Pair Production in Chromoelectric Field with Back Reaction

Massless quark pair production in SU(2) gauge chromoelectric field is investigated by solving the Wigner function with back reaction. The temporal evolution of specific field and its current are obtained self consistently. For the quark distribution function, both its time and momentum dependence are studied. In particular, some interesting phenomena are found, for example, the more abundant symmetry or/and antisymmetry characteristics, the existence of the attractive basin structure and the existence of the momentum "gap" in the quark distribution and so on. All the phenomena are associated with the quark-gluon plasma oscillation, which due to the back reaction effect. The study and analysis qualitatively about the components of the Wigner function are expected to be helpful to deepen the understanding of the QCD vacuum.     

The Interaction of Peregrine Solitons

We theoretically investigate the interaction of two in-phase and out-of-phase Peregrine sofitons in a Kerr nonlinear medium, addressing both the cases of first- and second-order solitons. Upon adjusting the interval between the sofitons, their interactions exhibit different properties. If the interval is sufficiently large, two Peregrine sofitons will propagate individually and will not interact each other. However, if the interval is not very large, the Peregrine solitons will strongly interact and display varying behavior.     

Fourth-Order Spatial Correlation of Thermal Light

We investigate the fourth-order spatial correlation properties of pseudo-thermal light in the photon counting regime, and apply the Klyshko advanced-wave picture to describe the process of four-photon coincidence counting measurement. We deduce the theory of a proof-of-principle four-photon coincidence counting configuration, and find that if the four randomly radiated photons come from the same radiation area and are indistinguishable in principle, the fourth-order correlation of them is 24 times larger than that when four photons come from different radiation areas. In addition, we also show that the higher-order spatial correlation function can be decomposed into multiple lower-order correlation functions, and the contrast and visibility of low-order correlation peaks are less than those of higher orders, while the resolutions all are identical. This study may be useful for better understanding the four-photon interference and multi-channel correlation imaging.     

运用三重排除法巧定线圈感应图

有关线圈在磁场中运动的电磁感应图像选择题,由于图形复杂多变,常规的数学分析法需要列大量的表达式,很难快速作答,如果运用三重排除法分析就能很快确定答案。     

Y型微通道两相流内部流动特性刘

利用显微粒子图像测速技术、高速度数码显微系统及数值模拟方法研究了Y 型微通道内液滴的形成. 主要考虑了Y 型角度（45°,90°,135°,180°）、两相流量大小等因素的影响. 发现在挤压机制中,Y 型微通道内分散相液滴的形成主要受到来自连续相的剪切作用,Y 型角度越小,分散相所受到的剪切作用越大. 在液滴生成过程中,连续相速度剖面呈非对称抛物线型分布. 当Y 型角度小于180°时,角度的变化对液滴直径大小影响较小,但角度的减小会加快液滴的生成时间. 当Y 型角度为180°时,生成的液滴体积最大且生成时间最长. 毛细数对液滴直径和生成时间的变化同时产生影响,连续相毛细数的增大使得连续相在两相交汇位置处对分散相的作用力更集中,导致分散相更易破裂.     

爆轰法合成纳米CeO粉末*2

爆轰合成过程中采用Ce(NO₃)₃·6H₂O制备的可爆药剂,并利用X射线衍射仪(XRD)和透射电子显微镜(TEM)对合成的纳米CeO₂粉末进行了检测,研究了起爆方式对于合成产物结晶化度、粒径和形貌的影响。结果表明,采用Ce(NO₃)₃·6H₂O制备的可爆药剂,可以合成立方晶系的球形纳米CeO₂; 提高可爆药剂的爆速,可有效降低纳米CeO₂的粒径,得到球形化更好的纳米粒子。     

白藜芦醇类似物与人血清白蛋白的相互作用

采用荧光光谱、三维荧光光谱、紫外吸收光谱研究白藜芦醇类似物(Z)-2-(3,4-二甲氧苯基)-3-(4-二甲氨基苯基)丙烯腈(HCQ)与人血清白蛋白(HSA)的相互作用,探讨其作为抗肿瘤药物的可能。结果发现HCQ与HSA形成了基态配合物,HCQ主要结合于HSA的位点Ⅰ,与位点Ⅱ也有微量的结合,反应为自发的放热反应,其ΔH、ΔS、ΔG均小于零,二者之间的结合力为氢键或者范德华力,结合常数为104～105数量级。HCQ与HSA的结合使HSA构象发生变化,Trp-214所处的环境疏水性增加,使得其内源性荧光显著降低。说明合成的白藜芦醇类似物能够与人血清白蛋白结合。     

极化诱导实现AlGaN薄膜材料中的超高电子浓度(1020cm-3)掺杂

材料的载流子浓度和迁移率是影响器件性能的关键因素, 变温Hall测试结果证明杂质掺杂AlGaN中的载流子浓度和迁移率随温度 降低而减小.然而极化诱导掺杂的载流子浓度和迁移率不受温度变化的影响.以准绝缘 的GaN体材料作为衬底, 在组分分层渐变的AlGaN中实现的极化诱导掺杂浓度 仅仅在10¹⁷ cm^-3数量级甚至更低. 本研究采用载流子浓度为10¹⁶ cm^-3量级的非有意n型掺杂GaN模板为衬底, 用极化诱导掺杂技术在分子束外延生长的AlGaN薄膜材料中实现了高 达10²⁰ cm^-3 量级的超高电子浓度. 准绝缘的体材GaN半导体作衬底时, 只有表面自由电子作为极化掺杂源, 而非有意掺杂的GaN模板衬底除了提供表面自由电子外,还能为极化电场 提供更多的自由电子"源", 从而实现超高载流子浓度的n型掺杂.     

可燃液体爆燃特性及其抑制实验

设计了一套可燃液体爆炸特性实验装置,利用该装置和立式爆轰管对RP-5油料、RP-3油料及工业酒精的爆炸特性、1301惰性气体对这3种燃料的抑制进行了研究。结果表明:RP-5油料、RP-3油料及工业酒精爆炸的体积分数范围分别为1.53%～7.73%、0.82%～7.17%及 3.38%～18.25%;酒精云雾爆轰的临界起爆能为2.11 MJ/m2、爆速和爆压分别为1 609 m/s 、1 480 kPa,爆轰波传播的胞格宽度为14.5 mm,长度为16.2 mm。1301惰性气体对RP-5油料、RP-3油料及工业酒精的最小惰化体积分数分别为6.75%、6.8%及 5.56%;二氧化碳和氮气对RP-3油料的最小惰化体积分数分别为45%和49%;1301惰性气体对油料爆炸抑制效果明显好于二氧化碳与氮气。