透明陶瓷夹层结构冲击响应及BP神经网络预测

首先,选择以蓝宝石陶瓷为迎弹层、二氧化硅无机玻璃和聚碳酸酯有机玻璃为吸能层和聚氨酯为胶结材料的透明夹层结构为研究对象,采用一级轻气炮对试样进行了冲击实验,试样呈现陶瓷层弯曲失效破坏主导和冲击压缩破坏主导的2种破坏模式,通过高速摄像详细记录裂纹动态扩展过程。然后,采用Abaqus有限元软件对多组结构层厚度配比的透明夹层结构进行120、150、180 m/s速度的弹体冲击模拟,针对陶瓷材料引入了基于JH-2本构模型的子程序,并结合单元删除法,对裂纹扩展和碎片飞溅过程进行了数值模拟。模拟结果与实验结果吻合较好。最后,采用BP神经网络算法对冲击点后侧位移峰值进行了预测,单层和多层神经网络模型平均计算耗时分别为1和3 min,与位移峰值的数值模拟结果相比,2种神经网络模型预测结果的平均相对误差分别为7.6%和3.2%。该BP神经网络模型计算时效和精度都满足要求,相比传统消耗5 h的有限元计算,节省大量时间,可对透明夹层结构的设计提供指导。     

新型1,1′-双乙酰基二茂铁席夫碱的合成

通过1,1′-双乙酰基二茂铁双肼腙与芳醛(酮)的缩合反应,合成了6个新型1,1′-双乙酰基二茂铁席夫碱,其结构经1H NMR,IR和元素分析表征。     

Yb3+,Er3+共掺BaGd2ZnO5材料的制备及其上转换发光效率

采用溶胶-凝胶法制备了含有不同Yb³⁺,Er³⁺掺杂浓度的BaGd₂ZnO₅上转换发光材料,测量了这些样品在不同激发光密度下的上转换光发射功率及上转换效率。实验结果表明:在不同激发光密度下,所有样品的光发射功率都存在极大值,其中Yb³⁺掺杂摩尔分数为4%,Er³⁺掺杂摩尔分数为1%时样品的最大发射光功率可达20 mW;样品的上转换绝对效率也存在极大值,随着Yb³⁺和Er³⁺浓度增加,绝对效率的极大值向较低激发光密度方向移动,在Yb³⁺掺杂摩尔分数为9%,Er³⁺掺杂摩尔分数为3%时样品的上转换效率达到最高,绝对效率为3.2%,极值效率最大值为6.9%。     

多腔虚阴极振荡器研究

 提出了一种具有预调制腔、主谐振腔和提取腔组成的多腔轴向提取虚阴极振荡器结构。腔体特性分析表明其在工作频段可以获得更高的提取效率。粒子模拟显示该结构在电压700 kV,电流23 kA的条件下,可输出功率大于1.7 GW,频率4.0 GHz,功率效率大于10％的微波。初步的实验研究获得了辐射功率约700 MW,频率约4.1 GHz的微波输出。对实验结果的进一步分析表明,通过适当加大器件虚阴极振荡工作区微波管直径的方法可以有效改善器件的谐振性能,从而获得更好的工作性能。     

多腔虚阴极振荡器研究

提出了一种具有预调制腔、主谐振腔和提取腔组成的多腔轴向提取虚阴极振荡器结构。腔体特性分析表明其在工作频段可以获得更高的提取效率。粒子模拟显示该结构在电压700 kV,电流23 kA的条件下,可输出功率大于1.7 GW,频率4.0 GHz,功率效率大于10％的微波。初步的实验研究获得了辐射功率约700 MW,频率约4.1 GHz的微波输出。对实验结果的进一步分析表明,通过适当加大器件虚阴极振荡工作区微波管直径的方法可以有效改善器件的谐振性能,从而获得更好的工作性能。     

以单环有机锡配合物为载体的水杨酸根阴离子选择电极的研究

Two new cyclic pentacoordinative organotin(Ⅳ) complexes, 2,4-dihydroxyacetophenone tribenzyltin(HAPTBT) and 2,4-dihydroxyacetophenone triphenyltin(HAPTPT) were synthesized and used as anion ionophore for PVC membrane electrode. The new electrodes exhibit specificity selectivity for salicylate. The electrode based on HAPTBT as a neutral carrier displays a highly potentiometric response to salicylate and an anti-Hofmeister selectivity sequence in the following order: Sal^- ＞ SCN^- ＞ I^- ＞ NO₂^- ＞ Br^- ＞ Cl^- ＞ ClO₄^- ＞ NO₃^- ＞ SO₄^2-. The electrode has the advantages of fast response, stability and reproducibility, simplicity. The response mechanism is discussed in view of UV spectroscopy technique. The results show that there are close relationship between the potentiometric response characteristics and structure of organotin(Ⅳ) complexes. The electrode was applied to medicine analysis with satisfactory results.     

空气飞秒激光成丝现象中产生的椭圆偏振单周期太赫兹脉冲

飞秒激光在空气中形成的等离子体细丝会辐射出太赫兹(THz)信号.实验利用1 mJ,800 nm,50 fs的飞秒激光脉冲产生等离子体细丝.应用光电取样方法探测了激光成丝现象中前向辐射的THz脉冲,得到了持续时间为0.1 ps、光谱峰值在1 THz左右的单周期THz脉冲.转动抽运光的偏振态,分析了电光取样信号的变化.通过比较实验数据和计算结果,证明了成丝辐射THz脉冲的偏振态为椭圆偏振态.     

Development of a quasi-periodic undulator for the HLS

China's first quasi-periodic undulator (QPU) has been developed for the Hefei Light Source (HLS). It uses a magnetic configuration with varied thicknesses of NdFeB blocks, which is based on the QPU of European Synchrotron Radiation Facility (ESRF). The depression of 3^rd harmonic radiation is significantly improved over the ESRF QPU, as deduced from the measured magnetic fields. A method of configuring shims of different geometries and sizes, based on a symmetric principle to correct multi-pole field integrals, is demonstrated.     

Cryptanalysis and Improvement of Quantum Private Comparison Protocol Based on Bell Entangled States

Recently, Liu et al. [Commun. Theor. Phys. 57(2012) 583] proposed a quantum private comparison protocol based on entanglement swapping of Bell states, which aims to securely compare the equality of two participants' information with the help of a semi-honest third party(TP). However, the present study points out there is a fatal loophole in Liu et al.'s protocol, and TP can make Bell-basis measurement to know all the participants' secret inputs without being detected. To fix the problem, a simple solution, which uses one-time eavesdropper checking with decoy photons instead of twice eavesdropper checking with Bell states, is demonstrated. Compared with the original protocol,it not only reduces the Bell states consumption but also simplifies the protocol steps.     

水热法α-Al2O3自发结晶和形态控制

本文研究了高温高压水热法合成α-Al2O3晶体的形态特征.在水热条件下,α-Al2O3的晶体形态和合成温度、矿化剂浓度有密切关系.当KOH浓度和温度较低时(如0.1M KOH,390℃),显露c{0001}、a{11-20}、r{01-12}、n{11-23}晶面.随着矿化剂浓度和温度的提高,晶体r{01-12}和n}11-23}面的显露面积越来越小,直到完全消失(如2MKOH,400℃),晶体只显露底面c{0001}、和柱面a{11-20},呈六棱柱形.