、直线度、定位精度及自动化程度的要求,研制了极坐标型紧缩场扫描架系统,通过采用高精度直线导轨、平面度微调方式和基于工业控制计算机的数字控制技术,达到了所要求的检测精度,满足了紧缩平面场扫描测量的要求.     

天线平面近场测量的研究(二)

<正>一、前言本文第一部分阐述了近场测量方法对今后卫星天线测量的实际必要性;讨论了平面极坐标扫描的近场测量方式。利用罗仑芝(Lorentz)互易原理和雅可比—贝塞尔级数展开的计算方法建立了近—远场变换的数学模式;并列出了一种应用微型计算机程控的平面近场自动测量系统。前面这些讨论仅从理想化的情况研究了平面近场测量的问题。这当中隐含着以下的假定:     

非晶态NiSiB薄膜电阻的弛豫

用射频溅射制备了一组厚度不同的NiSiB非晶态薄膜.在不同温度下,用不同时间对薄膜进行了循环退火.实验测量了循环退火后的薄膜电阻随温度的变化,得到可逆和不可逆两组曲线.厚度较大(>1 000)的薄膜,电阻随温度的增加而增大,厚度较小(<400)的薄膜,电阻随温度的增加而减小.电阻温度系数有正有负.从非晶态材料的结构弛豫出发,应用激活能谱模型和推广的Ziman理论讨论了实验所得的结果.     

太阳帆板平面度测量系统

介绍了一种采用斜光学三角形测量结构和基于虚拟精密测量基准的太阳帆板平面度无接触测量系统.首次提出斜光学三角形测量结构,使得测量系统的测量面积和分辨率大大提高,从而实现了对大面积平面平面度的高精度无接触测量.提出的虚拟精密基准的建模与误差补偿技术,解决了在非精密基准上实现精密测量这一难题,使得所研制的测量系统利用现有平台可实现对太阳帆板平面度的高精度测量.此外,对测量光斑位置估值精度与光斑图像尺寸大小和能量分布之间的定量关系进行了分析,为激光光斑的优化设计提供了理论依据.实际测量结果表明,该测量系统对面积为2581mm×1755mm太阳帆板的平面度测量精度达0.02mm(RMS).     

溅射薄膜热电偶在非金属结构表面瞬态温度测量中的应用研究

介绍了利用薄膜成型技术,在非金属试验件表面用真空离子溅射技术制作薄膜热电偶,进行表面温度测量,并探讨薄膜热电偶在瞬态加热条件下与粘贴的常规热电偶在测温结果上的区别,为今后将薄膜制作技术应用于温度、热流密度及高温应变测量打下基础。     

Bi_(1.9)Pb_(0.3)Sr_(2.0)Ca_(1.7)Mg_(0.3)Cu_(3.1)O_x 超导块材弱连接区的低磁场性

通过对在不同外磁场下Ｂｉ１．９Ｐｂ０．３Ｓｒ２．０Ｃａ１．７Ｍｇ０．３Ｃｕ３．１Ｏｘ超导块材的交流磁化率的测量，获得了样品内晶粒间和晶粒内对外场的不问响应范围．通过与粉状样品实验结果的比较和Ｘ光分析，认为块状样品在温度为１００Ｋ左右出现的抗磁台阶是样品内晶粒间超导弱连接的一种抗磁效应．对弱连接区有效钉扎力Ｆｐ和临界电流密度Ｊｃ与外场Ｈ的关系进行了讨论．     

非晶态（Fe0.5Ni0.5）80—xCrxP14B6合金薄带的磁谱的研究

以阻抗电桥法对非晶态(Fe_(0.5)Ni_(0.5))_(80-z)Cr_zP_(14)B_6(x=0,1,2,3,4,6,10)合金薄带的淬态和等温退火后样品的磁谱进行了测量。结果表明:退火后相对起始磁导宰μ_(?)提高了3.6～6倍,截止频率f_c下降,磁损耗μ_2的磁谱出现了共振峰。同时,等温退火处理对各样品相对起始磁导率的影响比改变Cr元素含量x要大得多。     

非晶态(Fe_(0.5)Ni_(0.5))_(80-x)Cr_xP_(14)B_6合金的内禀磁性和热稳定性的研究

对Cr含量变化对非晶态(Fe_(0.5)Ni_(0.5))_(80-x)Cr_xP_(14)B_6(x=0,1,2,3,4,6,10)合金薄带样品的内禀磁性和热稳定性进行了研究。对所得的随着Cr含量增加,样品的磁性原子的平均磁矩(?)和居里温度T_c的减少,热稳定性的提高等结果进行了讨论。当Cr含量x=4at％时,样品表现出一些特殊性质;而当x>4at％和<4at％时,样品的磁性和热稳定性的变化不尽相同。     

非晶态(Fe_(0.5)Ni_(0.5))_(80-x)Cr_xP_(14)B_6合金薄带的磁场敏感特性的研究

本文对非晶态(Fe_(0.5)Ni_(0.5))_(80-x)Cr_xP_(14)B_6(x=0,1,2,3,4,6,10)合金薄带样品的室温直流磁场敏感特性进行了测量。结果表明,在几十个A/m范围的外磁场内,样品具有开关型磁场敏感特性。对影响开关特性的三个因素进行了一些讨论。     

A Far Infrared Photometer (FIRP) for the Infrared Telescope in Space (IRTS)

We describe the design and calibration of the Far-Infrared Photometer (FIRP), one of four focal plane instruments on the Infrared Telescope in Space (IRTS). The FIRP will provide absolute photometry in four bands centered at 150, 250, 400, and 700 μm with spectral resolution λ/Δλ ≈ 3 and spatial resolution ΔΘ = 0.5 degrees. High sensitivity is achieved by using bolometric detectors operated at 300 mK in an AC bridge circuit. The closed-cycle ³He refrigerator can be recycled in orbit. A 2 K shutter provides a zero reference for each field of view. More than 10% of the sky will be surveyed during the ≈3 week mission lifetime with a sensitivity of <10⁻¹³ W·cm⁻²·sr⁻¹ per 0.5 degree pixel.     

Global Environmental Alert Service (GEAS)

Early warning systems represent an innovative and effective approach to mitigate the risk associated with natural hazards. Early warning technologies are now available for almost all natural hazards and systems are already in operation in all parts of the world. Nevertheless, recent disasters such as the Indian Ocean tsunami in 2004 and Katrina hurricane in 2005, highlighted inadequacies in early warning technologies.

Efforts towards the development of a global warning system are necessary for turning the tide in early warning processes and technologies. There is a pressing need for a globally comprehensive early warning system based on existing systems. The global system should be a mechanism which can consolidate scientific information and evidences, package this knowledge in a form usable to international and national decision makers and actively disseminate this information to those users.

The proposed Global Environmental Alert Service (GEAS) will provide information emanating from monitoring, Earth observing and early warning systems to users in a near-real-time mode and bridge the gap between the scientific community and policy makers. Characteristics and operational aspects of such a service, GEAS, are discussed.     

The INFRARED SPACE OBSERVATORY (ISO)

The INFRARED SPACE OBSERVATORY (ISO), a project of the European Space Agency (ESA), will make various astronomical observations in the wavelength range of 2 to 200 μm. Two-thirds of its observing time will be available to guest observers via the traditional route of proposal submission. ISO will be launched in 1995 by an Ariane 4 from Kourou (Guyana) and be brought into a very elongated orbit with a 24hr period of which 16 hr can be used for astronomical observations. The payload module is essentially a large cryostat with a tank that will be filled with over 2000 litres of superfluid helium to keep the instruments cold (2 to 4 K) during an expected lifetime of 18 months. Inside the dewar, there is a Ritchey-Chretien telescope with a primary mirror of diameter 60cm. Four instruments, each provided by a different PI consortium, share the ISO focal plane. These instruments are : a photometer, a camera and two spectrometers — one for the wavelength range 2–45 μm and the other for 45–180 μm.     

Cometary atmosphere (gas and dust)

There is important progress now in the identifications and measurements of primary (parent) molecules in the inner coma of Comet Halley. H₂O, CO₂ and CO are definitely in the list, CH and some complicate organic molecules are suspected. Gas production rate for water vapor is Q_H2O 10³⁰ s⁻¹. The bulk of data doesn't contradict to the Whipple model of nucleus (with clathrate modification). Pronounced spatial structure of gaseous flow in the coma was observed, but in general measured properties of neutral gas in the coma of Comet Halley are not very different from predicted. Situation for dust is different. In situ dust measurements show that size spectrum and optical properties of particles in coma are substantively declining from predicted on the base of groundbased photometry. However there are discrepancies between Vega and Giotto dust counter data. Dust in the inner coma didn't prevent the succesful imaging of nucleus by TV on Vega 1 and 2.     

光线示波器振子的选用

为了准确地测量记录各种被测信号,应当正确地选用振子的固有频率和阻尼,适当地选取被测信号的大小,保持信号源内阻Ri与振子的内阻rg相匹配,同时要正确地调整光点位置,以减小圆弧误差.