基于电吸收调制器的高速时钟信号的提取

对高速光时分复用系统中(2×10 Gb/s)基于电吸收调制器(EAM)的注入光电混合振荡器的时钟提取方法进行了实验验证. 实验证明,光电混合振荡器必须保证一定的增益才能提取出时钟,在此基础上,无论光电混合振荡器内或外的光功率的增加,将增加提取时钟的幅度,减小提取时钟的时间抖动.当偏置电压一定时,射频幅度增加,则电吸收调制器的窗口变窄,提取时钟幅度增大,抖动减小.     

玻恩近似下电子与离子碰撞的多组态计算

研究电子与离子碰撞激发过程,在波恩近似下,用多组态平面波与多组态库仑波方法计算振子强度与碰撞强度,并且编制了相应程序MCPBA(九)和MCCBX(九)。以四个组态、27个能级的类Ne-锗为例,从基态开始激发。用MCPBA(九)计算了13个包含直接碰撞的过程。用MCCBX(九)给出了全部26个交换效应的碰撞强度。考虑了不同离子波函数对碰撞强度的影响。还与国外扭曲波计算数据进行了比较。结果表明,对某些激发过程必须进行多组态计算,改进离子波函数的计算甚至比改进碰撞电子波函数更为重要。     

孔耦合自由电子激光振荡器光场横向结构特性

 孔耦合输出对自由电子激光(FEL)振荡器腔内光场的横向结构有很大的影响, 在输出镜上横模之间发生很复杂的耦合转换。基于中物院远红外自由电子激光振荡器, 研究了 孔输出波导 FEL的数值模拟, 对孔耦合及其引起的腔内光场的变化给以特别的注意, 依据数 值结果, 分析了孔耦合FEL光场横向结构的特性。     

光系统ⅡChl分子能量传递超快光谱动力学

利用ICCD飞秒扫描成象和飞秒时间分辨光谱装置实验研究了高等植物捕光天线LHCⅡ三聚体和PSⅡ颗粒复合物的超快光谱动力学,经过吸收光谱和发射光谱分析,确定在LHCⅡ三聚体中至少存在7种Chl分子光谱特性,分别是Chlb_653/656^658.7、Chla_662.0^665.2、Chla/b_670/671^677.1、Chla_675.0^677.1、Chla_680/681^682.9、Chla_685.0^689.1和Chla_695.0^695.6.采用光强1013光子/cm²/脉冲激励浓度为30μg/mL的捕光天线LHCⅡ三聚体,在650nm到705nm谱段逐点探测分析处理,产生了2组短寿命组分210fs、520fs和5.2ps、36.7ps及2个长寿命组分1.8ns、2ns.最快的3个寿命210fs、520fs和5.2ps反映了三聚体Chlb分子向Chla分子的激发能传递过程;寿命36.7ps反映了Chla分子向相邻单体Chla分子的激发能传递过程;最长的2个寿命1.8ns和2ns是在三聚体中Chla分子通过中间体Chla分子辐射荧光,分别跃迁回基态的过程.获得的6个寿命组分有把激发能传递时间与Chla/b分子发射光谱相结合的特点.经拟合处理解析PSⅡ颗粒复合物光谱,得到3个组分谱,其峰值分别为686.8nm、692.2nm和694.9nm,与LHCⅡ比较分析,说明天然构型的PSⅡ有很强的吸收光能和有效传递光能的本领.     

有优先权的光突发交换中光缓存的性能分析

分析了配置有限数量光纤时延线(FDLs)和优先权机制的光突发交换(pOBS)网络性能,建立了pOBS的网络模型和排队模型;并以模型为基础,比较了各级别数据包的排队等延时与FDLs单位、负荷强度比例的关系;比较了有和无FDLs时,包丢失率与FDLs单位、FDLs深度、系统负荷强度以及波长数的关系.研究发现;高优先级数据包的平均延时远小于其它数据包,负荷强度越大平均延时也越大,高优先级数据包的比例越大则低优先级数据包的延时越大且丢失率越高,加入有限数量和适当深度的FDLs、减小FDLs最小单位、增加波长数都能减小数据包的平均排队延时和丢失率.     

Cyclam Modified Carbon Paste Electrode as a Potentiometric Sensor For Determination of Cobalt （Ⅱ） Ions

IntroductionThe increasing use ofion sensors in the filed ofenviromental,agricultural and medicinal analysesis simulating analytical chemists to develop newsensors for the fast,accurate,reproducible and se-lective determination ofvarious species[1] .Cobaltisa biologically essential trace element.Althoughcobalt is required only in minute amounts for main-taining normal health,a lower or higher concentra-tion of it may lead to deficiency or toxicity states,respectively,resulting in impairmentor …     

圆柱坐标系下生物组织中激光传输的七流模拟

提出了圆柱坐标系下生物组织中激光传输的七流模型,根据此模型进行的计算结果与直角坐标系下七流模型的计算结果比较,二者吻合较好.在此基础上,研究了组织光学性质对激光在组织内传输过程的影响,结果表明:散射效应使入射激光分布到更大的组织范围内,并使激光的穿透率降低,但其影响是有限的,即当散射系数增大到一定程度后,组织内的激光能量分布就不再有明显的变化.相对而言,吸收系数对组织内激光能量分布的影响比散射系数要大,各向异性系数增大使组织内的散射趋于前向散射,激光能量分布也更深入组织内部.     

Blow up problem for Landau-Lifshitz equations in two dimensions

In 1986, Zhou and Guo in [1] proved the global existence of weak solution for generalized Landau-Lifshitz equations without Gilbert term in multi-dimensions. They consider thehomogeneous boundary problemwith the initial value conditionfor the system of ferromagnetic chain with several variableswhere j(x, t, Z) is a given 3-dimensional vector funC-non in x e R", t E R+, Z e R', W(x)is a given 3-dimensional initial value function on fi, fi is a bounded domain in n-dimensionalEuclidean space…     

Production of single-walled carbon nanotubes from methane over Co-Mo/MgO nanocatalyst:A comparative study of fixed and fluidized bed reactors

In this study,the performances of fixed and fluidized bed reactors in the production of single-walled carbon nanotubes(SWNTs)have been investigated.In both reactors,single-walled carbon nanotubes were grown by catalytic chemical vapor decomposition(CCVD)of methane over Co-Mo/MgO nanocatalyst under two different operating conditions.The synthesized samples were characterized by TEM,TGA and Raman spectroscopy.It is found that the performance of a fluidized bed in the synthesis of carbon nanotubes is much better than that of a fixed bed.The quality of carbon nanotubes obtained from the fluidized bed was significantly higher than that from the fixed bed and the former one with the ID/IG ratio of 0.11 while the latter one with the ID/IG ratio of 0.71.Also,the yield of SWNTs in the fluidized bed was 92 wt%,while it was 78 wt%in the fixed bed.These advantages of fluidized bed reactors for the synthesis of carbon nanotubes can be attributed to more available space for the growth of carbon nanotubes and more uniform temperature and concentration profiles.