New 3-mode bosonic operator realization of SU（2） Lie algebra： From the point of view of squeezing

We consider the quantum mechanical SU(2) transformation e2λ JzJ± e-2λJz= e±2λJ± as if the meaning of squeezing with e±2λbeing squeezing parameter. By studying SU(2) operators(J±,Jz) from the point of view of squeezing we find that(J±,Jz) can also be realized in terms of 3-mode bosonic operators. Employing this realization, we find the natural representation(the eigenvectors of J+ or J-) of the 3-mode squeezing operator e2λ Jz. The idea of considering quantum SU(2) transformation as if squeezing is liable for us to obtain the new bosonic operator realization of SU(2) and new squeezing operators.     

催化动力学荧光法测定中草药对羟基自由基的清除率

苯甲酸具有很弱的荧光,在Co2+的催化下,过氧化氢能氧化苯甲酸发出强的荧光。中草药提取物可以清除溶液中的·OH, 使产物的生成量减少, 从而使溶液的荧光增加程度降低。据此原理建立了一种测定中草药对羟基自由基清除率的催化动力学荧光新体系。当中草药的浓度为4.0 mg(干重)·mL-1时,测得紫花地丁、苍术和赤芍对羟基自由基的清除率分别为60.8%,40.1%和94.3%。该方法与分光光度法测定结果相比无显著性差异。     

液体的脉冲差分光声喇曼光谱

采用脉冲光声方法测量了各种有机和无机液体的受激喇曼光谱,探讨了影响这种光谱技术灵敏度的主要原因,即来自线性吸收信号的干扰,并进一步采用一种改进的方法——差分方法,消除了线性光声信号的影响,可以测量到比较弱的喇曼谱线以及浓度比较低的物质的喇曼光谱,并探讨了这种技术在痕量物质测量以及探测环境污染物质等领域中的应用前景.     

一种基于多准则决策和PSO-LM混合优化算法的多峰Brillouin散射谱的特征提取方法

采用传统方法对多峰Brillouin散射谱进行拟合的过程中,通常是以谱线最大功率点为基准的,却忽略了其他比该点小但却是极值的功率点。这样获得的拟合曲线通常只有一个峰值,相当于把除最高峰之外还有多个小峰的多峰Brillouin散射谱进行了简化,导致大量有用信息的丢失。为了提高Brillouin散射谱的特征提取精度,提出了一种基于MCDM和PSO-LM混合优化算法的多峰Brillouin散射谱特征提取方法(MCDM-PSO-LM)。MCDM可以识别和准确定位多峰Brillouin散射谱的各个波峰和波谷;PSO-LM混合优化算法可以实现分别对各个波峰和波谷的曲线进行拟合并找到每一个波峰的中心频率,该算法既克服了PSO算法过早收敛于局部极值和LM算法依赖初值的问题,又可以将PSO算法的全局搜索能力和LM算法的局部收敛能力结合在一起。较传统算法而言,MCDM-PSO-LM算法保证了对最优值求解的速度和精度,提高了运算能力,使解析解最大限度地接近最优值。分别在不同信噪比和不同线宽条件下进行仿真验证,频移和温度误差分析结果表明,MCDM-PSO-LM方法可以对多峰Brillouin散射谱的各个波峰与波谷进行准确定位,可用于多峰Brillouin散射谱的特征提取,识别效果明显强于传统算法,提高了信息分析的准确性。     

3,4-噻吩二羧酸、1,10-邻菲罗啉与稀土配合物的荧光性质及对硝基苯的检测

3,4-噻吩二羧酸(3,4-H₂tdc),1,10-邻菲罗啉(phen)和稀土硝酸盐经水热法合成三种配合物Ln₂(Htdc)₂(tdc)₂(phen)₂(H₂O)₄(Ln=Eu 1, Gd 2, Tb 3),并用X-射线单晶衍射分析方法测定了配合物1-3晶体结构,配合物1-3为双核分子。每个金属离子周围有2个3,4-tdc,1个3,4-Htdc,1个phen和2个配位水分子,配位数为9。配合物1和3在紫外灯下显强红光和绿光,其荧光发射光谱,在619和545 nm出现最大发射峰,分别对应于Eu(Ⅲ)离子的5D₀→7F₂和Tb(Ⅲ)离子的5D₄→7F₅跃迁。配合物2在425 nm观察到来自基于配体的π*→π最大发射峰。不同溶剂分子对配合物1荧光有不同程度的影响,基于荧光猝灭机理,配合物1具有选择性检测硝基苯污染物的能力。     

Linearization of Systems of Nonlinear Diffusion Equations

We investigate the linearization of systems of n-component nonlinear diffusion equations; such systems have physical applications in soil science, mathematical biology and invariant curve flows. Equivalence transformations of their auxiliary systems are used to identify the systems that can be linearized. We also provide several examples of systems with two-component equations, and show how to linearize them by nonlocal mappings.     

一种实现显微荧光寿命图的测量方法

将脉宽120fs、重复率76MHz激光引入激光扫描显微镜的激发光路,利用其扫描系统对荧光标记样品激发扫描,将激发出的荧光从荧光探测光路引入备用的外部探测口;在探测口接一快速光电倍增管,将光电倍增管的信号送给时间相关单光子计数器,获得时间相关的荧光强度图;最后通过计算机处理获得荧光寿命图。应用此系统对青色荧光蛋白(CFP)、黄色荧光蛋白(YFP)荧光寿命进行了测量,并应用CFP、YFP实现荧光共振能量转移的测量。通过实验看出利用已有的激光扫描显微镜,配合较先进的寿命测量方法,可以很好地实现显微荧光寿命图的测量。     

Extended Group Foliation Method and Functional Separation of Variables to Nonlinear Wave Equations

Generalized functional separation of variables to nonlinear evolution equations is studied in terms of the extended group foliation method, which is based on the Lie point symmetry method. The approach is applied to nonlinear wave equations with variable speed and external force. A complete classification for the wave equation which admits functional separable solutions is presented. Some known results can be recovered by this approach.     

GaAs基GaAsSb/GaInAs双层量子阱的发光

嵌入GaAs中的GaAsSb／GaInAs量子阱因其在1．3～1．5μm光通信波段发光的潜力而受到关注,我们研究了一系列MBE生长的GaAsSb／GaInAs量子阱样品的光致发光,发现所有样品在室温下都出现了一个较强的、波长在1．3μm附近的低能峰和一个较弱的高能峰。变温及变激发功率的荧光谱测量研究发现,高能峰只有在150K以上的测试条件下才能观测到,并且其相对强度随着温度的升高而增加,其调制光谱显示出第一类跃迁的特征。他们建立了理论模型,计算的结果支持将这一发光峰指派为GaInAs层内电子的基态与重空穴激发态间的跃迁,并与实验数据吻合得很好。同时初步讨论了改善1．3μm的低能峰发光的方法。     

Effect of Temperature on Polaron Stability in a One-Dimensional Organic Lattice

Effect of temperature on the polaron stability in a one-dimensional organic lattice is investigated within the Su-Schrieffer-Heeger model. The temperature effect is simulated by introducing random forces to the equation of the lattice motion. It is found that the localized polaron state becomes delocalized even at low temperatures. The time of polaron keeping localized depends on the magnitude of temperatures. By taking into account the thermal effect, we find that the dissociation field is weaker as compared with earlier works.