纳米铂颗粒的控制生长

利用吸氢再还原法,进行逐步还原反应,合成了一系列大小的铂纳米颗粒;透射电镜和X光衍射分析表征的结果表明,铂颗粒是逐步长大的,经过32次生长,铂颗粒的平均粒径从1.8nm增加到14.1nm,平均增加步长约为0.4nm,且粒子均具较好的单分散性.     

Solar Neutrino Oscillation Parameters after SNO Phase-Ⅲ and SAGE Part-Ⅲ

We analyse the recently published results from solar neutrino experiments SNO Phase-Ⅲ and SAGE Part-Ⅲ and show their constraints on solar neutrino oscillation parameters, especially for the mixing angle θ12. Through a global analysis using all existing data from SK, SNO, Ga＆Cl radiochemieal experiments and long base fine reactor experiment KamLAND, we obtain the parameters △m12^2= 7.684 -0.208^＋0.212×10^-5 eV^2, tan^2 θ12=0.440-0.057^＋0.059. also find that the discrepancy between the KamLAND and solar neutrino results can be reduced by choosing a small non-zero value for the mixing angle θ13.     

双波前校正器全光路像差校正自适应光学系统像差解耦分析

分析了双波前校正器全光路像差校正自适应光学系统的工作原理,并通过共模波前传感器中的两套波前传感器探测得到的波前信息进行数据差分融合,按照优化理论推导了两套波前校正器需要校正的像差公式.根据此像差公式,仿真分析了以两套61单元变形反射镜组成的双波前校正器全光路像差校正自适应光学系统的校正能力,并与单套波前校正器全光路像差校正自适应光学系统的校正能力进行了比较,结果验证了推导的像差公式的正确性,也说明了两套波前校止器不仅可以解耦,而且其校正效果与理想行程单套波前校正器全光路像差校正自适应光学系统的校正效果相当.     

Ca9R(VO4)7 : Eu3+ 发光粉的发光特性

采用高温固相法制备了Eu³⁺离子激活的Ca₉R(VO₄)₇(R = Y, La, Gd)红色发光粉,并利用荧光光谱对发光粉的特性进行研究。激发光谱中,Ca₉Y(VO₄)₇ : Eu³⁺ , Ca₉La(VO₄)₇ : Eu³⁺和Ca₉Gd(VO₄)₇ : Eu³⁺都有两个宽的VO^3-₄激发带和Eu³⁺的特征激发峰。发射光谱中,在Ca₉Y(VO₄)₇ : Eu³⁺ 和Ca₉La(VO₄)₇ : Eu³⁺中的350~550 nm范围内出现VO^3-₄的发射带,而在Ca₉Gd(VO₄)₇ : Eu³⁺中却没有观察到VO^3-₄的发射。在这三种发光粉中,Ca₉Gd(VO₄)₇ : Eu³⁺的发光强度远远高于其它两种,这是由于Gd³⁺的存在有效地使能量通过Gd³⁺ →VO^3-₄ → Eu³⁺及Gd³⁺ → Eu³⁺的两种方式进行能量传递,从而提高了Eu³⁺发光效率。     

Wavefront analysis for plenoptic camera imaging

The plenoptic camera is a single lens stereo camera which can retrieve the direction of light rays while detecting their intensity distribution. In this paper, to reveal more truths of plenoptic camera imaging, we present the wavefront analysis for the plenoptic camera imaging from the angle of physical optics but not from the ray tracing model of geometric optics.Specifically, the wavefront imaging model of a plenoptic camera is analyzed and simulated by scalar diffraction theory and the depth estimation is redescribed based on physical optics. We simulate a set of raw plenoptic images of an object scene, thereby validating the analysis and derivations and the difference between the imaging analysis methods based on geometric optics and physical optics are also shown in simulations.     

无阀微泵腔内气泡对周期驱动压力的影响

气泡的存在使无阀微泵的工作性能和使用寿命大大降低, 甚至无法正常工作. 为了合理地预测无阀微泵腔内气泡对周期驱动压力的影响, 给出了用来描述收缩管/扩张管型无阀压电微泵的数学模型, 包括泵腔体积变化、连续性方程、流体有效体积弹性模量以及锥管阻力系数的计算. 同时, 分析了腔内不同气泡体积对无阀微泵周期驱动压力的影响, 并对两个气泡进入无阀微泵泵腔时压力脉动过程进行了仿真和试验研究. 通过仿真结果与试验数据的比较表明, 所提出的存在气泡时无阀微泵数学模型及仿真方法是合理的. 关键词： 无阀微泵 气泡 压力脉动     

电路参数宽范围变化时电流控制开关变换器的动力学研究

以电流控制Buck—Boost变换器为例,通过对输入电压和负载电阻等电路参数宽范围变化时开关变换器的开关状态的完整描述,导出了电流控制开关变换器的两个电感电流边界,建立了它的精确离散时间模型,并利用分段线性模型验证了离散时间模型的正确性．基于离散时间模型,揭示了开关变换器存在周期分岔、边界碰撞分岔、鲁棒混沌和阵发混沌等复杂动力学行为;通过推演Jacobi矩阵,给出了电路参数变化时最大Lyapunov指数和特征值的运动轨迹;并采用参数空间映射图,由电路参数域对开关变换器的工作状态域进行了估计．最后进行了电路实验制作,实验观察结果与理论分析结果～致．本文系统研究了开关变换器的动力学理论,其分析方法和研究结果对开关变换器的设计及控制都具有重要的指导意义．     

正支共焦非稳腔的离焦像差特性

 正支共焦非稳腔在出光过程中易受环境扰动而造成腔长失调,易受热积累影响而使腔镜变形,从而使输出光束产生离焦像差和部分其它像差。为了实现对离焦像差的校正,针对不同的产生原因,提出了2种离焦像差特性分析方法：一为腔镜相对位置失调引起的离焦像差特性理论分析方法,它是另一种分析方法的基础;二为腔镜变形引起的等效腔长变化导致的离焦像差特性分析方法,它是实际激光器中的主要分析方法。得到了离焦像差与腔长的特性关系和离焦像差与腔镜变形量之间的特性关系。研究表明：腔长改变和腔镜变形对离焦像差的影响本质是一样的,都是改变了谐振腔的共焦点位置;腔长改变或腔镜矢高变化与离焦像差都成近似的线性关系。实验验证了离焦像差特性分析方法的有效性,最后指出离焦像差特性可作为激光器中离焦像差动态补偿的有效依据。     

The determination of the x value in doped Hg1-xCdxTe by transmission spectra

Variable-temperature transmission/absorption spectra are measured on As-doped Hg 1 x Cd x Te grown by molecular beam epitaxy.The nonlinear temperature-dependent shift of the absorption edge is also observed,which is similar to our previous report on V Hg (unintentionally)-doped HgCdTe.By referring to the empirical formulas of E g (x,T),the x value of the epilayer is calculated and its inconsistency between the extreme temperatures (e.g.10 and 300 K) is discussed.The results confirm the assumption of the effect of shallow levels on the shift of the absorption edge,and suggest that the x value (or E g) in intrinsic/extrinsic-doped HgCdTe should be determined by referring to as low a temperature as possible (e.g.10 K),and not the commonly used temperatures of 77 or 300 K,when the transmission spectrum should be employed.This can give brief guidelines for fabricating HgCdTe-related devices.     

The determination of the x value in doped Hg1-xCdxTe by transmission spectra

Variable-temperature transmission/absorption spectra are measured on As-doped Hg_1-xCd_xTe grown by molecular beam epitaxy. The nonlinear temperature-dependent shift of the absorption edge is also observed, which is similar to our previous report on V_textrmHg (unintentionally)-doped HgCdTe. By referring to the empirical formulas of E_g(x, T), the x value of the epilayer is calculated and its inconsistency between the extreme temperatures (e.g. 10 and 300 K) is discussed. The results confirm the assumption of the effect of shallow levels on the shift of the absorption edge, and suggest that the x value (or E_g) in intrinsic/extrinsic-doped HgCdTe should be determined by referring to as low a temperature as possible (e.g. 10 K), and not the commonly used temperatures of 77 or 300 K, when the transmission spectrum should be employed. This can give brief guidelines for fabricating HgCdTe-related devices.