ON LOCALIZATION IN DISORDERED ELECTRON SYSTEMS

The field theory of Anderson localization of disordered electron systems is formulated in the framework of closed time path Green's functions (CTPGF). The properties of the mobility edge are studied by the renormalization group method and the density of states is found to be zero at the mobility edge.     

土槿皮酸类化合物的质谱研究

本文系统地研究了土槿皮甲酸、乙酸和丙酸及其衍生物的质谱.通过质谱-结构关系的分析、高分辨质谱及亚稳数据的测定,阐明了它们在电子轰击下的裂解反应机制.     

SEEKING FOR THE U(5) LIMITING CASE OF IBA-Ⅱ

In the region of even-even nuclei from A=96 to A=120, only the energy spectrum of ¹¹⁰₄₈Cd₆₂ may be described by IBA-Ⅱ involving the states {N_π +N _L -1,1}. But it can be described by IBA-Ⅰ too. To distinguish these two schemes, more angular momentum measurement is needed.     

非齐次聚合分解过程的对偶性

文章研究了格子点上带扩散的非齐次聚合分解过程(HCFP)的对偶性, 给出了HCFP的平稳分布和HCFP 的积分形式的BBGKY hierarchy.     

PbWO4闪烁晶体的辐照损伤机理研究

完成了640—1040℃温度范围内钨酸铅［PbWO₄(PWO)］晶体的退火实验,观察到较低温退火时晶体中本征色心吸收带(350nm)先是增加,其后随退火温度的升高而逐渐降低直至消除的全过程．分析了PWO晶体的本征缺陷和电荷补偿机制．讨论了退火过程中氧进入晶体后色心的产生和转化规律,并提出可能发生Pb³⁺→Pb⁴⁺的进一步氧化过程,从而导致Pb³⁺空穴中心的湮没．测量并比较了不同退火温度处理后PWO晶体的紫外辐照诱导色心     

一系列薯蓣皂甙元-α-L鼠李糖基-(1→2)和(1→4)-β-D葡萄糖甙的1H和13C NMR归属

用同核和异核二维核磁共振方法全归属了一系列合成的薯蓣皂甙元-α-鼠李糖基-β-D葡萄糖甙的¹H和¹³C核磁共振谱线.这些薯蓣葡萄糖甙是薯蓣皂甙元-β-D葡萄糖甙(1),薯蓣皂甙元-α-L鼠李糖基(1→2)-β-D葡萄糖甙(2),薯蓣皂甙元-α-L鼠李糖基(1→4)-β-D葡萄糖甙(3),薯蓣皂甙元[-α-鼠李糖基-(→2)]-α-L鼠李糖基→-(1→4)-β-D葡萄糖甙(4)以及薯蓣皂甙元[-α-L鼠李糖基-(1→2)]-β-D阿拉伯糖基-(1→4)-β-D葡萄糖甙(5).     

一系列薯蓣皂甙元-β-D葡萄糖基-(1→2)和(1→3)-β-D葡萄糖甙的1H和13C NMR归属

用同核和异核二维核磁共振方法全归属了一系列合成的薯蓣皂甙元-β-D葡萄糖甙的¹H和¹³C核磁共振谱线.这些薯蓣葡萄糖甙是薯蓣皂甙元-β-D葡萄糖甙(1),薯蓣皂甙元-β-D葡萄糖基-(1→2)-β-D葡萄糖甙(2),薯蓣皂甙元,-β-D葡萄糖基-(1→3)-β-D葡萄糖甙(3),薯蓣皂甙元[-β-D葡萄糖基-(1→2)-β-D葡萄糖基(1→3)-β-D葡萄糖甙(4)以及薯蓣皂甙无[-α-L鼠李糖基-(1→2)]-β-D葡萄糖基-(1→3)-β-D葡萄糖甙(5).     

红外气体浓度测试仪设计

在实验室条件下采用红外光谱对气体浓度进行定量分析的技术已很成熟,但是,适用野外环境条件下进行气体浓度精密测量的仪器并不多见。本文设计的仪器是文献〔３〕所述的一种便携式红外气体浓度测试仪器的改型,测量范围０－１００％,精度比文献〔３〕所述红外气体浓度测试仪器有所提高,且使用方便,工作稳定,数据可靠。     

TOMOGRAPHY FORMULA FOR BIOCHEMICAL IMAGING OF THIN TISSUE WITH DIFFUSE-PHOTON DENSITY WAVES

Using the transport theory to describe the near infrared light propagating in tissue with finite parallel-plane geometry, and taking the zero-boundary condition, we obtain the analytical expression of average photon density and Green's function incorporating the boundary effects in the homogeneous tissure. Making use of perturbation theory we also obtain the analytical expression of scattered wave induced by the heterogeneity, and present the 2-dimensional spatial transform of scattered wave with respect to transverse coordinate. If the information of heterogeneity on depth and thickness is available, diffraction tomography formula is presented to save the time of image reconstruction; if the information is unknown, we suggest to obtain the inhomogeneous function from the one-dimensional integral equation of 2-dimensional spatial transform of scattered wave applying the direct matrix method or iterative method for image reconstruction. This approach avoids directly solving three-dimensional integral equation of scattered wave. In our proposed approach the strong points of the direct matrix method, iterative method, and diffraction tomography are fully combined.