CdSe/ZnSe自组装量子点中非线性系数随着温度的规律性变化(英文)

研究了在CdSe/ZnSe自组装量子点中CdSe量子点的发光随着激发光强度变化的特性。发现当激发强度(I)变化3个数量级的时候,量子点发光的峰位、峰形都没有发生明显的变化。通过公式L∝Ik(其中I是激发光强度,L是量子点发光强度,k是非线性系数)得到非线性系数k值。实验结果表明:在温度由21 K升高到300 K的过程中,k值随温度变化可以分为3个区域:当温度低于120 K时,k值接近于1;然后,随着温度升高,k值慢慢变小;最后,随温度进一步升高,k值由200 K时的0.946迅速减少到0.870。结合发光随温度变化的实验结果,确认在120 K以下发光主要来源于束缚激子复合。在温度由200 K升高到300 K的过程中,非线性系数的单调减小主要归因于随着温度的升高,发光部分来自于由自由电子或空穴到束缚态能级(FB)的复合。进一步通过分析量子点发光的积分强度随着温度的变化的实验结果,发现发光强度随温度升高而减弱的主要原因是材料中的缺陷或者位错等提供非辐射渠道。     

载气汽油在水平螺旋扁管管束中的沸腾换热

以汽油-空气为介质,在不凝性气体质量含量不超过5%时,对导程为200mm的螺旋扁管管束中的沸腾换热进行了实验研究,分析了沸腾换热系数随两相质量流量的变化规律以及流动压降随空气流量的变化规律。得到了相应条件下,载气汽油在该导程的螺旋扁管管束中的沸腾换热实验关联式。     

光谱成像检测法鉴别中药材

使用基于液晶可调谐滤光器的光谱成像检测系统,对西洋参及市面上常用做假冒西洋参的伪品桔梗进行了在体检测.该系统能对检品进行连续光谱成像,光谱分辨率可达0.5 nm,配合使用Matlab软件对图像信号进行处理和分析.获取了400 nm～680 nm之间的连续荧光光谱图像,通过对比西洋参、桔梗的特征光谱曲线,及进行相关系数的计算,有效地区分了西洋参及桔梗.为西洋参的真伪鉴别提供了一定的帮助.     

伽马射线吸收系数测量方法的研究

利用γ射线穿过物质时强度遵从指数衰减规律,选取不同的吸收材料进行γ射线吸收系数的测量,结果准确可靠,从而验证了实验室开设γ射线吸收系数测量实验方案的可行性。     

不良导体导热系数的测量与探讨

根据利用物体散热速率求传热速率的实验思想,给出了橡胶盘导热系数的实验结果。并对散热速率做了分析,给出了一个修正方案。     

利用反射与透射光谱测量GaN外延层的光学参数

GaN是一种理想的紫外发光和探测材料,其光学特性参数是光学器件设计的重要依据。采用紫外反射与透射光谱相结合的方法对国产GaN外延层进行光学特性测量,利用反射率与折射率之间的关系和薄膜干涉效应,建立了GaN外延层厚度、表面反射率、光谱吸收系数的光谱测量公式。测量结果表明,GaN外延层在紫外波段存在三个吸收区,其中364nm以下波段为强吸收区,吸收系数接近10^5cm^-1,364～375nm为吸收过渡区,375nm以上波段为弱吸收区;GaN表面反射率在三个吸收区的变化不大,为0．2～0．25之间。     

多级轴流压气机稳定性数值研究

本文以某压气机前五级为研究对象,利用计算流体力学方法研究了可转静叶对提高压气机部分转速下喘振裕度的效果,研究表明,可转静叶能够明显地提高压气机部分转速下的喘振裕度。通过分析影响压气机不稳定性的因素,给出了一个扩压参数来衡量压气机稳定性和承载能力,从而指导选取最优可转静叶安装角,使压气机喘振裕度达到最大,并在该参数的指导下,得出了可转静叶的一组最优安装角。     

Effect of heat treatment on the magnetic and magnetoelastic properties of cobalt ferrite

The influence of different heat treatments on the magnetic and magnetoelastic properties of highly magnetostrictive CoFe₂O₄ has been investigated. The first order cubic anisotropy coefficient, coercive field, magnetostriction and high strain sensitivity were observed to decrease as the heat treatment temperature increased. The saturation magnetization of the samples on the other hand increased with increase in heat treatment temperature. These changes were not accompanied by any observable changes in crystal structure or composition and are indicative of migration of Co²⁺ from the octahedral sites (B-sites) to the tetrahedral sites (A-sites) and Fe³⁺ from the A-sites to the B-sites of the spinel structure. Different distributions of the cations at the two distinct lattice sites can strongly affect the magnetic and magnetoelastic properties of these materials.     

Study of asymmetric wavenumber shift of the Fermi doublet ν1 − 2ν2 in the Raman spectrum of liquid carbon disulfide

The Raman spectra of liquid carbon disulfide (CS₂) diluted with benzene (C₆H₆) have been measured. By changing the CS₂, the concentration, we found an asymmetric wavenumber shift phenomenon. With decreasing concentration of CS₂, the position of the ν₁ (655 cm⁻¹) band remains practically unchanged, and the 2ν₂ (796 cm⁻¹) band shifts toward higher wavenumbers. To interpret this asymmetric wavenumber shift phenomenon of the Fermi doublet ν₁ − 2ν₂ in the Raman spectra satisfactorily, we propose a modified Bertran model. The values of the Fermi resonance (FR) parameters of CS₂ at different concentrations were calculated using the Bertran equations. In addition, we found the fundamental ν₂, which should be independent of the FR interaction, shifted to higher wavenumbers as the concentration decreased. This shift was probably driven by the tuning of the FR. Copyright © 2009 John Wiley & Sons, Ltd.     

Numerical method for solving matrix coefficient elliptic equation with sharp-edged interfaces

Solving elliptic equations with sharp-edged interfaces is a challenging problem for most existing methods, especially when the solution is highly oscillatory. Nonetheless, it has wide applications in engineering and science. An accurate and efficient method is desired. We propose an efficient non-traditional finite element method with non-body-fitting grids to solve the matrix coefficient elliptic equations with sharp-edged interfaces. Extensive numerical experiments show that this method is second order accurate in the L^∞ norm and that it can handle both sharp-edged interface and oscillatory solutions.