不同pH条件下木质素磺酸钠的静电逐层自组装研究

以来源于造纸废液中的木质素磺酸钠(SL)为研究对象,利用静电逐层自组装技术,与聚二烯丙基二甲基氯化铵(PDAC)交替吸附,制备木质素磺酸钠的自组装多层吸附膜.研究了不同pH值条件下木质素磺酸钠在固体表面的静电吸附规律.木质素磺酸钠的自组装过程用紫外-可见光吸收光谱来监控,而自组装膜的表面形貌用原子力显微镜来观察.研究表明,SL与PDAC多层吸附膜的紫外-可见光吸收光谱强度随层数增加而线性增长,说明SL/PDAC多层吸附膜的厚度增长是以逐层自组装的方式进行的.木质素磺酸钠浸渍溶液的pH值对多层吸附膜的厚度和表面形貌产生重要的影响.在所研究的pH范围内,pH值越低,越有利于生成吸光度高的自组装膜,而得到的自组装膜的表面粗糙度越大。     

Eddy current septum magnets for injection and extraction at SSRF

There are 6 in-vacuum eddy current septum magnets used for booster injection, extraction, and storage ring injection in SSRF. Special attention was paid to coils and their support designs because of the shock force they bear in the magnetic fields and the high heat which is hard to be dissipated in vacuum environment. For the storage ring magnets, good transverse homogeneity in the gap was achieved by careful design, precise machining and accurate assembly; and an extremely low leakage field on the stored beam is another key feature thanks to the high permeability Mu metal. Magnetic field measurement was conducted with both a point coil and a long integral coil, and the results agree well with the OPERA-2d/3d simulations. An inner tube is added to keep the continuity of impedance for the circulating beam with two RF finger flanges at each end. There is no vacuum separation between the inner tube and the magnet chamber. Sputter ion pumps integrated with NEG are used to acquire the UHV for the chamber.     

节能情形下制造企业动态批量生产策略与节能方式选择

随着诸多严厉的环保政策的实行,节能管理已成为我国高耗能制造企业运营管理中的一个重要内容。通过构建自我节能、节能效益分享和节能量保证三种节能方式下制造企业的动态批量生产决策模型,首先分析了给定节能方式下制造企业的最优动态批量生产策略,其次探讨了制造企业最优节能方式选择。结果表明,最优动态批量生产策略满足“零库存生产”规则。进一步的数值实验分析结果表明:面临前两种节能方式时,当节能服务公司与制造企业的节能投资成本系数比率和采用合同能源管理的预计节能率较小时,制造企业应选择后者,反之应选择前者;面临后两种节能方式时,当采用合同能源管理的预计节能率较小时,制造企业选择两者无差异,反之应选择前者。     

被动遥测光谱仪仪器响应函数的实验测定研究

被动遥测光谱技术在目标光谱探测、大气痕量气体监测等方面都有广泛的应用.为了得到准确和高灵敏度的遥测光谱测试数据,被动遥测光谱设备必须首先进行响应函数的测量,以消除仪器本身热量对测量数据的影响.利用标准高温黑体对BLUKER TENSOR 37型被动式FTIR光谱仪仪器响应函数进行了测定,得到了该型仪器在不同温度区间MCT探测器和InSb探测器仪器的响应函数和背景函数.实验发现MCT探测器响应函数随温度升高而增加,而InSb探测器则相反,随温度升高略有减小.背景函数不仅与背景相关,还与温度相关.MCT探测器背景函数随温度的升高而减小,而InSb探测器则相反,随温度升高而增加.     

CS2在Ｃ6H6中的弱费米共振特性及对Bertran公式修正

通过测量CS₂在C₆H₆中不同浓度的拉曼光谱,观察到了纯CS₂与溶液中的v₁—2v₂费米共振明显不同.用Bertran方程,计算了费米共振特性参数.结果表明,随着CS₂浓度降低,两光谱强度比R=I_v1/I_2v2减小,耦合系数W增加,其他参数 关键词： 拉曼光谱 费米共振 溶剂效应 二硫化碳     

Octave-spanning visible supercontinuum generation from an aluminum nitride single crystal pumped by a 355 nm nanosecond pulse

Supercontinuum generation(SC) of more than one octave spectrum spanning covering from 400 nm to 820 nm was achieved by pumping a piece of aluminum nitride(AIN) single crystal using a nanosecond 355 nm ultraviolet laser. The AlN with a thickness of ~0.8 mm was grown by an optimized physical vapor transport technique and polished with solidification technology. Compared to previously reported ones, the achieved visible SC exhibited the broadest spectrum spanning from bulk materials pumped by a nanosecond pulse laser. The visible supercontinuum in Al N presents new opportunities for bulk material-based white light SC and may find more potential applications beyond typical applications in integrated semiconductive photoelectronic devices.     

高能电子碰撞电离对高空核爆炸辐射电离的影响

利用数值模拟程序模拟了不同高度核爆炸下距离爆点不同位置处大气的X射线电离及演化过程,分析了高能电子碰撞电离过程对高空核爆炸电离效应的影响.结果表明:高能电子碰撞电离过程对高空核爆炸的电离结果产生了重要影响,在80 km爆高1 kt当量高空核爆炸条件下,在距离爆点1.5 km处高能电子的碰撞电离效应使得电子的峰值数密度提高了约2个数量级;随着时间的增加,高能电子能谱逐渐向低能方向发展,在5μs后高能电子数密度随电子能量近似呈负指数分布;电子峰值时间与爆高有关,随着爆高的增加而增大,电离的影响区域也随着爆高的增加而增大.在80 km爆高1 kt当量情况下电离效应对近百千米范围内的微波通信具有严重影响.     

分光光度法测定氨基羟基脲

建立了Fe(Ⅱ)-邻菲啰啉显色法测定HNO3体系中氨基羟基脲(HSC)的方法。在乙酸/乙酸钠缓冲体系中,HSC与Fe(Ⅲ)反应生成的Fe(Ⅱ)能与邻菲啰啉形成稳定的络合物,该络合物的最大吸收波长在510 nm。考察了缓冲溶液用量、反应时间等条件对吸光度(A)的影响。结果表明:HSC浓度在5~60μmol/L范围内遵循比尔定律,线性回归方程为:A=0.0292 cHSC(μmol/L),相关系数R2=0.9993。方法用于实际样品测定,加标回收率在100.1%~104.4%之间,检出限为3.8×10-2μmol/L,相对标准偏差0.04%~0.12%,满足HSC分析的需求。     

OSCILLATION CRITERIA FOR A CLASS OF HIGHER ORDER NEUTRAL DIFFERENTIAL EQUATIONS

We establish a new oscillation condition for even order neutral type differential equation of the following formwhere f is continuous and exists 1 ≤ k ≤ m(?)(t) ≡ Tk(t), a, (?)i ∈ C([0, ∞], R), i = 1, …,m. such that 0 ≤ a(t) ≤ L and