Thermal Performance of Laser Diode Array under Constant Convective Heat Transfer Boundary Condition

Three-dimensional heat transfer model of laser diode array under constant convective heat transfer coefficient boundary condition is established and analytical temperature profiles within its heat sink are obtained by separation of variables. The influences on thermal resistance and maximum temperature variation among emitters from heat sink structure parameters and convective heat transfer coefficient are brought forward. The derived formula enables the thermal optimization of laser diode array.     

Measuring Grüneisen Parameter of Lead by High Pressure-Jump Method

Using the technology of pressure jump, variations of temperature associated with pressure from 2.4 GPa to 4.6 GPa are measured for lead. The Grfuneisen parameter is calculated from the thermodynamic relation γ =（Ks/T）（aT/aP）s, in which substitution of △T/△P for aT/aP at median pressure is strictly justified. The correction of temperature change is carried out by analysing the experimental data, which makes the process more approaching to an adiabatic condition. The calculated values of △T/ △ P and γ gradually decrease with the increasing pressure. The decrease trend is consistent with the previous work. The γ values in the range of 2-3 GPa are averagely higher than the results of Ramakrishnan et al., indicating the effect of temperature correction. The improved method is promising for measurements of Grfineisen parameter to higher pressure range.     

Inverse Scattering Transform for the Derivative Nonlinear Schrodinger Equation

Since the Jost solutions of the derivative nonlinear Schrodinger equation do not tend to the free Jost solutions, when the spectral parameter tends to infinity（｜A｜→∞）, the usual inverse scattering transform （IST） must be revised. If we take the parameter κ = λ^-1 as the basic parameter, the Jost solutions in the limit of ｜κ｜→∞ do tend to the free Jost solutions, hence the usual procedure to construct the equations of IST in κ-plane remains effective. After we derive the equation of IST in terms of κ, we can obtain the equation of IST in λ-plane by the simple change of parameters λ = κ^-1. The procedure to derive the equation of IST is reasonable, and attention is never paid to the function W（x） introduced by the revisions of Kaup and Newell. Therefore, the revision of Kaup and Newell can be avoided.     

Research of the planar optical fiber Bragg grating hydrophone probe

This paper presents the planar Fiber Bragg Grating （FBG） hydrophone probe sensing principle, and theoretically and experimentally researches the probe structure sensitivity, the receiving sensitivity frequency response characteristic and the acceleration response property. Planar sheet is made of stainless steel, its thickness is 0.15 mm, its diameter is 15mm, and the length of hollow circular shell is 20 mm. For this size of the structure, the probe structure sensitivity is up to 23 fm/Pa, which is about 7300 times of the value of the bare fiber. The resonance frequency is 6.5 kHz, and the amplitude-frequency curve of the receiving sensitivity response is relatively flat within the frequency range of 100 Hz to 5.5 kHz. The output yielded by one unit acceleration （1m/s2） is equivalent to （2.52 to 3.26 Pa） acoustic pressure acting output. This probe structure is easy to form FBG hydrophone array by multiplexing technique. The research shows that this planar structure not only can form FBG hydrophone probe, but also can constitute optical FBG laser hydrophone probe. The structure can realize different bandwidth, different range acoustic pressure measurement by adjusting the geometrical size of the sheet.     

WDM网状网中动态域间流量疏导策略

对波分复用(Wavelength Division Multiplexing,WDM)网状网中的动态域间流量疏导问题进行了深入研究.在源路由模式下,提出了一种基于固定备选路由方式的动态域间流量疏导算法,并在其基础上提出了只考虑波长均衡和同时考虑波长均衡与业务均衡的改进方法.该算法可以有效地避免路由环,得到较低的阻塞率,节省全网的收发器数目和波长资源.仿真结果表明,这种算法可以有效地改善网络性能.     

掺杂香豆素6的杂化纳米颗粒的制备及荧光性能研究(英文)

采用一种再沉淀-封装法制备了掺杂香豆素6(C6)的杂化荧光纳米颗粒,并通过SEM和DLS对其进行了形貌和粒径大小表征。在450 nm光激发下,制备的C6掺杂纳米颗粒表现出绿色荧光。通过比较光致发光光谱随掺杂浓度的变化,得出C6掺杂纳米颗粒的浓度猝灭是因为分子间能量转移而非C6分子聚集所致。另外,由于所选聚合物基质材料PS和PMMA分子结构的区别,导致PS-基质和PMMA-基质的纳米颗粒的光谱形状不同。C 6分子在PS-基质的纳米颗粒中处于两种不同的微环境,所以发射峰较宽;PMMA是线性分子,PMMA-基质的纳米颗粒中只存在一种局域环境,所以发射峰较窄。高的掺杂浓度会超过纳米颗粒对C6分子的负载能力,从而导致C6分子在水溶液中聚集。     

聚合物波导型表面等离子体共振传感器的特性研究

基于表面等离子体共振理论,将SU-8作为波导芯层材料,以聚甲基丙烯酸甲酯(PMMA)为下包层材料,设计了一款聚合物波导型SPR传感器。理论计算了波导芯层折射率、被测物折射率、不同金属薄膜及其厚度等因素对表面等离子体共振曲线的影响。分析结果表明,在可测试范围内,被测物折射率越大,灵敏度越高;波导芯层折射率减小,共振峰向长波方向移动,被测物检测范围整体向折射率小的方向偏移,波导芯层折射率增大则相反。     

壳聚糖/SrHAP复合涂层的制备及其FTIR特征分析

在含有Sr2+,Ca2+,PO3-₄和壳聚糖(CHI)的电沉积液中,用恒电流沉积法,在医用纯钛(Ti)表面上得到壳聚糖/掺锶羟基磷灰石(SrHAP)复合涂层。采用扫描电镜(SEM)、能量弥散X射线谱(EDS)、X射线衍射(XRD)对涂层进行检测,用傅里叶变换红外光谱(FTIR)考察了壳聚糖和锶离子的掺杂对HAP涂层构象和生物活性的影响。结果表明：锶部分取代磷灰石中的钙,表面形貌由疏松的针状变为较致密的片状。FTIR分析表明,涂层中出现了典型的amideⅠ和amideⅡ的壳聚糖振动峰,则CHI与SrHAP杂化良好;模拟生理液浸泡后表面覆盖有球状类骨磷灰石,则涂层具备较好的生物活性。塔菲尔测试表明,复合涂层使得Ti表面的抗生理腐蚀性显著提高。     

强碱胁迫枯草芽孢杆菌芽孢致死的拉曼光谱研究

应用单细胞拉曼分析技术结合PCA方法,以枯草芽孢杆菌芽孢为对象,以强碱为诱导剂实时记录芽孢生理变化过程,探究芽孢在强碱胁迫下的致死机制。实验表明,枯草芽孢杆菌芽孢和其萌发后芽孢在一定范围均有一定的耐受强碱能力,但萌发后芽孢的耐受力明显下降,主要原因是释放了维持其抗性及稳定性的特有Ca2+-DPA的保护;芽胞受强碱胁迫也会有少量Ca2+-DPA释放过程的行为特征,但通过分析所记录的光谱数据结果表明,其释放行为不同于由L-丙氨酸引起的芽孢的正常Ca2+-DPA释放过程。通过PCA比较分析强碱胁迫芽孢和萌发后芽孢Ca2+-DPA释放过程,主要是强碱破坏芽孢膜结构,膜损伤后强碱比较容易进到芽孢内部从而破坏蛋白质的主链结构链及核酸;芽孢膜通道也可能受到强碱的伤害,造成微量Ca2+-DPA的释放。     

新型4-氨基安替比林席夫碱的合成及对Cu2+的选择性识别

设计合成了一种新型安替比林-席夫碱衍生物M(4-氨基安替比林缩5-硝基水杨醛席夫碱),用IR、1H NMR及元素分析对其结构进行了表征。通过紫外光谱和荧光光谱研究了M对Cu2+的选择性识别作用。结果表明:M与Cu2+能够以1∶1的化学计量比形成配合物,结合常数为6.5×104L·mol-1;M和Cu2+的结合导致M在496 nm处的荧光猝灭,紫外可见吸收光谱红移,且M对Cu2+有较高的选择性,受常见离子的干扰较小。