金锡共晶互连对HP-LED光热性能的改善

随着功率型LED(HP-LED)对散热的要求越来越高,传统导电银胶越来越难以满足LED的高散热要求。虽然共晶互连工艺是微电子领域中的一种有效的散热互连方法,但是由于LED的特殊性,该工艺在LED互连封装中的性能改善研究还比较少。本文对金锡共晶互连、锡膏互连和银胶互连的3种LED器件分别进行了光学、热学以及剪切力等方面的测试分析研究,结果表明:底部与顶部同时加热的金锡共晶工艺互连的LED器件可以有效地改善仅底部加热共晶互连层中的空洞缺陷,在1 000 mA电流条件下,相对于锡膏、银胶互连的LED器件具有较低的热阻、较稳定的峰值波长偏移、较强的互连层剪切力等性能。金锡共晶互连工艺是一种可以有效改善大功率LED散热及互连强度的方法。     

紫外预电离放电引发的非链式脉冲DF激光器

采用紫外预电离的横向放电方式和稳定光学谐振腔,使用无毒无腐蚀性的六氟化硫(SF6)和氘气(D2)作为工作物质,研究了工作气体配比、总气压对放电引发非链式脉冲氟化氘(DF)激光器输出能量的影响。实验发现SF6与D2的最佳比例为10:1,最佳总气压为10.5 kPa。使用DF激光谱线分析仪对激光输出谱线进行了测量,得到了17条P支跃迁谱线,激光能量集中在3.876μm附近的几条谱线。利用烧蚀光斑的方法测得输出激光束水平方向、垂直方向的发散角均为1 mrad。在最佳工作条件下,充电电压为39 kV时,激光单脉冲输出能量达到最大值3.58 J,此时激光脉冲宽度为215 ns,峰值功率为16.65 MW,电光转换效率为2.08%。     

ICF靶丸装配误差检测

针对激光惯性约束聚变装置中靶丸装配误差检测困难、要求精度高的特点,研制了一套用于微靶装配参数检测的测量系统。提出了一种基于激光与CCD的复合式测量方法,建立了二者数据融合的数学模型,通过标定空间位置关系有效地把二者的测量数据融合到同一个坐标系中,从而实现了高精度三维测量。分两种情况讨论了靶丸装配误差的检测方法。实验结果验证了这两种方法的可行性,并比较了两种方法的测量精度,其极限测量误差均不超过3 m。     

丙烯腈-尿素包合物的形成过程及特征

利用差示扫描量热法(DSC)和X射线衍射(XRD)研究了在不同丙烯腈/尿素投料比情况下的丙烯腈-尿素包合物的形成过程和组成. 实验结果表明DSC是一种研究包合物的客主比及分解热的有效方法. 测定了丙烯腈-尿素包合物的客主比和分解热分别为1.17和5361.53 J/mol. 同时发现丙烯腈-尿素包合物的形成依赖于冷冻时间,在足够长的冷冻时间之后丙烯腈-尿素包合物的组成达到稳定状态. 实验结果表明,丙烯腈分子可能是采用堆叠的方式排布在尿素晶道结构中. XRD结果表明只要丙烯腈分子进入尿素晶格中,丙烯腈-尿素包合物的结构便形成了,并且这种结构与形成过程终了时的结构是一致的. 只要丙烯腈是足量的,包合物中的丙烯腈分子排列会随冷冻时间的延长而增长,直到尿素的晶道结构被丙烯腈分子填满.     

Influence of Sulfur on Cure Kinetics of Natural Rubber/Sulfur/N-t-butylbenzothiazole-2-sulfenamide (TBBS) System Studied by Rubber Processing Analyzer

Based on the cure characteristics of the Natural Rubber/Sulfur/N–t–butylbenzothiazole– 2–sulfenamide (NR/S/TBBS) system, a kinetic model with induction, curing, and overcure periods was chosen to simulate the cure reaction of this system. Cure-curves reflecting the development of torque were recorded as a function of cure time for NR compounds by a rubber processing analyzer. The cure curves were then non-linear fitted. The results show that the simulated curves fit well with the experimental curves. Rate constant K ₂ for formation of activated crosslink precursors is much higher than rate constant K ₆ for crosslink degradation under the same cure condition. Reaction activation energy E ₂ and E ₆ calculated from K ₂ and K ₆ through the Arrhenius equation showed that E ₆ is higher than E ₂. The increase of sulfur dosage led to the decrease of E ₆ and E ₂, but E ₆ decreased more evidently.     

Evaluation of ADC measurements among solid pancreatic masses by respiratory-triggered diffusion-weighted MR imaging with inversion-recovery fat-suppression technique at 3.0 T

Purpose

The objective of this paper was to investigate the value of apparent diffusion coefficients (ADCs) for differential diagnosis among solid pancreatic masses using respiratory triggered diffusion-weighted MR imaging with inversion-recovery fat-suppression technique (RT-IR-DWI) at 3.0 T.

Materials and Methods

20 normal volunteers and 72 patients (Pancreatic ductal adenocarcinoma [PDCA, n = 30], mass-forming pancreatitis [MFP, n = 15], solid pseudopapillary neoplasm [SPN, n = 12], and pancreatic neuroendocrine tumor[PNET, n = 15]) underwent RT-IR-DWI (b values: 0 and 600 s/mm²) at 3.0 T. Results were correlated with histopathologic data and follow-up imaging. ADC values among different types of pancreatic tissue were statistically analyzed and compared.

Results

Statistical difference was noticed in ADC values among normal pancreas, MFP, PDCA, SPN and PNET by ANOVA (p < .001). Normal pancreas had the highest ADC value, then followed by PNET, PDCA, MFP and SPN. There was noticeable statistical difference in ADC values among PDCA, MFP and normal pancreas by Least Significant Difference (LSD) (p < .001). ADC of SPN was statistically lower than that of PNET (p = 0.1800 × 10^− 4), PDCA (p = 0.0300 × 10^− 4) and normal pancreas (p = 0.0007 × 10^− 4). ADC of PNET was statistically lower than that of normal pancreas (p = 0.0360) and higher than that of MFP (p = 9.3000 × 10^− 4).

Conclusions

ADC measurements using RT-IR-DWI at 3.0 T may aid to disclose the histopathological pattern of normal pancreas and solid pancreatic masses, which may be helpful in characterizing solid pancreatic lesions.     

掺杂Y2O3和BaCeO3提高MOD-YBCO超导性能的研究

本文通过在前驱液中添加过量钇盐和铈的有机盐,采用三氟乙酸盐-金属有机沉积法(TFA-MOD) 在铝酸镧单晶基体上制备了含有纳米氧化钇和纳米铈酸钡的YBCO薄膜. 与纯YBCO薄膜相比,掺杂Y₂O₃/BaCeO₃的YBCO膜的临界转变温度几乎保持不变,为91 K左右. 而掺杂Y₂O₃/BaCeO₃的YBCO膜的临界电流密度达到5.0 MA/cm² (77 K, 0T), 是纯YBCO膜临界电流密度的1.5倍.薄膜中的Y₂O₃和BaCeO₃可能在YBCO内部起到了 有效的钉扎磁通作用. 关键词： 钇钡铜氧薄膜 2O₃和纳米BaCeO₃')" href="#">纳米Y₂O₃和纳米BaCeO₃ 磁通钉扎 三氟乙酸盐-金属有机沉积     

基于Add-drop型微环谐振腔的硅基高速电光调制器设计

相比于传统的All-pass型微环谐振腔硅基电光调制器, Add-drop型微环谐振腔可提供更多的设计自由度, 使调制器在不改变杂质掺杂浓度的情况下就能在调制带宽和消光比性能上获得均衡考虑. 本文设计了基于Add-drop型微环谐振腔的高速、且在低调制电压下实现大消光比的硅基电光调制器, 所用微环谐振腔的半径仅仅为20 μm. 重点分析了直波导与微环谐振腔的耦合对调制器性能的影响, 发现较小的Drop端耦合系数有利于消光比的提高, 但是不能同时达到最佳的调制带宽, 因此设计上存在一个带宽和消光比性能上的折中考虑. 根据优化设计的结果进行了实际器件的制作和测试. 静态光谱测试表明, 在3 V反向偏置电压的作用下, 调制器的消光比最大可达12 dB. 动态电光响应测试中, 在仅仅1.2 V的信号幅值电压下测得了8 Gbps数据传输速率的清晰眼图. 关键词： 电光调制器 绝缘体上的硅 微环谐振腔 载流子色散效应     

Synthesis and Spectra of a Kind of Novel Longer-Wavelength Benzoxazole Indole Styryl Cyanine Dye with a Carbazole-Bridged Chain

Based on cyanine dye probe oxazole yellow (YO) and Cy₃, a series of novel styryl cyanine dyes were designed and synthesized. Carbazole was inserted into the structures of YO and Cy₃ to act as a bridge to link the benzoxazole and indole group. This modification resulted in a novel kind of benzoxazole indole styryl cyanine dye with a carbazole-bridged chain. The dyes were characterized by ¹HNMR and MS. The spectra of the novel dyes were also performed and the results showed that the maximum emission wavelength of the carbazole styryl cyanine dye was shifted red, the Stokes shift increased and the fluorescence intensity enhanced compared with those of YO and Cy₃. These results indicated that the novel dye could be used as an excellent fluorescent probe in biological labeling.     

On the spectral radius of ‡-shape trees

Let A(G) be the adjacency matrix of G. The characteristic polynomial of the adjacency matrix A is called the characteristic polynomial of the graph G and is denoted by φ(G, λ) or simply φ(G). The spectrum of G consists of the roots (together with their multiplicities) λ ₁(G) ? λ ₂(G) ? … ? λ _n (G) of the equation φ(G, λ) = 0. The largest root λ ₁(G) is referred to as the spectral radius of G. A ?-shape is a tree with exactly two of its vertices having maximal degree 4. We will denote by G(l ₁, l ₂, … l ₇) (l ₁ ? 0, l _i ? 1, i = 2, 3, …, 7) a ?-shape tree such that $G\left( {l_1 ,l_2 , \ldots l_7 } \right) - u - v = P_{l_1 } \cup P_{l_2 } \cup \ldots P_{l_7 }$ , where u and v are the vertices of degree 4. In this paper we prove that ${{3\sqrt 2 } \mathord{\left/ {\vphantom {{3\sqrt 2 } 2}} \right. \kern-0em} 2} < \lambda _1 \left( {G\left( {l_1 ,l_2 , \ldots l_7 } \right)} \right) < {5 \mathord{\left/ {\vphantom {5 2}} \right. \kern-0em} 2}$ .