Cl/HN3/I2全气相化学激光体系的化学动力学模拟计算

 对Cl/HN₃/I₂产生NCl(a)/I激光的过程进行了化学动力学计算，主要考察了Cl,HN₃和I₂的初始粒子数密度及其配比对小信号增益系数的影响。结果发现,当温度为400K, 初始Cl粒子数密度为1×10¹⁵，1×10¹⁶和1×10¹⁷cm^-3时,小信号增益系数分别达到1.6×10^-4,1.1×10^-3和1.1×10^-2cm^-1，获得最佳小信号增益系数的HN₃和I₂的初始粒子数密度分别为初始Cl粒子数密度的1～2倍和2%～4%。同时，对Cl，HN₃和I₂配比对小信号增益系数和增益持续时间的影响进行了讨论。     

用于高功率激光装置中的电脉冲整形系统

采用射频GaAs场效应管和微带传输线技术,研制出用于高功率激光装置中的电脉冲整形系统.该系统电脉冲整形宽度为3.5 ns,幅度在0~5 V范围内调节,时域调整精度200 ps.整形后的方波,前沿383 ps,后沿642 ps,顶部不平坦度4~5%,波形幅度稳定性4~5%（p-p).利用该系统产生的整形电脉冲驱动电光波导调制器进行激光脉冲整形,得到了理想的整形激光脉冲.     

皮秒脉冲功率技术理论模型及其优化设计

为了产生100~500 ps,200~500 kV,1~10 kA数量级的皮秒放电脉冲,建立了一个皮秒脉冲发生器理论模型,并提出利用增益系数极值法,确定其最大兼容工作点,相对于纳秒脉冲成形线,皮秒脉冲成形线实现了90%,70%,85%的归一化电压增益、能量增益和放电功率增益。为了最大限度地降低皮秒脉冲成形线的载压时间,提高系统的绝缘安全因子,利用华罗庚0.618优算法,设计了电压传输系数。在纳秒脉冲成形线与皮秒脉冲成形线阻抗比值等于1.63条件下,在4倍和6倍皮秒脉冲成形线时间之内,归一化电压增益、能量增益和放电功率增益就可以分别达到94%,72%,89%与99%,53%,97%。     

稀土掺杂ABS防激光玻璃的制备及其结构研究

在稀土掺杂碱硼硅酸盐(ABS)玻璃形成能力研究的基础上,采用核磁共振NMR、红外激光拉曼光谱等测试手段研究该种玻璃的结构特征。研究结果表明,[SiO4]2-、[BO4]5-和[BO3]3-等结构单元通过[SiO4]4--[BO4]5-、[BO4]5--[BO3]3-、[BO3]3--[SiO4]4-等连接方式构成了玻璃网络结构,形成了巨大的介稳体系,稀土Sm3+等阳离子则填充在网络空隙之中。光谱研究结果表明,Sm3+掺杂ABS玻璃对1.06μm波长的激光具有很强的吸收,当稀土含量达到20mol%时,玻璃在1.06μm波长的透过率仅为0.03%。     

高位K2(1Λg) 与基态原子的碰撞转移

在K原子密度约为0.5～5×1016cm-3的样品池中,脉冲激光710 nm线双光子激发K2基态到高位1Λg态,研究了K2(1Λg)+ K(4S)碰撞转移过程.K原子密度由测量KD2线蓝翼对白光的吸收得到.测量不同K密度下1Λg态发射的时间分辨荧光强度,它是一条指数衰减曲线,由此得到1Λg态的有效寿命,从描绘出的有效寿命倒数与K原子密度关系直线的斜率得到1Λg态总的碰撞猝灭截面为(2.1±0.2)×10-14cm2,从截距得到的辐射寿命为(22±2)ns.测量了K的6S →4P3/2和4D→4P3/2在不同K密度下的时间积分荧光强度,得到了K2(1Λg)+K→K2(11∑ +g)+K(6S,4D)碰撞转移截面为(1.5±0.3)×10-15cm2(对转移到6S)和(8.5±3.0)×10-15cm2(对转移到4D).     

Study of weakly-bound odd-A nuclei with quasiparticle blocking

The coordinate-space Hartree-Fock-Bogoliubov(HFB) approach with quasiparticle blocking has been applied to study the odd-A weakly bound nuclei ~(17,19)B and ~(37)Mg,in which halo structures have been reported in experiments.The Skyrme nuclear forces SLy4 and UNEDF1 have been adopted in our calculations.The results with and without blocking have been compared to demonstrate the emergence of deformed halo structures due to blocking effects.In our calculations,~(19)B and ~(37)Mg have remarkable features of deformed halos.     

Dipole bands in nucleus ~(139)pm

High-spin states in nucleus (~139)Pm have been studied using the reaction ~(116)Cd(~(27)Al, 4n)~(139)Pm. Two dipole cascades have been found. Spin and parity assignments were based on the Directional Correlation of Oriented Nuclei (DCO) ratios and systematic behavior in neighboring odd-proton nuclei. The level structures of ~(139)pm are compared with those of the N = 78 isotone ~(141)Eu in which two dipole bands have been confirmed as magnetic rotational bands. The close similarity between them suggests that the dipole bands in ~(139)Pm may be magnetic rotational bands.     

稳定性同位素评价南方膳食结构中铁的吸收率

评价南方膳食结构中铁的吸收率,为我国不同人群、不同膳食类型的铁吸收率提供参考资料。采用~(57)Fe-EDTA或~(57)FeSO4两种铁的稳定性同位素示踪方法,以稀土元素Dy作为排泄物的回收标记物,于现场进行人体代谢试验,受试者为健康成年男子和孕龄妇女各10名,分6次口服3.0mg的~(57)Fe稳定性同位素示踪剂及2.0mg的Dy,粪便监测法收集同位素排出粪样;用电感耦合等离子体质谱仪测定粪样~(57)Fe/~(56)Fe的比值,用原子吸收光谱法测定粪样总Fe,从而计算该人群膳食铁的吸收率。在南方膳食结构中,口服~(57)Fe-EDTA示踪剂,成年男子膳食铁的吸收率为7.34%,孕龄妇女的吸收率为6.92%;口服~(57)Fe-SO4示踪剂,成年男子膳食铁的吸收率为6.01%,孕龄妇女的吸收率为5.40%。本研究结果表明口服~(57)Fe-EDTA评价膳食铁吸收率虽有高于用~(57)FeSO4评价结果的趋势,但无显著性统计分析差异。中国南方城市膳食中铁的吸收率与2000年中国营养学会对我国居民膳食铁吸收率的估计水平大致相当。     

Structural evolution of the intruder band in 118Sn

Excited states of the positive-parity intruder band in~(118) Sn have been studied via the ~(116)Cd(~7Li,lp4n) reaction at ~7Li energy of 48 MeV using techniques of in-beam γ-ray spectroscopy.This intruder band has been observed up to 7187 keV with spin (16~+). The structural evolution of this intruder band with increasing angular momentum has been discussed in terms of the aligned angular momentum and the ratio of the E-Gamma Over Spin (E-GOS) curve.     

双奇核172Re的高自旋

对149Sm(27Al, 4n)172Re反应产生的172Re在束γ的实验数据进行了重新分析, 新发现了可归属于172Re的3个转动带, 由此建立了由6个转动带构成的172Re高自旋态能级纲图。依据相邻核的带结构知识和推转壳模型分析方法, 对新发现的3个转动带的准粒子组态进行了指定, 讨论了它们的转动特征。We have re analyzed the experimental data of in beam γ spectroscopy for 172Re via the 149Sm(27Al, 4n)172Re reaction. Three rotational bands have been newly found and assigned to 172Re. A new level scheme of 172Re, consisting of 6 bands, is thus presented. Based on the existing knowlegde from the neighboring nuclei and the cranked shell model, the quasiparticle configurtions have been assigned to the 3 newly observed bands and their structure properties have been dicussed.     

Discharge in the Atmosphere in a Gaussian Beam of Subthreshold Millimeter Waves

The propagation velocities of a subthreshold discharge excited in air at atmospheric pressure by a pulsed microwave beam with a Gaussian field distribution, a wavelength of 4 mm, and an intensity up to 30 kW/cm² have been measured by means of optical and microwave diagnostics. It has been shown that the motion of a discharge front along the path of the beam toward the region of an increasing microwave field is accompanied by an increase in the velocity from subsonic (~10^–4 cm/s) to supersonic (~(6–8) × 10⁴ cm/s). At the same time, motion toward the decreasing field region is accompanied by a decrease in the velocity from supersonic to subsonic. It has been found that the maximum temperature of the gas in the discharge at velocities of ~10⁴ cm/s reaches ~5.3 kK.     

晕核6He（25 MeV/u）在9Be上的破裂反应

25 MeV/u 6He+9Be反应的实验中利用多个探测器望远镜对反应产物进行了测量, 对实验中各个角度测量到的4He进行观察, 将其中两个有高能峰成分的探测器划分成三部分, 得到不同角度4He的单举能谱和破裂产生4He的微分截面. Different products of 6He nuclei from 9Be target has been measured with a 6He beam at energy of 25 MeV/u. The energy spectra at different angles for 4He isotope were analyzed and the experiment differential cross sections for the direct breakup reaction were obtained.     

PuN基态和低激发态的分子结构与相对论有效原子实势

用Pu的三种不同相对论有效原子实势 (RECP)和密度泛函(B3LYP)方法对PuN基态和低激发态(4Σ+、6Σ+、8Σ+、10Σ+)的分子结构进行了计算,得到了相应的平衡几何构型和谐振频率.采用最小二乘法拟合得到了PuN分子的Murell-sorbie势能函数,在此基础上推导出完整的力常数和光谱数据,并与实验值作对比.结果表明:PuN的基态为X6Σ+,其余为低激发态;在三种RECP中,对于ωe的计算,60个中心电子的SDDRECP/B3LYP给出的结果与实验值符合得比较好(如X6Σ+:ωe=840.77 cm-1,ωeχe=5.73·"cm-1,De=5.880 6 eV,Re=0.176 3 nm,Be=0.408 4 cm-1,αe=3.3E-03 cm-1).计算还给出了相应的电荷布居、自旋密度、电偶极矩和能量特征等系列分子的性质.     

Measurement of 85Rb（n, 2n） 84Rb reaction cross-section from 12 MeV up to 19.8 MeV

The cross-section data of the 85Rb(n,2 n)84Rb reaction have been measured with the neutron energies of 12 MeV to 19.8 MeV using the activation technique and the relative method.The 85Rb samples were irradiated on the surface of a two-ring orientation assembly with neutrons produced from the 3H(d,n)4He reaction at the 5SDH-21.7-MV Tandem accelerator in China.Theoretical model calculations were performed with the TALYS-1.9 code.The present data were compared with previously obtained experimental data and the available evaluated data.     

Laser-particulate interactions in a dusty RF plasma

The interaction of particulates formed in an argon RF discharge containing 1-5% CCl₂F₂ admixture with a pulsed infrared laser (Nd:YAG, intensity ~10⁹ W m^-2, pulse duration ~10^-4 s) has been studied in situ. The white light emitted during this process has been monitored as a function of time and wavelength using a fast photo diode and an optical multichannel analyser. The spectra have been fitted with blackbody curves with a standard deviation of 5%. A spectral temperature of about 3500 K has been obtained for various plasma conditions and attributed to the decomposition temperature of the particulate material. A model based on laser heating, internal heat conduction and chemical decomposition is compared with the experimental results. This model predicts the time constants for heating and decomposition of the particulates and explains the dependence of the measured emission intensity on the laser intensity     

Effect of Weak Magnetic Fields on the Electric Properties of CdTe Crystals

The effect of static and pulsed magnetic fields (~1 T) on the electrical conductivity of CdTe crystals has been revealed. With a delay after the magnetic exposure of crystals, the effect is observed in the form of two peaks of their conductivity with the subsequent relaxation return. The first peak at both types of magnetic treatment is observed ~1 h after exposure and its amplitude exceeds the background value by ~23–36% (the larger value corresponds to the static field). The second peak appears in both cases also at commensurate but much larger delays of ~50–60 h, and its amplitudes are much different for the two types of exposure, exceeding the background by ~60% for the static field and only by ~11% for the pulsed field. Possible mechanisms of the observed effects have been discussed.     

Transport properties of graphene in the region of its interface with water surface

The graphene growth by thermal decomposition of silicon carbide at the temperature of ~1400°C in a high vacuum of ~10^–6 Torr has been optimized. By Raman spectroscopy, the mean thickness of obtained graphene (2–4 single layers) has been estimated and the presence of high-quality graphene areas in the samples has been demonstrated. It has been found out that the four-point resistance of graphene increases in the region of its interface with water approximately by 25%. For the graphene–water interface in the transistor geometry, with variation in the gate-to-source voltage, the field effect corresponding to the hole type of charge carries in graphene has been revealed.     

Core–shell nanophosphor with enhanced NIR–visible upconversion as spectrum modifier for enhancement of solar cell efficiency

A distinct enhancement of upconversion luminescence from core to core/shell (C/S) structure under low flux near infrared (NIR) excitation at 976 nm has been achieved in lanthanide (Er³⁺, Yb³⁺)-doped NaYF₄ core with undoped NaYF₄ shell nanoparticles (NP). A green chemistry approach has been taken to synthesize monodisperse monophasic C/S NP with the core (~20 nm) and shell (~5 nm) crystallizing into cubic phase. Hydrophobic C/S NP have been further made hydrophilic by coating a transparent SHMP layer without affecting luminescence. C/S (NaYF₄: Er, Yb/NaYF₄) NP integrated dye-sensitized solar cell indicated 11.9% enhancement in overall conversion efficiency under AM 1.5 conditions, due to NIR–visible spectrum modification by fluorescent NPs. The results indicate great potential of such upconverting C/S nanophosphor in solar cell applications.     

正硅酸锂陶瓷小球离线释氚实验研究

中国氦冷球床包层(CH HCSB TBM)初步采用Li₄SiO₄陶瓷小球作为氚增殖材料,实验研究了Li₄SiO₄陶瓷小球的中子辐照产氚性能。将冷冻成型法制备的Li₄SiO₄ 陶瓷小球置于反应堆中辐照100min,然后在离线释氚实验平台上进行退火行为研究。实验结果表明,在用He +1% H₂为载气,流速为100mL•min^-1,升温速率为5K•min^-1的实验条件下,氚气(HT+T₂)是Li₄SiO₄陶瓷小球的主要释氚形态,占总氚的70%左右(不包括自由氚中的氚气),在400℃~700℃范围内出现两次释氚峰;氚化水(HTO+T₂O)所占比例小于20%,主要在300℃~500℃的低温段进行释放;氚在800℃前基本释放完,小球退火后的残氚量小于1%。冷冻成型干燥法制备的Li₄SiO₄陶瓷小球在300℃~700℃范围内有较好的释氚性能,氚残留量低,在聚变堆固态氚增殖包层设计中具有一定应用价值。     

皮秒脉冲功率技术理论模型及其优化设计

为了产生100~500 ps,200~500 kV,1~10 kA数量级的皮秒放电脉冲,建立了一个皮秒脉冲发生器理论模型,并提出利用增益系数极值法,确定其最大兼容工作点,相对于纳秒脉冲成形线,皮秒脉冲成形线实现了90%,70%,85%的归一化电压增益、能量增益和放电功率增益。为了最大限度地降低皮秒脉冲成形线的载压时间,提高系统的绝缘安全因子,利用华罗庚0.618优算法,设计了电压传输系数。在纳秒脉冲成形线与皮秒脉冲成形线阻抗比值等于1.63条件下,在4倍和6倍皮秒脉冲成形线时间之内,归一化电压增益、能量增益和放电功率增益就可以分别达到94%,72%,89%与99%,53%,97%。