Prediction and suppression of strong dispersive coupling in microracetrack channel drop filters

For a four-port microracetrack channel drop filter, unexpected transmission characteristics due to strong dispersive coupling are demonstrated by the light tunneling between the input-output waveguides and the resonator, where a large dropping transmission at off-resonance wavelengths is observed by finite-difference time-domain simulation. It causes a severe decline of the extinction ratio and finesse. An appropriate decrease of the coupling strength is found to suppress the dispersive coupling and greately increase the extinction ratio and finesse, a decreased coupling strength can be realized by the application of an asymmetrical coupling waveguide structure. In addition, the profile of the coupling dispersion in the transmission spectra can be predicted based on a coupled mode theory analysis of an equivalent system consisting of two coupling straight waveguides. The effects of structure parameters on the transmission spectra obtained by this method agree well with the numerical results. It is useful to avoid the strong dispersive coupling region in the filter design. (c) 2007 Optical Society of America.

稀土铁双核配合物的合成

本文通过LnCl_3·nTHF和[C_5H_4(SiMe_3)]Na反应得到了两类配合物[C_5H_4(SiMe_3)] LnCl_2·nTHF (Ln = Nd，Sm，Gd；n = 0，1，2)、[C_5H_4(SiMe_3)] LnCl_2·HCl·nTHF (Ln = Nd，Sm，Gd；n = 1，2)。通过元素分析、红外分析、质谱、核磁共振和热重分析确定了配合物的分子组成，特别是带氯化氢的产品在红外光谱中有1250 cm~(-1)，835 cm~(-1)，748 cm~(-1)自的三甲基硅基特征吸收峰。对氯化稀上进行了结构分析，结果发现LnCl_3·4THF (Ln = Sm，Gd)是与NdCl_3·4THF之间存在着变态关系。GdCl_3·4THF。晶体属单斜晶系，空间群为P21/C，晶胞参数为a = 30.765(7)，b = 8.219(3)，C = 17.534(3)A~·，β = 93.71(2)°；SmCl_3·4THF。晶体属单斜晶系，空间群为P21/C，晶胞参数为a = 30.921(13)，b = 8.287(7)，C = 17.665(8)，β = 94.17(4)°。LnCl_3·4THF的单位晶胞中存在着八个分子，每对分子互相等同，但每对分子内部两个分子之间互不等同。SmCl_3·2THF·DME晶体属单斜晶系，空间群为P21/a，晶胞参数为a = 13.547(8)，b = 8.607(4)，C = 16.029(9)A°，β = 90.53(5)°。铲原子与三个氯原子。两个四氢呋喃中的氧原子以及DME中的两个氧原子键合，形成七配位的配合物，但是配位多面体不是理想的五角双锥，而是形成了比五角双锥(D_(5h))对称性更低的多面体(C_(3v))。它能看作是在正八面体的一个面的中心加上第七个原子的结果，而且这八面体主要受到决定上述那个面的三个原子伸展开的畸变。在制备C_5H_5SiMe_3时，如果不用减压蒸馏，而在常压下直接蒸馏，则得到的不是C_5H_5SiMe_3而是它的二聚体(C_5H_5SiMe_3)_2。用红外光谱和核磁共振确定了它的组成和结构，特别是在1650 cm~(-1)处出现(C_5H_5SiMe_3)_2的孤立双键吸收峰。用C_5H_5SiMe_3和Ee(CO)_5回流反应制得了[C_5H_4(SiMe_3) Ee(CO)_2]_2。经过元素分析，红外光谱，质谱，顺磁共振确定了配合物的组成，红外光谱中有桥羰基的吸收峰，质谱图中498的离子峰的出现标志着上述二聚体的存在。用[C_5H_5Fe(CO)_2]_2作为制备双金属配合物的原料，用Na/Hg并还原[C_5H_5Fe(CO)_2]_2。反应时间为6-7小时得到中间体[C_5H_5Fe(CO)_2]_2Na·4THF的深紫红色晶体。反应时间加长，中间体被破坏，反应到15小时时生成了[C_5H_5Fe(CO)_2]Na·TMEDA的黄色晶体，特别是中间体的获得及晶体结构的测定对我们解释反应的机理非常重要。[C_5H_5Fe(CO)_2]_2Na·4THF为单斜晶系，空间群为P21/n，晶胞参数为a = 10.155(5)，b = 17.121(4)，C = 18.667(6)A°，β = 97.61(3)°，V = 3216.9A°~3， 2 = 4。铁的配位数为七，钠的配位数为六，钠离子和桥连羰基氧以配位键结合，每个钠离子连结着两个[C_5H_5Fe(CO)_2]_2~-，而每个[C_5H_5Fe(CO)_2]_2~-又连结着两个钠离子，组成一个无限链状分子，键状分子间以Van de W力结合。[C_5H_5Fe(CO)_2]Na·TMEDA正交晶系，空间群为P_(2,2,2,)。晶胞参数为a = 6.001(4)，b = 10.644(6)，C = 24.214(11)A~·。α = β = r = 90°。z = 4 V = 1546·7A°~3，铁的配位数为五。钠的配位数为四，钠离子和羰基氧以配位键结合，每个钠离子连结着两个[C_5H_5Fe(CO)_2]~-，每个[C_5H_5Fe(CO)_2]~-又连结着两个钠离子，体系就是以这种连结方式或正负电荷交替的形式无限螺旋分子，每个链节存在着两个[C_5H_5Fe(CO)_2]Na·TMEDA分子，链节的长度为a轴的轴长，说明螺旋分子以a轴轴长向上平移。用LnCl_3·nTHF和[C_5H_5Fe(CO)_2]Na反应制得了[C_5H_5Fe(CO)_2] LnCl_2·nTHF (Ln = Nd, Sm, Gd; n = 1, 2)，用[C_5H_5Fe(CO)_2] LnCl_2和[C_5H_4(SiMe_3)]Na或用[C_5H-4(SiMe_3)] LnCl_2和[C_5H_5Fe(CO)_2]Na得到[C_5H_5Fe(CO)_2] [C_5H_4(SiMe_3)] LnCl·nTHF (Ln = Nd, Sm, Gd; n = 0, 1, 3)，配合物[C_5H_5Fe(CO)_2] LnCl_2·nTHF及[C_5H_5Fe(CO)_2] [C_5H_4(SiMe_3)] LnCl·nTHF中存在着2000 cm~(-1)左右的终端羰基吸收峰及1766 cm~(-1)左右的桥连羰基吸收峰。说明稀土和铁之间是以羰基相连的。在TOTOE质谱仪上，配合物[C_5H_5Fe(CO)_2]Gd~·Cl·THF出现[C_5H_5Fe(CO)]GdCl_2、[Fe(CO)_2] Gd~+Cl_2的离子峰，配合物[C_5H_5Fe(CO)_2]-[C_5H_4(SiMe_3)] GdCl·THF出现[C_5H_5Fe(CO)_2] [C_5H_4]Gd~+Cl、[C_5H_5Fe(CO)_2]Gd~+Cl·[C_5H_4C(SiMe_3)] Gd~+Cl等离子峰。所有稀土有机配合物都溶于四氢呋喃、苯，对空气和水敏感。

南海北部白云凹陷渗漏型天然气水合物地球物理证据

根据水合物的聚集方式，海底水合物可以分为以似海底反射（BSR）为标志的扩散型水合物和无BSR的渗漏型水

INFRARED-ABSORPTION DUE TO 2-DIMENSIONAL-ELECTRON-GAS COLLECTIVE EXCITATION IN GAAS/ALXGA1-XAS MULTIPLE-QUANTUM-WELL STRUCTURES

Infrared absorption due to a collective excitation of a two-dimensional electronic gas was observed in GaAs/AlxGa1-xAs multiple-quantum wells when the incident light is polarized parallel to the quantum-well plane. We attribute this phenomenon to a plasma oscillation in the quantum wells. The measured wavelength of the absorption peak due to the plasma oscillation agrees with our theoretical analysis. In addition, in this study the plasma-phonon coupling effect is also fitted to the experimental result. We show that the absorption is not related to the intersubband transitions but to the intrasubband transition, which originates from a plasma oscillation.

PLD方法制备ZnO薄膜的特征温度研究

用PLD方法在Si(111)衬底上制备了ZnO薄膜.在薄膜的沉积过程中,用安装在激光脉冲沉积设备上的反射高能电子衍射仪(RHEED)对薄膜的生长进行了原位监测.结合薄膜的X射线衍射(XRD)分析和荧光光谱(PL)分析,发现达到或者超过650C时生长的薄膜,结构和光学特性得到了显著的改善.

基于DBFNN的推设及其在电力系统励磁控制中的应用

本文采用后推设计算法为一类严格反馈系统设计了基于方向基函数神经网络(DBFNN)的自适应控制器.在后推算法中的每步都引入一积分型的Lyapunov函数来设计一个虚拟控制器,并在最后一步为闭环系统综合设计了神经网络控制器.网络权值的调整基于所选择的Lyapunov函数,于是设计方案能保证整个闭环系统是最终一致有界的.把所设计控制方案用于带有未知参数和外部干扰的电力系统励磁控制中.仿真结果表明了所设计控制器的有效性.

Study of turbulent heat transfer of aviation kerosene flows in a curved pipe at supercritical pressure

The now and heat transfer characteristics of China No. 3 aviation kerosene in a heated curved tube under supercritical pressure are numerically investigated by a finite volume method. A two-layer turbulence model, consisting of the RNG k-epsilon two-equation model and the Wolfstein one-equation model, is used for the simulation of turbulence. A 10-species kerosene surrogate model and the NIST Supertrapp software are applied to obtain the thermophysical and transport properties of the kerosene at various temperature under a supercritical pressure of 4 MPa. The large variation of thermophysical properties of the kerosene at the supercritical pressure make the flow and heat transfer more complicated, especially under the effects of buoyancy and centrifugal force. The centrifugal force enhances the heat transfer, but also increases the friction factors. The rise of the velocity caused by the variation of the density does not enhance the effects of the centrifugal force when the curvature ratios are less than 0.05. On the contrary, the variation of the density increases the effects of the buoyancy. (C) 2010 Elsevier Ltd. All rights reserved.