合肥高新区园区企业积极参与合肥对接会

第四届中国·合肥高新技术项目资本对接会筹备工作启动后，得到了合肥高新区园区企业的积极响应。据统计，该区共申报近80个参展项目参加此次展会，这些项目总投资9．45亿元，其中资金需求4．3亿元。     

TiO_2纳米棒阵列的水浴法制备及形貌控制

展示一种在FTO玻璃基底上直接生长TiO2纳米棒阵列的简单方法.利用化学水浴法,通过控制反应过程中钛源和盐酸(HCl)量,在FTO导电玻璃基底上直接生长分布均匀的TiO2纳米棒阵列,棒的高度约为500nm,直径约为20nm.纳米棒阵列薄膜在退火之前为无定型结构;经过450℃退火0.5h后,为锐钛矿和金红石的混合相.     

Lifetimes of High Spin States in an Odd-Proton Nucleus 129Cs

Lifetimes of high spin states in 129Cs axe measured using the Doppler shift attenuation method. The high spin states of 129 Cs axe populated following the fusion evaporation reaction 124 Sn（UB, 6n）129 Cs at a beam energy of 65 MeV. The reduced transition probabilities B（E2） and the transition quadrupole moments Qt in the negativeand positive-paxity bands are deduced. The experimental results indicate that the Qt values of the negative parity band are smaller than those of the positive parity bands, probably due to different γ-deformation driving effects of different proton orbitals. The Qt values exhibit a considerable increase near the band crossing region in these bands. This behavior demonstrates that nuclear shape changing results from the neutron or proton alignments. The signature splitting of the πh11/2 and πg7/2 bands shows the opposite changing trend after backbending due to the h11~2 neutron and h11/2 proton alignments, respectively.     

室温生长ZnO薄膜晶体管的紫外响应特性

在室温下采用射频磁控溅射法制备了以ZnO薄膜为沟道层的薄膜晶体管(TFTs).研究表明ZnO薄膜在紫外区具有较高的吸收率,并且ZnO-TFTs对紫外光照射较为敏感.因此,进一步深入研究了ZnO-TFTs紫外光照下的输出和转移特性,结果表明,紫外光照将引起较为明显的光响应电流,且经过光照的器件在光源移除7天后,ZnO沟道层中仍能观察到残余电导现象,其原因可以归结为紫外光辐射在ZnO沟道层中引入了一定数量的氧空位施主态缺陷.     

c(2×2)-(K+CO)在Co{1010}表面吸附的NEXAFS研究

对CO和K共吸附在CO{1010}表面的系统进行了O的1s NEXAFS理论研究,证实吸附分子CO的键长比气体状态时增长约0.01nm.用MSC(多重散射团簇)理论计算谱与实验结果比较发现：在原π峰右侧出现了一个新的弱结构.证明了此结构是由于K通过钴衬底对CO的间接作用造成的,它具有π共振的性质. 关键词：     

页岩氮气吸附BET比表面积测定误差校正方法

基于多分子层吸附理论的BET模型是最成熟、最常用于比表面测试的计算方法,然而,针对页岩样品在液氮温度下的氮气吸附数据,选取0.05~0.30间的相对压力点(适用于中孔材料)进行BET比表面计算时,将出现回归曲线相关系数较差、常数C为负值(无物理意义)情况,这一问题往往被测试者忽视。通过页岩的二氧化碳吸附数据运用DFT模型,计算出页岩的微孔分布可知,页岩含有大量0.5~1.0 nm之间的微孔,页岩纳米级孔隙分布范围广的特点是出现上述问题的根本原因,即页岩并非孔径分布较窄的介孔材料。通过调整相对压力点的选取范围,在相对压力0.05~0.20下计算页岩比表面其相关系数能达到0.999 9以上,且在Y轴上产生正截距,该相对压力范围更为合理,计算出的BET比表面更为可靠。     

Shape evolution and test of the critical-point symmetry X(5) in 176Os

The lifetimes of excited states in the yrast band of ¹⁷⁶Os have been measured up to I=20h level using the Doppler shift attenuation method. The high-spin states of ¹⁷⁶Os were populated via fusion evaporation reaction ¹⁵²Sm(²⁸Si, 4n)¹⁷⁶Os at a beam energy of 140 MeV. The results support an X(5) structure for ¹⁷⁶Os at low spin. This structure disappears at high spin and shows a symmetry rotor character. The shape change of ¹⁷⁶Os is similar to that of ¹⁷⁸Os.     

论我国民事管辖权异议制度的改革与完善

由于我国民事诉讼法对管辖权异议的规定过于原则,适用程序不完备,导致审判实务中对此制度运用不规范,设立管辖权异议制度的根本价值难以实现。本文通过分析我国民事管辖权异议制度在立法和司法实践中存在的弊端及其原因,提出完善我国民事管辖权异议制度的浅见。     

基于强度参数演化的裂隙岩体峰后应力-应变关系求法

完整岩块峰后应力应变关系的表达不能较好反映裂隙岩体峰后特性,为得到适合裂隙岩体峰后应力-应变关系,在试验数据基础上,基于库伦强度准则,分析裂隙岩体峰后强度参数的演化行为。根据裂隙岩体在不同围压和裂隙倾角时的不同峰后特性,将峰后应力-应变关系简化为A和B两种类型。以应变作为应变软化参数,假设黏聚力、内摩擦角为应变的分段线性函数,给出裂隙岩体峰后两种类型应力-应变关系式的求法。将A和B两种类型应力-应变关系式算出结果与试验结果进行比较,得出用裂隙岩体的应力-应变关系求得峰后应力-应变曲线与试验数据基本一致。     

Shedding vortex simulation method based on viscous compensation technology research

Owing to the influence of the viscosity of the flow field, the strength of the shedding vortex decreases gradually in the process of backward propagation. Large-scale vortexes constantly break up, forming smaller vortexes. In engineering, when numerical simulation of vortex evolution process is carried out, a large grid is needed to be arranged in the area of outflow field far from the boundary layer in order to ensure the calculation efficiency. As a result, small scale vortexes at the far end of the flow field cannot be captured by the sparse grid in this region, resulting in the dissipation or even disappearance of vortexes. In this paper, the effect of grid scale is quantified and compared with the viscous effect through theoretical derivation. The theoretical relationship between the mesh viscosity and the original viscosity of the flow field is established, and the viscosity term in the turbulence model is modified. This method proves to be able to effectively improve the intensity of small-scale shedding vortexes at the far end of the flow field under the condition of sparse grid. The error between the simulation results and the results obtained by using fine mesh is greatly reduced, the calculation time is shortened, and the high-precision and efficient simulation of the flow field is realized.