NONCOMMUTATIVE ORLICZ-HARDY SPACES

Let(Φ, Ψ) be a pair of complementary N-functions and HΦ(A) and HΨ(A) be the associated noncommutative Orlicz-Hardy spaces. We extend the Riesz, Szeg and innerouter type factorization theorems of Hp(A) to this case.     

求解一维热传导方程数值解的高精度方法

利用加权隐格式，在固定网比的前提下，得到修正加权因子θｏｐｔ，利用此θｏｐｔ，利用此θｏｐｔ求解一维热传导方程所得到的数值解，同Ｃｒａｎｋ－Ｎｉｃｈｏｌｓｏｎ格式求得的数值解相比，具有更高的精度，并在此基础上，在一定的加细划分下求解，同时得到了较好的高精度数值解。     

光子晶体液体浓度传感器

为了有效地检测混合液体的浓度,运用平面波展开法与光子晶体禁带理论,研究了光子晶体禁带宽度和混合液体浓度的对应关系。以砷化镓(GaAs)为背景材料的三角格子空气孔二维光子晶体内分别填充不同浓度的水醋酸、水甲醇混合液体,讨论了混合液体浓度与介电常数对二维光子晶体禁带宽度的影响。模拟结果表明,在温度保持不变的情况下,浓度在0～0.60mol/kg之间变化时二维光子晶体TE模没出现光子晶体禁带而TM模出现的光子晶体禁带宽度随着混合液体浓度和介电常数的增大而逐渐变窄且向高频区域移动。这一结果为生物化学中混合液体浓度的检测方面提供很好的参考依据。     

不确定度在物理实验中的应用

目前，新疆大学物理实验的数据处理中还未采用测量不确定度这一概记念，本文从不确定度的基本概念出发，介绍在物理实验中的实际应用。     

光子晶体空气孔中质量分数对其禁带宽度影响的仿真分析

为了掌握光子晶体空气孔中液体质量分数对禁带宽度的影响,利用平面波展开法研究了由椭圆形空气孔介质周期性排列的长方晶格光子晶体在不同偏振模式下的禁带宽度。数值模拟显示:溶液的质量分数变化与光子晶体带隙宽度或输出功率变化接近线性关系,而线性相关程度受填充空气孔内液体质量分数的影响。进行了多组参数比对与优化,最终获得了线性度最高的禁带宽度和输出功率与溶液质量分数的对应关系。基于这个对应关系,提出了基于光子晶体带隙宽度测量的溶液质量分数检测方法。该方法可被应用于各蛋白质聚集探测、快速检测气体或液体质量分数、DNA检测等领域。     

Ultrabright γ-ray emission from the interaction of an intense laser pulse with a near-critical-density plasma

An efficient scheme for generating ultrabright γ-rays from the interaction of an intense laser pulse with a near-critical-density plasma is studied by using the two-dimensional particle-in-cell simulation including quantum electrodynamic effects. We investigate the effects of target shape on γ-ray generation efficiency using three configurations of the solid foils attached behind the near-critical-density plasma: a flat foil without a channel (target 1), a flat foil with a channel (target 2), and a convex foil with a channel (target 3). When an intense laser propagates in a near-critical-density plasma, a large number of electrons are trapped and accelerated to GeV energy, and emit γ-rays via nonlinear betatron oscillation in the first stage. In the second stage, the accelerated electrons collide with the laser pulse reflected from the foil and emit high-energy, high-density γ-rays via nonlinear Compton scattering. The simulation results show that compared with the other two targets, target 3 affords better focusing of the laser field and electrons, which decreases the divergence angle of γ-photons. Consequently, denser and brighter γ-rays are emitted when target 3 is used. Specifically, a dense γ-ray pulse with a peak brightness of 4.6×10²⁶ photons/s/mm²/mrad²/0.1%BW (at 100 MeV) and 1.8×10²³ photons/s/mm²/mrad²/0.1%BW (at 2 GeV) are obtained at a laser intensity of 8.5×10²² W/cm² when the plasma density is equal to the critical plasma density n_c. In addition, for target 3, the effects of plasma channel length, foil curvature radius, laser polarization, and laser intensity on the γ-ray emission are discussed, and optimal values based on a series of simulations are proposed.     

讨论埃特金加速法的收敛性

埃特金加速法是一种对不动点迭代进行加速的方法,在一些参考资料中仅提出：埃特金加速法只对收敛阶为P=1的迭代函数有加速作用,而对于P＞1的情况不一定起作用.本文便要对此问题做出相应的理论分析,而且给予证明.