校园网邮件服务器安全防范与构建

讨论了目前校园网电子邮件服务器的安全问题，并用postfix和openwebmail等自由软件实现了一个具有较高安全和性能的校园网电子邮件系统、     

A Wafer-Level Sn-Rich Au-Sn Bonding Technique and Its Application in Surface Plasmon Resonance Sensors

Sn-rich Au Sn solder bonding is systematically investigated. High shear strength （64 MPa） and good hermeticity （a leak rate lower than 1 × 10-7 torr.1/s） are obtained for Au-Sn solder with 54wt% Sn bonded at 310℃. The AuSn2 phase with the highest Vickers-hardness among the four stable intermetMlic compounds of the Au Sn system makes a major contribution to the high bonding strength. This bonding technique has been successfully used to package the Surface Plasmon Resonance （SPR） sensors. The Sn-rieh Au-Sn solder bonding provides a reliable, low-cost, low-temperature and wafer-level hermetic packaging solution for the micro-electromechanical system devices and has potential applications in high-end biomedical sensors.     

球形集声器在生物组织中形成的组织损伤

球形集声器可在亚波长焦域内形成高强度声压,在高强度聚焦超声治疗中具有潜在应用前景.本文结合非线性声传播理论及生物传热学理论,研究球形集声器在生物组织中形成的组织损伤.实验中采用430 kHz,内径为240 mm的球形集声器对肝组织作用,结果表明:集声器表面声压为53 kPa时作用2 s,可以形成小于波长尺度的组织损伤.理论计算结果与实验结果符合得较好,并且理论模型可优化球形集声器的开口孔径.研究结果表明,球形集声器可应用于肿瘤的精细超声治疗.     

最小化总完工时间与分批费用之和的有界分批排序问题

考虑了当每分一批均产生固定费用、批容量有界且为固定值b、加工不允许中断抢先.所有工件在零时刻到达时的单机平行分批排序问题.目标是最小化总完工时间与分批费用之和.利用动态规划方法给出了多项式时间算法,时间界为O(n~(b(b-1))).     

基于偏振光波导分光光谱技术原位研究纳米金-细胞色素c 自组装过程

时间分辨偏振光波导分光光谱技术是一种用于研究表面分子吸附动力学的强大工具. 利用该技术实时、原位监测纳米金与细胞色素c的静电自组装过程, 发现随着吸附层数的增加, 纳米金粒子吸附层产生的局域等离子体共振(LSPR)吸收峰发生了红移, 而且在横磁(TM)模式下的红移比横电(TE)模式下的红移更快; 细胞色素c在纳米金表面的吸附导致LSPR吸收峰的峰位和强度在TM模式下显著红移和升高, 相比之下, TE模式下的LSPR吸收峰无明显变化. 对实验数据的分析验证了纳米金在细胞色素c单分子层表面的吸附动力学行为遵循扩散控制模型, 细胞色素c在纳米金单粒子层表面的吸附动力学行为遵循Langmuir等温吸附模型, 进一步估算了细胞色素c在纳米金表面的吸附速率常数、脱附速率常数和吸附自由能.     

牛磺酸干预对高糖培养H9c2心肌细胞的保护效应与机制

为研究与分析牛磺酸干预对高糖培养H9c2心肌细胞的保护效应及其具体机制。通过将复苏的H9c2心肌细胞传至3～4代,分为以下三组:(1)对照组(CN):葡萄糖浓度为5. 5 mmol/L;(2)高糖组(HG):葡萄糖浓度为25. 5 mmol/L;(3)牛磺酸干预组(TAU):HG组基础上,加终浓度为40 mmol/L的牛磺酸。48 h后收集细胞,采用Annexin-V/碘化丙啶(propidine iodide,PI)结合流式细胞仪检测心肌细胞凋亡发生情况,Western Blot检测丝裂原活化蛋白激酶p38 MAPK的蛋白表达,放射免疫法检测TNF-α表达量,并采用相关试剂盒检测丙二醛(MDA)、超氧化物歧化酶(SOD)水平。结果显示:与CN组相比较,HG组H9c2心肌细胞经高糖培养48 h后细胞凋亡率增加(P 0. 001),细胞TNF-α、MDA显著水平升高(P 0. 001),SOD水平降低(P 0. 001),胞内磷酸化p38水平亦升高(P 0. 001);加入牛磺酸干预后,与HG组比较,TAU组细胞凋亡率减小(P 0. 01),细胞TNF-α、MDA及磷酸化p38蛋白水平明显降低(P 0. 05),SOD水平升高(P 0. 01)。可见牛磺酸能够减轻高糖刺激下H9c2心肌细胞的凋亡,其机制可能通过上调SOD水平,下调TNF-α、MDA水平,降低胞内p38磷酸化来实现对高糖细胞损伤的保护效应。     

锰纯度定值及其单元素溶液标准物质的研制

以高纯锰为原料研制锰单元素溶液标准物质。采用电感耦合等离子体质谱法、电感耦合等离子体发射光谱法以及元素分析仪3种方法测定高纯锰中杂质元素的含量,并通过杂质扣除法确定了高纯锰的纯度为(99.95±0.04)%(k=2)。采用重量–容量法制备了锰单元素溶液标准物质,以配制值作为锰单元素溶液标准物质的标准值。对溶液标准物质的均匀性和稳定性进行了检验,其均匀性与稳定性良好。对标准物质的不确定度进行了评定。锰单元素溶液标准物质的浓度值为100μg/mL,相对扩展不确定度为0.8%(k=2)。该标准物质的量值准确,可用于锰元素的分析检测、检测方法评价与仪器校准。     

Bow shocks formed by a high-speed laser-driven plasma cloud interacting with a cylinder obstacle

A bow shock is formed in the interaction of a high-speed laser-driven plasma cloud with a cylinder obstacle. Its temporal and spatial structures are observed by shadowgraphy and interferometry. The width of the shock transition region is ～ 50 μm, comparable to the ion–ion collision mean free path, which indicates that collision is dominated in the shock probably. The Mach-number of the ablating plasma cloud is ～ 15 at first, and decreases with time resulting in a changing shock structure. A two-dimension hydrodynamics code, USim, is used to simulate the interaction process. The simulated shocks can well reproduce the observed.     

Application of multi-pulse optical imaging to measure evolution of laser-produced counter-streaming flows

A counter-streaming flow system is a test-bed to investigate the astrophysical collisionless shock(CS) formation in the laboratory. Electrostatic/electromagnetic instabilities, competitively growing in the system and exciting the CS formation, are sensitive to the flows parameters. One of the most important parameters is the velocity, determining what kind of instability contributes to the shock formation. Here we successfully measure the evolution of the counter-streaming flows within one shot using a multi-pulses imaging diagnostic technique. With the technique, the average velocity of the high-density-part(ne ≥ 8–9 × 10~(19)cm~(-3)) of the flow is directly measured to be of ～ 10~6cm/s between 7 ns and 17 ns.Meanwhile, the average velocity of the low-density-part(ne ≤ 2 × 10~(19)cm~(-3)) can be estimated as ～ 10~7cm/s. The experimental results show that a collisionless shock is formed during the low-density-part of the flow interacting with each other.