高功率密度软X射线在X光导管中传输效率测量

为优化软X射线聚束透镜设计参数,使之与等离子体辐射源组合来获得洁净的高功率密度宽能带的软X光束,在西北核技术研究所的强光一号加速器装置上,对高功率密度的软X射线（6×10^6～1．5×10^7W／cm^2）在X光导管中的传输特性进行研究。研究结果表明：对于DM308型号玻璃材料拉制成的X光导管,在该功率密度范围内,软X射线在X光导管中的传输没有出现非线性效应,随着入射软X射线功率密度的提高,出射软X射线功率密度基本成线性增大;当入射软X射线的功率密度为1．2×10^7W／cm^2时,实验中获得X光导管的平均传输效率达到了16．3％。在强光一号加速器装置上,使用由该规格X光导管制作的软X射线聚柬透镜与钨丝阵Z-pinch等离子体辐射源组合,获得了功率密度达2．1×10^9W／cm^2的宽能带的软X光源。     

关于OTF比较计算的建议

七十年代初期,随着电子计算机在光学计算上的应用,国内一些单位先后开始了光学传递函数(OTF)的计算工作。OTF的计算工作与国外相比我们起步大约晚十年,经过十多年的努力,我们与国外的差距正在逐步缩小。目前,编制了OTF程序的单位已有二十个左右,至于使用OTF程序的单位就更多了。     

湿空气的比相对湿度和通用焓湿图

本文提出了比相对湿度的概念,给出了在宽广的参数范围内计算湿空气热力性质的精确公式,并在此基础上绘制了可用于不同压力的通用焓湿图,为空调、干燥等技术中各种湿空气过程的热力计算提供了方便条件。     

瓶颈开口角对二维颗粒流的影响

实验研究了平面传送带上颗粒流的特性，主要包括传送带出口处开口宽度以及瓶颈开口角度对颗粒流的影响.实验结果发现，改变瓶颈开口角度θ，当θ大于15°时，颗粒流量Q随着cosθ呈线性变化.同时，颗粒流量Q与传送带速度v以及开口大小R也密切相关，而在θ小于15°时，颗粒流量Q基本不随开口角度变化.     

强光一号装置单氘丝中子发射实验研究

 介绍了利用飞行时间技术测量Z箍缩装置单氘丝中子发射。实验发现，Z箍缩中子发射过程中,伴随产生很强的硬X射线，利用铝丝阵产生硬X射线的实验，建立较好的硬X射线屏蔽,大大减弱了它的辐射强度。所采用的双闪烁探测器中子探测系统，进行了3个发次的单氘丝负载实验，确认产生了聚变氘氘中子。4172发次实验测量结果表明，中子产额1.5×10⁹，中子能量为(2.45±0.26) MeV。实验结合分幅照相数据分析认为，峰电流和负载未能很好匹配，等离子体存在不稳定现象。     

丝阵Z箍缩实验1维X光辐射功率分布

 在Angara-5-1联合实验中，利用条纹像机和光纤阵列实现时间分辨和1维空间分辨，得到了丝阵条纹像，观察到丝阵负载箍缩区X光辐射的1维轴向空间分布信息随时间的演化过程，考察了内爆的同步性和均匀性。通过对比不同结构负载内爆等离子体X光1维时空分布信息，发现由于内层等离子体对磁流体瑞利-泰勒不稳定性的抑制作用，(40+20)根双层钨丝阵比60根单层钨丝阵的内爆轴向同步性好，产生的X光辐射功率高；由于负载存在弯曲、断丝、扭曲等现象，(60+30)根双层钨丝阵比90根单层钨丝阵的轴向同步优势不明显；轴向同步性好与辐射功率高之间存在相关性；辐射波形前沿较快时，X光功率较高。     

Isoscaling in Statistical Sequential Decay Model

A sequential decay model is used to study isoscaling, i.e. the factorization of the isotope ratios from sources of different isospins and sizes over a broad range of excitation energies, into fugacity terms of proton and neutron number, R21（N, Z） = Y2（ N, Z）/Y1（ N, Z） = Cexp（αN -βZ）. It is found that the isoscaling parameters α and β have a strong dependence on the isospin difference of equilibrated source and excitation energy, no significant influence of the source size on α andβ has been observed. It is found that α and β decrease with the excitation energy and are linear functions of 1/T and △（Z/A）2 or△（N/A）2 of the sources. Symmetry energy coefticient Gsym is constrained from the relationship of a and source △（Z/A）2, /3 and source △（N/A）2.     

First-Principles Study of Electronic Structure of the Laves Phase ZrFe2

We perform the ab initio calculation for obtaining the density of states and magnetic properties of ZrFe2 Laves phase compound based on the method of augmented plane waves plus local orbital The results indicate that the ferromagnetic state is more stable than the paramagnetic one, but with a slightly larger volume. The 3d - 4d exchange interactions between Fe and Zr electrons lead to the antiparallel coupling for Fe 3d and Zr 4d states, which is responsible for the ferrimagnetic ordering of the compound. The resulting magnetic moment of about 1.98μB for Fe is spatially localized near the Fe site, while around Zr a small but extended negative spin states causes a moment of about -0.44 μB. Moreover, the resulting magnetic moments with the generalized gradient approximation are more consistent with experimental values than that of the local-spin density approximation.     

Electrochemical Deposition and Properties of ZnTe Nanowire Array

Pulsed electrodeposited technique is applied to fabricate ZnTe nanowire arrays with different diameters into the anodic alumina membrane in citric acid solution. The x-ray powder diffraction, scanning electron microscopy and transmission electron microscopy indicate that the high ordered, uniform and single-crystalline nanowires have been fabricated. The optical absorption spectra of the nanowire array show that the optical absorption band edge of the ZnTe nanowire array exhibit a blue shift compared with that of bulk ZnTe, and the nonlinear current-voltage characteristic is observed.     

Flat Supercontinuum Generation at 1550 nm in a Dispersion-Flattened Microstructure Fibre Using Picosecond Pulse

The generation of a flat supercontinuum of over 80nm in the 1550nm region by injecting 1.6ps 10 GHz repetition rate optical pulses into an 80-m-long dispersion-flattened microstructure fibre is demonstrated. The fibre has small normal dispersion with a variation smaller than 1.5 （ps·nm^-1·km^-1） between 1500 and 1650nm. The generated supercontinuum ranging from 1513 to 1591 nm has the flatness of ±1.5 dB and it is not so flat in the range of several nanometres around the pump wavelength 1552nm. Numerical simulation is also used to study the effect of optical loss, fibre parameters and pumping conditions on supercontinuum generation in the dispersion-flattened microstructure fibre, and can be used for further optimization to generate flat broad spectra.