椭圆回路下暗条电流的特性

给出了椭圆暗条电流回路下暗条垂直平衡方程,并用它计算了NOAA131活动区暗条的平衡电流,分析了其暗条电流的特性.      

暗条电流演化和耀斑储能

利用紫金山天文台观测的编号为McMath8207和McMath16171两个活动区光学资料,采用KR和KS两种理论模型,计算了活动区暗条电流演化过程.结果表明:不同的暗条扰动可以导致不同类型的耀斑;出现在强活动区新浮磁流附近的拱状暗条可用KR模型描述,它们往往处于较低层次,具有较强的初始电流,在新浮磁流的挤压和剪切作用下可形成中性电流片,导致高能耀斑发生.而符合KS模型的宁静暗条,在新浮磁流或耀斑波作用下亦可被激活,但其初始电流较弱,往往只能为热耀斑提供能量.      

AR2522活动区中暗条的演化与耀斑的爆发

利用AR2522活动区多波段的观测资料,分析了暗条演化与1B/M4级双带耀斑爆发之间的关系。结果表明:(1)足点的剪切运动导致暗条电流增强和耀斑贮能;(2)暗条上升运动和绞扭现象是暗条电流增强和耀斑贮能的结果;(3)Marttens-Kuin模型至少适合于解释与暗条快速上升有关的双带耀斑爆发。      

活动区新浮磁流和暗条的激活

用数值计算方法探讨了新浮磁流驱动下暗条运动的基本规律。计算表明,活动区新浮磁流是驱动暗条运动导致暗条激活的有效机制之一,这个过程是通过暗条电流和背景磁场的相互作用来实现的。当选取不同强度的浮现磁流时,暗条可出现周期性振荡、激活上升和闪烁;此外,对同极性磁流浮现,当浮现强度足够强时,暗条一开始就会下沉。      

1986年2月4日AR4711拱形双带黑子暗条系激活的分析

根据1986-02-04AR47ll由观测所确定的物理参数和特征值,采用电动力学方法数值计算该活动区中两个拱形黑子暗条在大耀斑爆发前的动力学演化过程.结果表明:(1)以旋涡黑子为标志的光球物质旋转运动和以暗条下方磁力线强剪切为特征的剪切运动引起暗条电流增加和背景磁场变化,电流和磁场的相互作用导致暗条向上运动,大耀斑爆发前暗条的上升速度达26km／S;(2)背景场位形对暗条整体动力学行为有很大影响,AR47ll在7×104km高度范围内场强随高度似乎按指数规律衰减.      

火星空间大尺度电流体系分布特征

在MHD模型基础上, 对火星空间环境的电流分布进行了模拟. 结果表明, 火星空间存在着弓激波电流、磁堆积区电流、电离层电流和磁尾电流. 弓激波电流在激波曲面上均由北向南自成体系, 电流密度在弓激波顶区域较大. 在向阳面磁堆积区边界电流与电离层电流彼此耦合形成完整的回路, 在背阳面磁堆积区边界电流与磁尾中心电流片耦合形成完整的回路.      

会切磁场推力器低频振荡特性

针对会切磁场推力器的低频振荡特性,将推力器的工作模式分为高电流模式和低电流模式,在此基础上研究了低频振荡随工作参数和磁场位形的变化特性,并针对推力系统外回路对低频振荡的影响进行了研究。结果表明,在高质量流量下,随着放电电压的增加,会切磁场推力器的工作模式从高电流模式转换为低电流模式。在高电流模式下,放电电流具有高振幅、低频率的特征,羽流比较模糊,并且电流振荡幅值随着放电电压增大呈先增大后降低的趋势,而对应的振荡频率随着放电电压的增大而增大。在低电流模式下,放电电流具有低振幅、高频率的特征,羽流有两条明显的亮线,并且电流振荡幅值和频率均随放电电压的增大而增大。在不同工况下,随着质量流量增大,放电电流振荡幅值和频率均呈现增大的趋势。研究还发现,外回路中的电阻和电感对低频振荡起到一定的抑制作用,而电容对低频振荡的影响并不明显。     

电离辐射对部分耗尽SOI器件关态电流的影响

针对辐射前后环栅与条栅结构部分耗尽绝缘体上硅(SOI,Silicon On Insulator)器件关态电流的变化展开实验,研究结果表明辐射诱使关态电流增加主要取决于侧壁泄漏电流、背栅寄生晶体管导通、带-带隧穿与背栅泄漏电流的耦合效应.在条栅结构器件中,辐射诱生场氧化层固定电荷将使得器件侧壁泄漏电流增加,器件前、背栅关态电流随总剂量变化明显;在环栅结构器件中,辐射诱使背栅晶体管开启将使得前栅器件关态电流变大,而带-带隧穿与背栅泄漏电流的耦合效应将使得器件关态电流随前栅电压减小而迅速增加.基于以上结果,可通过改良版图结构以提高SOI器件的抗总剂量电离辐射能力.     

电离辐射对部分耗尽SOI器件关态电流的影响

针对辐射前后环栅与条栅结构部分耗尽绝缘体上硅(SOI,Silicon On Insulator)器件关态电流的变化展开实验,研究结果表明辐射诱使关态电流增加主要取决于侧壁泄漏电流、背栅寄生晶体管导通、带-带隧穿与背栅泄漏电流的耦合效应.在条栅结构器件中,辐射诱生场氧化层固定电荷将使得器件侧壁泄漏电流增加,器件前、背栅关态电流随总剂量变化明显；在环栅结构器件中,辐射诱使背栅晶体管开启将使得前栅器件关态电流变大,而带-带隧穿与背栅泄漏电流的耦合效应将使得器件关态电流随前栅电压减小而迅速增加.基于以上结果,可通过改良版图结构以提高SOI器件的抗总剂量电离辐射能力.     

Evolution of coronal mass ejections in the early stage

This work reports the investigation of two coronal mass ejections (CME) observed in white light, H, EUV and X-ray by various instruments both in space and on ground on February 18, 2003 and January 19, 2005, respectively. The white light coronal images show that the first CME began with the rarefaction of a region above the solar limb and was followed by the formation of its leading edge at the boundary of the rarefying region at altitude of 0.46 R from the solar surface. The rarefaction coincided the slow rising phase of the filament eruption, and the CME leading edge was observed to form as the filament eruption started to accelerate apparently. In the early stage of the second CME, a bright loop was first observed above the solar limb with height of 0.37 R in EUV images. We found that the more gradual CMEs initial process, the larger the timing difference between CMEs and their associated flares. The lower part of the filament brightened in H images as the filament rose to a certain height. These brightenings imply that the filament may be heated by magnetic reconnection below the filament in the early stage of the eruption. We suggest that the possible mechanism which led to the formation of the CME leading edge and cavity is magnetic reconnection which occurred under the filament when it reached a certain height.     

Model of a fluxtube with a twisted magnetic field in the stratified solar atmosphere

We build a single vertical straight magnetic fluxtube spanning the solar photosphere and the transition region which does not expand with height. We assume that the fluxtube containing twisted magnetic fields is in magnetohydrostatic equilibrium within a realistic stratified atmosphere subject to solar gravity. Incorporating specific forms of current density and gas pressure in the Grad–Shafranov equation, we solve the magnetic flux function, and find it to be separable with a Coulomb wave function in radial direction while the vertical part of the solution decreases exponentially. We employ improved fluxtube boundary conditions and take a realistic ambient external pressure for the photosphere to transition region, to derive a family of solutions for reasonable values of the fluxtube radius and magnetic field strength at the base of the axis that are the free parameters in our model. We find that our model estimates are consistent with the magnetic field strength and the radii of Magnetic bright points (MBPs) as estimated from observations. We also derive thermodynamic quantities inside the fluxtube.     

Solar atmosphere wave dynamics generated by solar global oscillating eigenmodes

The solar atmosphere exhibits a diverse range of wave phenomena, where one of the earliest discovered was the five-minute global acoustic oscillation, also referred to as the p-mode. The analysis of wave propagation in the solar atmosphere may be used as a diagnostic tool to estimate accurately the physical characteristics of the Sun’s atmospheric layers.In this paper, we investigate the dynamics and upward propagation of waves which are generated by the solar global eigenmodes. We report on a series of hydrodynamic simulations of a realistically stratified model of the solar atmosphere representing its lower region from the photosphere to low corona. With the objective of modelling atmospheric perturbations, propagating from the photosphere into the chromosphere, transition region and low corona, generated by the photospheric global oscillations the simulations use photospheric drivers mimicking the solar p-modes. The drivers are spatially structured harmonics across the computational box parallel to the solar surface. The drivers perturb the atmosphere at 0.5?Mm above the bottom boundary of the model and are placed coincident with the location of the temperature minimum. A combination of the VALIIIC and McWhirter solar atmospheres are used as the background equilibrium model.We report how synthetic photospheric oscillations may manifest in a magnetic field free model of the quiet Sun. To carry out the simulations, we employed the magnetohydrodynamics code, SMAUG (Sheffield MHD Accelerated Using GPUs).Our results show that the amount of energy propagating into the solar atmosphere is consistent with a model of solar global oscillations described by Taroyan and Erdélyi (2008) using the Klein-Gordon equation. The computed results indicate a power law which is compared to observations reported by Ireland et al. (2015) using data from the Solar Dynamics Observatory/Atmospheric Imaging Assembly.     

太阳质子耀斑的一个统计性质

本文研究太阳质子耀斑相对于太阳光球大尺度平均磁场中性线的分布, 给出一个新得到的质子耀斑的统计性质。研究太阳质子事件及其源耀斑的统计性质, 是太阳物理和空间物理学的重要前沿课题。从太阳活动预报及地球空间环境预报研究的角度看, 一个重要的问题是质子耀斑在      

子午面内Alfvén波的传播特征

本文使用由ＷＫＢ近似得到的Ａｌｆｖｅｎ波传播的张量表达式,具体计算和讨论了一种太阳子午面内含盔形－电流片磁位形的流场中Ａｌｆｖｅｎ波的传播特征,主要结果是：（１）Ａｌｆｖｅｎ波磁场起伏随日心距离的增加而衰减,其中极开区的衰减远快于赤道区,但随着距离的增大,这种纬度关系将迅速变弱,以致在较远空间,磁起伏相差很小,衰减很慢;（２）Ａｌｆｖｅｎ波的相对磁场起伏ｂ／Ｂ随着距离的增加而迅速增大,在几个太阳半径之后变化不再明显,达到所谓的＂饱和＂;在大日心距离的盔形电流片附近,Ａｌｆｖｅｎ波将成为重要的磁场组成部分;（３）Ａｌｆｖｅｎ波速度起伏纬度关系较为明显,相对速度起伏。ｕ／Ｕ随着距离增大而衰减,电流片区衰减得较快,但这种纬度差别将变弱．与黄道面内Ａｌｆｖｅｎ波传播特征的具体比较表明,磁场涨落的变化特征与背景场位形存在着十分密切的关系,但速度涨落与背景场没有这种明显关系．