能动反射镜低频像差补偿能力分析

 采用Algor软件包并利用有限元法对37单元能动反射镜低频误差补偿能力进行了分析计算，确定了镜面厚度8mm，驱动器间距46mm，极头直径12mm等能动反射镜制造的关键参数。通过计算机仿真分析证明，基于这些参数所设计的能动反射镜可以对低频误差进行有效校正，校正精度的均方根值小于等于λ／８，从而可以为能动反射镜的制造提供理论依据。     

自旋为1/2的XY模型亚铁磁棱型链的物性和有序-无序竞争

利用不变本征算符法, 计算低温下自旋为1/2的XY模型一维亚铁磁棱型链系统的元激发谱, 讨论在此系统中不同的特殊情形下的元激发能量, 从而给出体系的三个临界磁场强度的解析解H_C1, H_C2, H_peak. 分析不同外磁场下 体系的磁化强度随温度的变化规律, 发现三个临界磁场强度的解析解H_C1, H_C2, H_peak是正确的, 并从三个元激发对磁化强度的贡献进行了说明. 低温下磁化强度随外磁场的变化呈现1/3磁化平台. 体系的磁化率随温度或者外磁场的变化都出现了双峰现象. 这说明双峰源于二聚体分子内电子自旋平行排列的铁磁交换作 用能和二聚体与单基体分子间电子自旋反平行排列的反铁磁交换作用能, 热无序能, 外磁场强度相关的自旋磁矩势能之间的竞争.     

Er3+在二氧化硅介孔分子筛中的高效率发光及其分析

研究了一种新型的负载Er3 的二氧化硅介孔分子筛纳米材料,分析了其在有无功能化试剂全氟甲基磺酰(bis(perfluoromethylsulfonyl)amine)修饰作用下的吸收和荧光光谱特性,获得了高强度的荧光发射.应用Judd-OfelI理论计算了强度参数(Ω2=1.88×10-20,Ω4=5.45×10-20 cm2,Ω6=3.11×1O-20cm2)、跃迁振子强度、自发跃迁概率、能级辐射寿命等重要的光谱参数,讨论了吸收和发射跃迁截面(Ωem=10.9×10-21 cm2),研究了在介孔分子筛纳米材料中的Er3 在不同的抽运功率条件下的荧光强度变化情况.比较了Er3 在不同基质材料中的带宽特性.研究表明二氧化硅介孔分子筛有利于实现高效率的激光输出或具有较宽带宽的高增益光放大,能够成为掺铒激光器或光放大器的新型基质材料.     

大功率LED脉冲位置调制解调设计

脉冲位置调制是室内可见光通信的主要调制方式之一,它具有功率利用率高,频带利用率好,抗干扰性强的特点.为实现室内大功率白光LED照明通信,在分析PPM的原理基础上提出了一种改进的调制方式,给出了这种PPM符号的结构,并设计了大功率LED的驱动电路.其主要特点是由单片机直接输出帧同步信号加PPM信号,不设置保护时隙,其利用...     

n模耦合谐振子量子系统的精确波函数

利用不变本征算符法研究了n模耦合谐振子量子系统的简正频率及其对应的简正坐标与共轭动量,并对系统的哈密顿量进行了退耦合,得到了系统的明显的简正频率解析解.推导出坐标表象中系统的精确波函数的解析解.并对不同情形的耦合系数进行了讨论,认识到n模动量耦合谐振子体系和n模坐标耦合谐振子体系是本文所研究的体系的特例.     

傅里叶变换近红外反射用于鸡蛋蛋品质的研究

鸡蛋的无损检测技术一直以来都是蛋品质检测领域的重要研究课题,建立相应的检测技术对蛋鸡育种和蛋品质监测具有实际意义.文章利用近红外光谱仪测定保存时间不同的鸡蛋,探讨了蛋白高度、哈氏单位、气室直径、气室高度近红外模型的可行性,并运用无偏最小二乘法建立了鸡蛋蛋白高度、鸡蛋气室直径、气室高度的近红外测定模型,蛋白高度、气室直径与气室高度的测定模型的决定系数R2分别为0.867,0.821,0.865,RMSECV分别为0.476,0.014与0.479.对33个鸡蛋样品的模型验证的R2分别为0.873,0.861,0.895.鸡蛋新鲜度主要指标的预测值与实际值间的差异不显著(P＞0.05),所建模型具有较好的准确性与预测能力,能够满足蛋品新鲜度快速无损检测的要求.     

Large magnetoresistance in metamagnetic CoMnSi0.88Ge0.12 alloy

The magneto-transport properties are investigated in metamagnetic CoMnSi0.88Ge0.12 alloy.By applying a magnetic field or increasing temperature,a metamagnetic phase transition from antiferromagnetic to ferromagnetic is observed in this alloy.Around the metamagnetic phase transition,CoMnSi0.88Ge0.12 alloy exhibits a large and negative magnetoresistance effect(～32%) under a magnetic field of 20 kOe(1 Oe = 79.5775 A/m),which is ascribed to the spin-dependent scattering of conduction electrons.     

基于引导滤波和核相关滤波的红外弱小目标跟踪

为了解决传统跟踪算法不能有效区分背景边缘和红外弱小目标的问题,基于图像引导滤波和核相关滤波,提出了一种改进型的红外弱小目标跟踪算法。将采用6组红外弱小目标图像序列得到的实验结果与采用经典跟踪算法得到的实验结果进行了比较。实验结果表明,所提算法在主观视觉和客观评价指标方面均优于传统算法,具有更高的目标跟踪精度与较好的实时性。     

Investigation of magnetization reversal process in pinned CoFeB thin film by in-situ Lorentz TEM

Exchange bias effect has been widely employed for various magnetic devices.The experimentally reported magnitude of exchange bias field is often smaller than that predicted theoretically,which is considered to be due to the partly pinned spins of ferromagnetic layer by antiferromagnetic layer.However,mapping the distribution of pinned spins is challenging.In this work,we directly image the reverse domain nucleation and domain wall movement process in the exchange biased Co Fe B/Ir Mn bilayers by Lorentz transmission electron microscopy.From the in-situ experiments,we obtain the distribution mapping of the pinning strength,showing that only 1/6 of the ferromagnetic layer at the interface is strongly pinned by the antiferromagnetic layer.Our results prove the existence of an inhomogeneous pinning effect in exchange bias systems.     

Possible Martensitic Transformation in Heusler Alloy Pt_2MnSn from First Principles

Using density functional theory calculations, we investigate the tetragonal distortion, electronic structure and magnetic property of Pt_2 Mn Sn. The results indicate that, when the volume-conserving tetragonal distortion occurs, the energy minimum appears at c/a(6 = 0.84, and the energy difference between the minimum and cubic phase is as high as 107 me V/f.u. Thus from the point of view of thermodynamics, martensitic transformation may occur in Pt_2 Mn Sn with decreasing the temperature. The electronic structure of its cubic and martensitic phases also approves this. Moreover, both the cubic and tetragonal phases of Pt_2 Mn Sn are ferromagnetic structures and their total magnetic moments are 4.26 μ_B and 4.12 μ_B, respectively.