双模相干态和压缩真空态光场-非等同两原子体系的腔场谱

研究了两个非等同二能级原子与双模腔场相互作用过程的腔场谱.导出了双模初始光场处于任意量子态时腔场谱的计算公式,给出了光场处于相干态和压缩真空态时的数值结果,讨论了相对耦合常数R=g2/g1和初始场强对腔场谱的影响.发现相干态光场的腔场谱在R很小时为双峰,在R接近于1时为3峰.压缩真空态的腔场谱在弱场条件下表现为复杂的多峰结构,在强场条件下则只有单一经典共振峰或裂距很小的双峰.     

基于顾客低碳行为偏好的选址-路径-库存集成优化模型与算法

针对自愿减排驱动下的顾客低碳行为偏好对选址-路径-库存决策的影响进行研究。首先推导了顾客低碳行为偏好下的市场需求函数和价格函数,并构建了考虑单位产品碳排放量和经济成本的多目标选址-路径-库存优化模型,通过对多目标优化模型的求解可得碳排放量和经济成本间的Pareto解集。在此基础上,定义了碳配额税的概念,可得顾客低碳行为偏好和碳配额税下的总收益函数。最后通过数值分析给出了自愿减排和监管减排两种机制共同作用下的企业减排方案和灵敏度分析。     

液体燃料云雾爆轰参数实验

为深入了解液体燃料云雾爆轰机理,借助自行设计和建造的立式爆轰管,并采用升降法和烟迹技 术,对环氧丙烷等液体燃料云雾爆轰参数(爆速、爆压、临界起爆能和爆轰胞格尺寸)与当量比的关系进行了实 验研究。结果表明,环氧丙烷的爆速和爆压随当量比的增加先增大后平缓减小;碳氢液体燃料云雾爆轰的临 界起爆能与当量比呈U型关系,最佳值点偏向富燃料一侧;临界起爆能的大小与燃料的分子结构和挥发性 有密切关系,IPN和PO 临界起爆能相当,而烷烃类临界起爆能均较大。环氧丙烷在25和50 ℃时的爆轰胞 格宽度与当量比皆呈U型关系,最小值点偏向富燃料一侧;气相爆轰胞格宽度比云雾爆轰略小。常温下环 氧丙烷云雾爆轰主要由气相反应所控制。     

半寿命低周疲劳Glidcop?材料导热系数的测量

针对上海同步辐射装置（SSRF）光束线前端挡光元件需要承受高热负载的要求,对挡光元件所使用的纳米Al2O3颗粒增强Cu基复合材料Glidcop,采用一维稳态纵向热流法测量其在不同应变状态下的热传导系数。用有限元模拟了试件的温度场分布,并对试验结果进行了误差分析,揭示了试验误差的主要来源。试验测量结果表明,经历半寿命低周疲劳循环所产生的应变损伤累积对Glidcop导热系数的影响可以忽略。     

Stark效应对双模压缩真空场与原子耦合系统腔场谱的影响

研究了Stark效应对两模双光子J-C模型腔场谱的影响,推导计算出了腔场处于压缩真空态时腔场谱的计算公式和数值结果,讨论了Stark效应和初始场强对腔场谱的影响.发现初始场较弱时,Stark效应主要影响谱线的频率,对峰的强度影响不大;初始场n1=n2≥2后,Stark效应对主峰有较强的强化作用,对边峰产生抑制作用;在初始场较强时,对谱强度的影响显著.改变Stark移动参数和初始场的强度,可得到各式各样的腔场谱结构.     

Kerr介质腔中非线性J-C模型的腔场谱

研究了Kerr介质腔中非线性J-C模型的腔场谱.导出了初始光场处于任意量子态时腔场谱的计算公式,给出了光场处于数态、相干态和压缩真空态时的数值结果,讨论了Kerr效应和初始场强对腔场谱的影响.发现在光子数态的情况下,n≠1时均为2峰结构,Kerr介质使得中心频率按x(2n-1)的规律向高频方向移动,并破坏谱结构的双峰对称性;在相干态和压缩真空态情况下,当Kerr效应较弱时,非线性J-C模型中腔场谱的非经典特性较为突出,Kerr效应较强时,呈现多峰结构,谱的结构特征主要由Kerr效应决定,由于原子与腔场的耦合被抑制,腔场谱的非线性特征趋于消失.     

Preliminary study of residual orbit oscillation in BEPCⅡ

BEPCII has two rings each with an injection system. The injection system of each ring consists of two kicker magnets and a septum magnet. The injection layout of two rings is the same. Both two kickers would kick the beam in horizontal plane. The betatron phase advance in the horizontal plane between two kickers is designed exactly 180° in order to reduce the perturbation to the circulating beams during injection. In fact, the residual orbit oscillation will originate because of the existence of a variety of errors. The Librea Electron BPM processor is used to acquire the beam position data in turn-by-turn mode and to analyze the residual orbit oscillation. According to the measurement results, minimization of the residual orbit oscillation can be done by adjusting the peak field strength and trigger timing delay of two kickers. With very small residual orbit oscillation the two beams can keep collision condition during the injection.     

Effect of Rolling Massage on Particle Moving Behaviour in Blood Vessels

The rolling massage manipulation is a classic Chinese massage, which is expected to eliminate many diseases. Here the effect of the rolling massage on the particle moving property in the blood vessels under the rolling massage manipulation is studied by the lattice Boltzmann simulation. The simulation results show that the particle moving behaviour depends on the rolling velocity, the distance between particle position and rolling position. The average values, including particle translational velocity and angular velocity, increase as the rolling velocity increases almost linearly. The result is helpful to understand the mechanism of the massage and develop the rolling techniques.     

DCD格式在破碎发射药床两相流内弹道计算中的应用

利用DCD(dispersion controlled dissipative scheme)格式,提出了一种研究发射装药发射安全性问题的两相流内弹道计算方法。将内弹道气固两相流动力学方程组中与压力有关的项进行变形,实现了用同一种格式对气相和固相统一处理,而无须分别对待,采用DCD格式无须数值粘性和人工滤波,提高了计算精度。实例计算了某榴弹内弹道两相流动力学,计算结果与实验结果吻合较好。把破碎发射药床视为混合装药结构,用DCD格式计算了发射药床不同破碎程度对发射安全性的影响。计算结果表现出了通常计算方法难以反映的破碎发射药床内弹道压力极为剧烈的变化过程和极高的危险膛压。 更多还原     

Effect of cavity dissipation on the emission spectrum of an atom interacting with a field in the dispersive approximation

The emission spectrum of a two-level atom interacting dispersively with a single mode radiation field in the dissipative cavity is investigated. A general expression for the emission spectrum is derived. The numerical results for the initial field in coherent state are calculated. It is found that the spectrum structure is influenced significantly by the cavity damping constant \kappa , and the spectrum structure is dependent on the interaction time T when the cavity dissipation is present. Only one peak located at Ω_a appears in the atomic spectra for larger T.