退火时间对MgB_2超导薄膜的影响

在多晶A l2O3衬底上,以B2H6作为硼源,化学气相沉积先驱B薄膜,采用Mg扩散方法,在不同退火时间条件下制备了MgB2超导薄膜。通过电阻-温度曲线测量、X射线衍射分析和扫描电子显微镜形貌观测方法,研究了退火时间对MgB2薄膜的超导特性、晶体结构、表面形貌的影响。     

利用近红外光谱技术预测粗皮桉木材弹性模量

采用近红外光谱分析技术,对粗皮桉木材弹性模量进行了快速预测研究.使用快速傅里叶变换(FFT)分析法和常规力学测试方法测定了粗皮桉木材无疵小试样的弹性模量,并用近红外光谱仪采集试样径切面和弦切面的近红外漫反射光谱,对原始光谱进行二阶导数预处理,并选择410～2 480 nm光谱段建立回归模型.以2/3的试样作为校正集建立弹性模量的偏最小二乘法校正模型,以1/3/的试样作为预测集对模型进行验证.结果表明,粗皮桉木材的弹性模量与近红外光谱之间有较好的相关性,纵向弹性模量和抗弯弹性模量的预测模型的相关系数分别为0.93和0.81,相对分析误差分别为2.70和1.71.利用近红外光谱分析方法可以实现对粗皮桉木材无疵小试样弹性模量的快速预测.     

有机半导体的物理掺杂理论

基于最低未被占据分子轨道（LUMO）和最高被占据分子轨道（HOMO）的高斯态密度分布与载流子在允许量子态中的费米-狄拉克（Fermi-Dirac）分布,提出有机半导体中物理掺杂的理论模型;研究了掺杂浓度、温度和禁带宽度对载流子浓度的影响,并与一些报道的实验结果做了比较.研究发现无论是否掺杂,温度升高时,有机半导体中的载流子浓度都会增大,并且随温度倒数的线性减小而指数增大;对于本征有机半导体,载流子浓度随禁带宽度的增大而指数下降,随高斯分布宽度的平方指数增加;对杂质和主体不同能级关系的掺杂情形下掺杂浓度对载 关键词： 有机半导体 掺杂 高斯态密度 载流子浓度     

基于ARM和CPLD的NMR谱仪前放控制设计

提出了一种基于ARM（Advanced RISC Machine,先进精简指令计算机）和CPLD（Complex Programmable Logic Device, 复杂可编程逻辑器件）的NMR（Nuclear Magnetic Resonance,核磁共振）谱仪前放控制系统设计方案. 该控制系统以ARM为控制核心、 CPLD为控制命令执行单元, 控制前置放大器和混频器的工作状态. 本电路包括以下主要功能：1) 前置放大器收发切换的门控信号电平转换;2) 氘梯度匀场时身频通道自动切换;3) 探头调谐的信息显示;4) 锁前放和混频器的配置. 该设计方案具有系统运行速度高、 控制灵活和成本低的优点,并且可以有效减小系统噪声,降低控制部件对前置放大器和混频器的干扰.     

红外探测装置中光谱分光镜的设计与制备

在红外探测装置中,光谱分光镜是用来把3 μm～5 μm和8 μm～12 μm 2个波段的光谱分开的零件.介绍了一种在通用镀膜机上制备光谱分光镜的新工艺.在该膜系的设计过程中,把Willey公式引入到对其平均透过率最高值进行估算的过程中,同时针对国产镀膜机控制精度不高的特点,尽量使用规整膜层进行设计.为了进一步提高8 μm～12 μm波段的透过率,在膜系的最外侧引进了一层自行配制的低折射率氟化物材料,制备出了符合技术指标的红外光谱分光镜.     

Preparations for the study on the cluster structure of 16C

In order to look for a proposed cluster structure of 16C, simulation work was made. The simulation of the reaction dynamics give the resolution of the excitation energy on 16C which was reconstructed prior to breakup. The excitation energy resolution is typically ～200 keV at 2 MeV above the two body decay threshold for 16C→12Be+4He. Moreover,some performances of detectors tested using 241 Am α source are also reported.     

Electronic properties close to Dirac cone in two-dimensional organic conductor α-(BEDT-TTF)<Subscript>2</Subscript>I<Subscript>3</Subscript>

A zero-gap state (ZGS) has been found in a bulk system of two-dimensional organic conductor, α-(BEDT-TTF)₂I₃ salt which consists of four sites of donor molecules in a unit cell. In the present paper, the characteristic of the ZGS is analyzed in detail and the electronic properties are examined in the vicinity of the Dirac point where the conduction and valence bands degenerate to form the zero-gap. The eigenvectors of the energy band have four components of respective sites, where two of them correspond to inequivalent sites and the other two correspond to equivalent sites. It is shown that the former exhibits an exotic momentum dependence around the contact point and the latter shows almost a constant dependence. The density of states of each site close to the Dirac point is calculated to demonstrate the temperature dependence of the local magnetic susceptibility and the local nuclear magnetic relaxation rate. Further, the robust property of the ZGS against the anion potential is also shown by using the second-order perturbation.     

Improved synthesis of polyfluorinated l-lysine for 19F NMR-based screening

Polyfluorinated N-α-Fmoc--Boc-l-lysine represents the best-in-class among a set of polyfluorinated amino acids (PFAs) which are useful tools for ¹⁹F NMR-Based Screening. In this communication, optimized reaction conditions that allowed for the multi-gram preparation of this unnatural amino acid are reported.     

A study of the evaporative deposition process: Pipes and truncated transport dynamics

We consider contact line deposition of an evaporating thin drop. Following Dupont’s proposal (unpublished), we focus on transport dynamics truncated by a maximal concentration as the single deposition mechanism. The truncated transport process, formalized as the “pipe model”, admits a characteristic shock front that has a robust functional form and depends only on local hydrodynamic properties. By applying the pipe model, we solve the density profile in different asymptotic regimes. In particular, we find that near the contact line the density profile follows a scaling law that is proportional to the square root of the concentration ratio defined as the initial solute volume concentration divided by the maximal concentration. The maximal deposit density occurs at about 2/3 of the total drying time for uniform evaporation and 1/2 for diffusion-controlled evaporation. Away from the contact line, areal density decays exponentially with the radial distance to the power of -3 for the uniform evaporation and -7 for the diffusion-controlled evaporation.