用于高功率微波器件的永磁体的设计和测试

报道了用于高功率相对论返波管振荡器的永磁体的设计和试制。以Halbach阵列结构为基础, 通过选择高性能的永磁材料, 调整磁钢的充磁方向、排列方式和尺寸, 优化设计了可用于某相对论返波管振荡器的永磁体结构, 其均匀区磁场强度0.98 T。采用粒子模拟方法, 进行了永磁体与返波管振荡器的一体化设计, 设计结果表明：器件输出功率超过1 GW, 设计的永磁体能够满足器件对磁场强度和位形的要求。对永磁体进行了试制和测试, 测试结果为：均匀区磁场0.88 T, 均匀区长110 mm, 磁体重量约306 kg。     

半导体泵浦铯蒸气实现激光输出

采用线宽0.26 nm的Littrow外腔巴条半导体激光器泵浦增益长度8 mm缓冲气体为80 kPa甲烷的铯（Cs）蒸气室,在Cs蒸气室温度120 ℃时,我们获得了394 mW的894.6 nm线偏振Cs蒸气激光,光光效率7.4%,斜率效率11.2%,阈值功率为1.72 W。     

Energetics of a strongly correlated Fermi gas

The energy of the two-component Fermi gas with the s-wave contact interaction is a simple linear functional of its momentum distribution:

     

Ionization effect to plasma expansion study during nanosecond pulsed laser deposition

The dynamic characteristic and effects of plasma play an important role in film growth process of pulsed laser deposition (PLD). Based on numerical hydrodynamic modeling, supposed the laser radiation and partial ionization of the plasma as a dynamic source, we deduce a set of new plasma expansion dynamics equations. Based on which, as an example of carbon target, using finite difference method, the plasma flow dynamics evolvement in vacuum is investigated. Our results show the dynamic partial ionization increases the expansion in all directions, which changes into a new dynamic source for plasma expansion. In the axial direction, because of the collisional interactions between particles, the plume density peak is in the vicinity of the target surface and the acceleration of plasma occurs mainly near the target surface too. In the transverse direction, the plume peak is not near the target, but at the surface. The space expansion distance is far less than the axial direction because there is no high initial velocity component in this direction. The predictions of the plasma expansion action based on the proposed dynamics source assumption are found to be in agreement with the experimental observation.     

Entanglement dynamics of a moving multi-photon Jaynes-Cummings model in mixed states

Using the algebraic dynamical method,the entanglement dynamics of an atom-field bipartite system in a mixed state is investigated.The atomic center-of-mass motion and the field-mode structure are also included in this system.We find that the values of the detuning and the average photon number are larger,the amplitude of the entanglement is smaller,but its period does not increase accordingly.Moreover,with the increase of the field-mode structure parameter and the transition photon number,the amplitude of the entanglement varies slightly while the oscillation becomes more and more fast.Interestingly,a damping evolution of the entanglement appears when both the detuning and the atomic motion are considered simultaneously.     

钕玻璃的热致断裂及泵浦极限

以激光介质的第一主应力为评判标准,依据Griffith微裂纹理论作为断裂临界应力,基于已报道的断裂实验数据和3维、瞬态的有限元计算,建立了预测一定泵浦参数下钕玻璃断裂可能性的Weibull统计模型,同时分析了影响介质泵浦极限的其它因素。结果表明:材料的抛光工艺决定了介质的断裂应力;对于短脉冲大能量方式工作的钕玻璃介质,基于美国2 0世纪9 0年代的抛光水平,1 Hz以下低重频时应优先考虑18 kW.cm-2的泵浦饱和极限,10 Hz以上高重频时应优先考虑介质的断裂极限。     

多壁碳纳米管-Nafion复合膜修饰玻碳电极测定硝苯地平的研究

研制了以Nafion分散羧基化多壁碳纳米管的化学修饰电极(Nafion-MWCNTs/GC),研究了硝苯地平(NIF)在修饰电极上的电化学行为和测定方法。实验结果表明,在0.1mol/LNH3-NH4Cl(pH9.6)溶液中,Nafion-MWCNTs/GC,对NIF具有明显的催化和增敏作用,还原峰电位由-0.85V(裸电极)正移到-0.75V(vs.AgCl/Ag)(修饰电极),灵敏度增加约7倍。对各种实验条件进行了优化。定量测定的线性范围为2.5×10-7~4.5×10-5mol/L,r为0.9974;检出限为8.0×10-8mol/L。探讨了NIF在Nafion-MWCNTs/GC上的电极过程和反应机理,测得在本体系中参与反应的质子数和电子转移数均为4,电子转移系数α为0.41。对NIF药片进行了测定,回收率为94.5%~101.0%。     

KdV-Burgers方程的级数解

给出ＫｄＶ－Ｂｕｒｇｅｒｓ方程的有界行波解的精确级数解,采用Ａｄｏｍｉａｎ算子分解法分别求行二个区域ζ〈０和ζ〉０的级数解,然后利用对接连续条件构成整体级数解。所得级数解能精确满足对接连续条件,并由此得到确定级数的系数递推公式,无需解非红性高阶代数方程组。与某些精确解及其它方法比较,计算简捷具在对接点处是收剑的。对某些非线性波动现象的研究,可作为计算和分析的数学依据。     

受激双层石墨烯量子点中的激子耦合动态变化

有机聚集体中分子间相互作用决定了聚集体的光物理性质,从而显著影响基于此类材料的光伏器件性能. 分子间激子耦合(或电偶极耦合)是一种常见且重要的分子间相互作用. 本文利用瞬态吸收光谱研究了石墨烯量子点二聚体(一种大稠环芳烃的π-π堆叠二聚体)中的激子耦合作用. 发现了瞬态吸收谱随泵浦-探测延时的演化起源于二聚体激发态中激子耦合强弱的动态变化. 通过拟合瞬态光谱,进一步证实了可利用最低能量的两个振动吸收峰的瞬态吸收动力学直接表征二聚体中激子耦合强度的动态变化.     

Lattice-BGK approach to simulating granular flows

Many continuum theories for granular flow produce an equation of motion for the fluctuating kinetic energy density (granular temperature) that accounts for the energy lost in inelastic collisions. Apart from the presence of an extra dissipative term, this equation is very similar in form to the usual temperature equation in hydrodynamics. It is shown how a lattice-kinetic model based on the Bhatnagar-Gross-Krook (BGK) equation that was previously derived for a miscible two-component fluid may be modified to model the continuum equations for granular flow. This is done by noting that the variable corresponding to the concentration of one species follows an equation that is essentially analogous to the granular temperature equation. A simulation of an unforced granular fluid using the modified model reproduces the phenomenon of clustering instability, namely the spontaneous agglomeration of particles into dense clusters, which occurs generically in all granular flows. The success of the continuum theory in capturing the gross features of this basic phenomenon is discussed. Some shear flow simulations are also presented.