对称强双色共振场中弛豫效应对二能级系统斯塔克分裂的影响

本文应用半径典理论、密度矩阵方法和探索场中二能级系统的能级斯塔克(Stark)分裂。指出与无弛豫效应相比较,弛予效应不仅改变了由光学斯塔克效应所产生的分裂能级的权重、展宽了这些能级,而且还出现新的分裂能级。     

原子发射高次谐波偏振态的调控

利用分裂算符法数值求解二维含时薛定谔方程研究了He原子在反旋双色组合激光场(由椭圆极化的基频场与圆极化的三倍频场构成)中产生高次谐波的偏振特性。研究结果表明,改变基频场的椭偏率、强度及相位可实现对高次谐波偏振态从圆偏振到椭圆偏振以及线偏振的完全调控,为实验室产生偏振态可控的紫外-软X射线光源提供了参考。     

Generation of the wavelength-tunable XUV pulse using the two-color and three-color infrared pulses

We present an efficient method to generate an ultrashort wavelength-tunable XUV pulse by using the harmonic selec- tive enhancement scheme. The results show that by properly controlling the delay times of a two-color field or a three-color field, selective enhancement of the harmonics with photon energies between 80 eV and 315 eV can be obtained. Fur- ther, a wavelength-tunable and bandwidth-controllable XUV radiation can be obtained by Fourier transformation of these enhanced harmonics.     

润滑油膜双色光干涉测量系统的特性研究

基于多光束干涉理论和摄像系统的光谱响应特性,建立了润滑油膜彩色光干涉测量的色度学模型,以红绿双色光干涉测量为例设计了计算机程序复现了油膜厚度测量的干涉图像。双色光干涉的理论计算和实验测量取得了很好的一致性。进一步的计算表明,润滑油膜双色光干涉图像的色彩主要受光源双色光的半峰全宽、析光膜厚度、垫层厚度及润滑介质特性的影响。在所设定的计算参数条件下,双色光的半峰全宽较窄,析光膜厚度为4～10nm和垫层厚度较薄时图像的对比度较高。     

EGR对高压共轨柴油机燃烧过程影响的可视化研究

以某高压共轨柴油机为样机,结合AVL 513D可视化研究系统,搭建柴油机缸内工作过程可视化研究平台,进行EGR对高压共轨柴油机燃烧过程影响的可视化研究。研究表明:通过所搭建的柴油机缸内工作过程可视化平台可以直观地分析柴油机缸内燃烧过程,为合理组织缸内燃烧过程提供依据。小负荷条件下,EGR率的增加(≤30%)可以有效地缩短着火延迟期,缸内氧浓度不断降低,燃烧火焰平均温度下降,高温强辐射区域的比例也减小,导致柴油机缸内燃烧持续期延长,缸内火焰熄灭的时刻推后。     

双视场/双色红外消热差光学系统设计

双色红外光学系统能够同时获取长波红外与中波红外的波段信息,有利于目标的搜索和识别.本文针对红外热像仪的需求,对双视场/双色红外光学系统进行了设计.实现了4.4～5.4μm/7.8～8.8μm双波段同时清晰成像,在F#为2.68情况下,通过切换变倍组完成9°×6.75°/3°×2.25°双视场转换.通过红外材料与光焦度的合理分配实现了折射式被动消热差设计.设计结果表明,系统在-40℃～+60℃工作温度下,像面稳定、像质优良,能够满足红外热像仪的使用需求.     

Electron Correlation in Nonsequential Double Ionization of Helium by Two-Color Pulses

We investigate the momentum and energy correlations between the two electrons from nonsequential double ionization （NSDI） of helium by strong two-color pulses with the classical three-dimensional ensemble model. The correlated momentum distribution in the direction parallel to the laser field exhibits an arc-like structure and the sum-energy spectrum shows a sharp peak for the NSDI of helium in the two-color fields. Back analysis reveals that the narrow time interval during which recollisions occur, the low returning energy and the short time delay between recollision and double ionization lead to the novel momentum and energy correlations.     

量子路径控制生成宽频软X射线连续辐射谱

数值研究了双色激光脉冲与一维氩原子相互作用的谐波发射功率谱.双色激光脉冲由800 nm和1600 nm的两束激光组成,脉冲持续时间为9.7 fs.计算结果表明,相对相位为π时,谐波截止频率从单色场情形的58 eV大幅度地展宽到316 eV,获得频宽为93 eV的软X射线连续辐射谱.此外,还采用短程的普薛耳－特勒势和长程的软化库仑势进行比对,数值结果表明该连续辐射谱的存在具有普适性.通过半经典的“三步”模型和时频分析小波变换方法对该连续辐射谱进行分析,发现其主要由单一的“短”量子路径生成,直接叠加频率从22 关键词： 红外双色激光脉冲 连续辐射谱 阿秒脉冲     

Creation of Molecular Vortex

The molecular vortex is predicted to be generated from an atomic Bose-Einstein condensate through the two-color photoassociation process with a specially designed field configuration in which a Gaussian and a first-order Laguerre Gaussian laser beam are applied between the bound-bound and free-bound transition, respectively. We show that such a configuration can lead to a coherent superposition of an atomic condensate and a molecular quantized vortex. We develop stimulated adiabatic passages to minimize the effect of mean-field shifts due to collisions for optimal conversi9n of an atomic condensate into a ground molecular vortex.     

Intensity correlation time of a single-mode laser driven by two coloured noises with coloured cross-correlation with direct signal modulation

In this paper, the intensity correlation time T is studied for the gain-noise model of a single-mode laser driven by coloured pump noise and coloured quantum noise with coloured cross-correlation with a direct signal modulation. By using the linear approximation method, it is found that when the pump noise is modulated directly by a signal, the effects of the cross-correlation between the pump noise and the quantum noise will disappear. In addition, there exists a maximum (i.e. resonance) in the curve of the intensity correlation time $T$ versus the pump noise self-correlation time \tau¹. Furthermore, when \tau¹\le\tau², the intensity correlation time T increases monotonically with the increase of $D$ and decreases monotonically with the increase of Q, but when \tau¹>\tau², the intensity correlation time T increases monotonically with the increase of Q and decreases monotonically with the increase of D.