位移测量中真空室偶极涡流的影响及其扣除

一、真空室上偶极涡流对测量的影响 在托卡马克放电中,出现宏观不稳定性时,等离子体电流会出现小的正尖峰,并在整个大环上沿水平方向向内快速收缩。这时真空室(薄不锈钢壳)上会感应出很大偶极涡流,如图1所示,真空室上偶极电流分布为     

激子位置不同微腔有机电致发光器件性能模拟

微腔有机电致发光器件(MOLED)的发光特性直接与微腔的结构相关,可以根据微腔器件的相关计算公式,运用传输矩阵法对MOLED进行模拟设计。本文对微腔总长度L=λ/2(λ:中心波长)不变情况下,激子在微腔内不同位置复合发光的电致发光(EL)光谱性能进行模拟并比较。结果表明:发光谱的峰值都在所设计的中心波长520nm处,半峰全宽(FWHM)都是17nm,激子处在微腔的中心区域时,峰值强度和积分强度都是最大,这是因为激子此时位于腔内电场的最大值处,偏离此处的两侧逐渐变小。以上结果表明:要制作出高效率的MOLED,必须使激子处于微腔内的最佳位置处。     

10m×10m大靶面激光立靶设计

针对10m×10m大靶面、高精度立靶坐标测量的要求,提出了一种激光阵列式光电立靶坐标测量系统,该立靶采用半导体激光平行光管形成平行光光源,高灵敏度光电二极管及相应信号放大、转换电路组成接收阵列,光源和接收器件相距10m,当飞行弹丸穿越激光形成的光幕时,分别在X和Y方向上挡住了投射在某一个或几个光电二极管上的光线,该光电二极管对应的信号放大、转换电路将二极管产生的微弱电信号放大、整形,最后输出脉冲信号,后续信号编码识别电路将判断出被挡住光线的光电二极管的编号,进而得出弹丸穿越该光幕的X坐标和Y坐标。经实弹试验证明,系统具有测量靶面大,精度高的优点。     

如何通过测量复摆的周期计算转动惯量

本文给出一种简约可行的方法,用来计算不规则物体绕任意轴转动时的转动惯量,同时,亦可定出质心轴位置.本文讨论的内容对教学有意义.     

Development of diamond-based X-ray detection for high-flux beamline diagnostics

High‐quality single‐crystal and polycrystalline chemical‐vapor‐deposition diamond detectors with platinum contacts have been tested at the white‐beam X28C beamline at the National Synchrotron Light Source under high‐flux conditions. The voltage dependence of these devices has been measured under both DC and pulsed‐bias conditions, establishing the presence or absence of photoconductive gain in each device. Linear response consistent with the theoretically determined ionization energy has been achieved over eleven orders of magnitude when combined with previous low‐flux studies. Temporal measurements with single‐crystal diamond detectors have resolved the nanosecond‐scale pulse structures of both the NSLS and the APS. Prototype single‐crystal quadrant detectors have provided the ability to simultaneously resolve the X‐ray beam position and obtain a quantitative measurement of the flux.     

First high-resolution analysis of the 4ν1+ν3 band of nitrogen dioxide near 1.5 μm

The high-resolution absorption spectrum of the 4ν₁+ν₃ band of the ¹⁴N¹⁶O₂ molecule was recorded by CW-Cavity Ring Down Spectroscopy between 6575 and 6700 cm⁻¹. The assignments involve energy levels of the (4,0,1) vibrational state with rotational quantum numbers up to K_a=8 and N=48. A large majority of the spin-rotation energy levels were reproduced within their experimental uncertainty using a theoretical model which takes explicitly into account the Coriolis interactions between the spin-rotational levels of the (4,0,1) vibrational state and those of the (4,2,0) and of (0,9,0) dark states, the anharmonic interactions between the (4,2,0) and (0,9,0) states together with the electron spin-rotation resonances within the (4,0,1), (4,2,0) and (0,9,0) states. Precise vibrational energies, rotational, spin-rotational, and coupling constants were determined for the {(4,2,0), (0,9,0), (4,0,1)} triad of interacting states. Using these parameters and the value of the transition dipole-moment operator determined from a fit of a selection of experimental line intensities, the synthetic spectrum of the 4ν₁+ν₃ band was generated and is provided as Supplementary Material.     

位置控制在HX-500E分断机中的应用

简述了HX500E玻璃分断机所以能切割特殊ITO玻璃的设计特点、工作原理及工艺过程,介绍了该机运动机构及控制组成,并以平台伺服的选型为例,介绍了伺服系统电机的选型方法,三菱定位模块FX2N-1PG的使用特点及应用,FX2N-1PG模块在位置控制中利用近点检测法和伺服编码器Z相脉冲组合完成伺服回归机械原点的方法,并指出了一些位置控制原点回归方法注意事项.     

Approximation by light maps and parametric Lelek maps

The class of metrizable spaces M with the following approximation property is introduced and investigated: M∈AP(n,0) if for every ε>0 and a map g:In→M there exists a 0-dimensional map g^′:In→M which is ε-homotopic to g. It is shown that this class has very nice properties. For example, if Mi∈AP(ni,0), i=1,2, then M₁×M₂∈AP(n₁+n₂,0). Moreover, M∈AP(n,0) if and only if each point of M has a local base of neighborhoods U with U∈AP(n,0). Using the properties of AP(n,0)-spaces, we generalize some results of Levin and Kato-Matsuhashi concerning the existence of residual sets of n-dimensional Lelek maps.     

零维理想关于变元正常与一般位置

设k[x_1,…,x_n]是域k上关于变量x_1,…,x_n的多项式环,I是k[x_1,x_2,…,x_n]中的零维理想.本文对I关于某个变元x_i正常与一般位置之同的关系进行探讨,并证明了零维理想对于变元x_i正常与一般位置在某种情况下的等价性.     

基于束流位置探测器的束团长度测量

分析了驱动电子束团的频域特性,研究了基于该特性进行长度测量的理论基础;使用三维模拟软件对束流位置探测器(BPM)进行建模,用模拟的方法对传输阻抗进行了数值计算;对不同长度的束团进行了测量和计算,并且分析了束团位置在真空管道中偏移对束团长度测量的影响。由测量结果可见,电子束团长度在10~100 ps(3~30 mm)时,测量误差均小于2%,满足中国工程物理研究院高平均功率自由电子激光太赫兹实验测量的使用要求。