HT-6M托卡马克装置杂质输运

利用多道可见光谱探测系统和近紫外转镜系统测量了HT-6M托卡马克等离子体中杂质的时空分布.建立完备的杂质输运程序，数值模拟碳、氧杂质在欧姆放电时的输运行为，得出了杂质的扩散和对流系数、不同电离态杂质离子密度、辐射功率密度和有效电荷数的空间分布. 分析低混杂波电流驱动（LHCD）期间杂质行为，结果表明等离子体粒子约束、杂质约束和能 量约束提高，辐射功率和有效电荷数减小. 关键词： 托卡马克 杂质输运 扩散系数 对流系数     

光谱学与光谱技术

利用光学多道分析仪(OMA)拍摄了HT-6M托卡马克等离子体近紫外可见谱。系统分析了杂质行为,给出了主要杂质碳和氧的朝内的通量,在简化模型下计算了碳氧的化学溅射率,并由此得出碳氧杂质产生机制和可能的循环途径。结果表明,氧杂质在循环途径中起关键性的作用,控制氧     

HT-6M托卡马克等离子体紫外-可见谱

利用光学多道分析仪(OMA)拍摄了HT-6M托卡马克等离子体近紫外可见谱.系统分析了杂质行为,给出了主要杂质碳和氧的朝内的通量,在简化模型下计算了碳氧的化学溅射率,并由此得出碳氧杂质产生机制和可能的循环途径.结果表明,氧杂质在循环途径中起关键性的作用,控制氧杂质尤其重要.     

含有杂质的托卡马克等离子体输运的数值研究

应用一维输运模型数值研究杂质及中性粒子对托卡马克放电的影响,对含氧杂质的ST和HT-6B放电进行计算模拟,结果与实验符合很好。     

HT-6M托卡马克边界杂质循环的研究

利用多道可见光谱探测系统测量了Hα、CⅢ(464.7nm)和OⅡ(441.5nnm)谱线的时间行为,得出了碳、氢和氧元素的入射通量。在简化模型下算出了氧碳间的化学溅射率,结果表明HT-6M托卡马克边界杂质产生机制主要是氢氧间的化学溅射和氧碳间的化学溅射,因此控制氧杂质尤其重要。     

基于阿秒XUV-飞秒IR泵浦-探测的冷靶反冲离子动量成像谱仪

利用多道可见光谱探测系统测量了Hα、CⅢ(464.7nm)和OⅡ(441.5nnm)谱线的时间行为,得出了碳、氢和氧元素的入射通量。在简化模型下算出了氧碳间的化学溅射率,结果表明HT-6M托卡马克边界杂质产生机制主要是氢氧间的化学溅射和氧碳间的化学溅射,因此控制氧杂质尤其重要。     

利用低杂波改善约束的实验研究

介绍了在HT-6M托卡马克上,利用双低杂波的组合,成功地实现了准稳态的高约束模式运行. 能量约束时间提高两倍以上,粒子的约束在较高密度下依然改善3倍以上.通过应用波扩散及 电流径向扩散方程计算低杂波电流传播的方法,对一组典型的数据进行数值模拟.计算表明 ,在HT-6M低杂波实验中,由于纵场较低,密度较高,低杂波的能量沉积在离磁轴较远的位 置,使等离子体电流密度分布成为反剪切位形,内部输运垒地形成,大大提高了等离子体的 约束状况.实验数据也给出了反剪切的证据. 关键词： 托卡马克 低杂波 约束改善     

HT-6M托卡马克的同位素交换实验

通过变换工作气体(氢气和氘气的相互转换)研究了HT-6M托卡马克中等离子体的再循环。用光谱方法(Balmer线)跟踪了放电中等离子体浓度的相对变化。结果表明,等离子体在壁处的反射系数约为0.59,变换工作气体后,在第一次放电的等离子体中,由壁释放的同位素含量约占65％。讨论了HT-6M托卡马克中再循环的物理机制。 关键词：     

HL—1装置电流上升段辐射与杂质特性

托卡马克等离子体中的杂质会影响托卡马克的放电品质及等离子体特性。许多理论和实验对杂质的产生和输运做了深入详细的研究。等离子体电流起始阶段,由于约束性能不好,会引起大量的杂质产生,辐射损失增大是杂质增加引起的直接后果。杂质辐射是等离子体辐射的主要组成部分之一,等离子体线辐射功率～Z_(eff)~6,复合辐射功率～Z_(eff)~4,轫致辐     

HT-6托卡马克装置上的质谱诊断

用质谱方法研究受控实验中的杂质,已证明是一种有效的诊断手段。在ST[1],TFR[2]等托卡马克装置上都进行过大量的质谱测量,探测装置的真空特性、杂质输运以及放电过程的化学反应.在我所建造的HT-6托卡马克装置上,也进行了质谱研究.我们分析了轻杂质的种类和清洁手段的效果,提出了识别真空油脂和机械泵油污染的方法,并且测量了分子泵的返油. 一、实验条件和仪器 装置的真空系统见图1.真空室及管道均由不锈钢制成,总容积约为350升,内表面积约4×10～4厘米～2.经去油、酸洗和电抛光处理,内表面呈镜面.极限真空为1.7×10～(-7)托.工作泵为抽口…     

EAST托卡马克杂质输运蒙特卡洛模拟

介绍DIVIMP程序的基本思想和采用的物理模型,研究EAST托卡马克欧姆放电条件下碳杂质的产生与输运.模拟结果与实验测量具有较好的一致性,说明将该程序应用于EAST装置中杂质输运模拟的合理性.并利用DIVIMP程序预测EAST在8MW加热功率条件下钨杂质的输运特性.     

托卡马克等离子体的热平衡特性与脱栏现象

本文利用欧姆加热条件下简化的能量平衡方程研究了热传导与杂质辐射的综合效应。首先指出边缘辐射带的建立与随半径增大而增大的K=nx模型紧密相关(x为电子热传导系数,n为等离子体密度),然后利用删削层中能量平衡关系确定边界温度,自洽地求解了能量平衡方程,得出的脱栏等离子体形成条件能较好地解释有关实验观察到的多种现象。     

托卡马克边缘湍流的数值研究

本文从电阻率梯度驱动的托卡马克边缘湍流理论模型出发,通过数值计算方法,观察了这一湍流随时间演变的过程。研究了湍流发展的物理本质,进一步探明了欧姆耗散效应在湍流发展过程中的作用。发现了它对湍流饱和时间的延缓现象,尤其是在高密度托卡马克装置上,欧姆效应明显地降低了各涨落量的饱和水平。     

Study of the effect of manganese impurities on dielectric characteristics of BSTO films

Capacitance voltage and current voltage characteristics of BSTO ferroelectric films containing a manganese dioxide impurity (～1.5–2 mol%) are compared to those of impurity-free samples. It is shown that in Mn-doped samples tan δ drops to 10^?3, and the dependence of tan δ on the applied voltage changes as well. IVCs of these samples are strictly ohmic and do not show a nonlinearity at high voltages. A mechanism is proposed of the effect of Mn on the charge state of the defects comprising oxygen vacancies in BSTO films.     

Study of solid electrolyte polarization by a complex admittance method

The polarization behavior of zirconia-yttria solid electrolyte specimens with platinum electrodes has been studied over a temperature range of 400° to 800°C and a wide range of oxygen partial pressures. The complex admittance of these specimens was determined over a frequency range from d.c. to 100kHz. An analysis of these data in the complex admittance plane indicated the presence of three polarizations: (1) an electrode polarization characterized by a double layer capacity and an effective resistance for the overall electrode reaction, O₂(gas) + 2e(platinum) O²⁻ (electrolyte); (2) a capacitive-resistive electrolyte polarization, probably corresponding to a partial blocking of oxygen ions at the electrolyte grain boundaries by an impurity phase there; and (3) a pure ohmic electrolyte polarization.     

The carbon impurity ohmic discharges on particle transport in the HT-7 tokamak

The line-integrated optical measurement of impurity radiation profiles for the study of light impurity transport is performed in the HT-7 tokamak. The carbon impurity line emissivity is obtained by Abel inversion. The radial transport behaviours of carbon impurities at different central line averaged electron densities ne are investigated in ohmic discharges. The diffusion coefficient Dk（r）, the convection velocity Wk（r） and the total flux of the impurity ions Fk decrease with the increase of ne, which shows a reduction in the impurity particle transport at higher electron densities.     

氧空位浓度对ZnO电子结构和吸收光谱影响的研究

目前,氧空位对ZnO形成杂质能级的研究结果存在相反的结论,深杂质能级和浅杂质能级两种实验结果均有文献报道,并且,在实验中高温加热的条件下,氧空位体系ZnO中导带自由电子增加的来源认识不足.为了解决此问题,本文采用密度泛函理论框架下的第一性原理平面波超软赝势方法,建立了纯的与两种不同氧空位浓度ZnO超胞模型,分别对模型进行了几何结构优化、态密度分布、能带分布、布居值和差分电荷密度的计算.结果表明,氧空位浓度越大,系统能量越上升、稳定性越下降、形成能越高、氧空位越难、导带越向低能方向移动、电子跃迁宽度越减小、吸收光谱越红移.这对设计制备新型氧空位ZnO体系光学器件有一定的理论指导作用.     

Hidden Caldeira-Leggett dissipation in a Bose-Fermi Kondo model

We show that the Bose-Fermi Kondo model (BFKM), which may find applicability both to certain dissipative mesoscopic qubit devices and to heavy-fermion systems described by the Kondo lattice model, can be mapped exactly onto the Caldeira-Leggett model. This mapping requires an ohmic bosonic bath and an Ising-type coupling between the latter and the impurity spin. This allows us to conclude unambiguously that there is an emergent Kosterlitz-Thouless quantum phase transition in the BFKM with an ohmic bosonic bath. By applying a bosonic numerical renormalization group approach, we thoroughly probe physical quantities close to the quantum phase transition.     

长直管束通电加热吸合现象的研究

利用一组 3×3 的长直不锈钢管束通电加热液态水.实验结果表明:当通电电压升高到一定值时,管间产生吸合效应,导致管束发生短接.本文主要从热应力效应和磁场力效应这两方面因素及其相互关系分析了长直通电加热管束产生吸合现象的原因,该研究有利于发热式管壁直接加热器的研制.     

Effect of driving frequency on electron heating in capacitively coupled RF argon glow discharges at low pressure

A one-dimensional(1D) fluid model on capacitively coupled radio frequency(RF) argon glow discharge between parallel-plates electrodes at low pressure is established to test the effect of the driving frequency on electron heating. The model is solved numerically by a finite difference method. The numerical results show that the discharge process may be divided into three stages: the growing rapidly stage, the growing slowly stage, and the steady stage. In the steady stage,the maximal electron density increases as the driving frequency increases. The results show that the discharge region has three parts: the powered electrode sheath region, the bulk plasma region and the grounded electrode sheath region. In the growing rapidly stage(at 18 μs), the results of the cycle-averaged electric field, electron temperature, electron density, and electric potentials for the driving frequencies of 3.39, 6.78, 13.56, and 27.12 MHz are compared, respectively. Furthermore,the results of cycle-averaged electron pressure cooling, electron ohmic heating, electron heating, and electron energy loss for the driving frequencies of 3.39, 6.78, 13.56, and 27.12 MHz are discussed, respectively. It is also found that the effect of the cycle-averaged electron pressure cooling on the electrons is to "cool" the electrons; the effect of the electron ohmic heating on the electrons is always to "heat" the electrons; the effect of the cycle-averaged electron ohmic heating on the electrons is stronger than the effect of the cycle-averaged electron pressure cooling on the electrons in the discharge region except in the regions near the electrodes. Therefore, the effect of the cycle-averaged electron heating on the electrons is to "heat" the electrons in the discharge region except in the regions near the electrodes. However, in the regions near the electrodes, the effect of the cycle-averaged electron heating on the electron is to "cool" the electrons. Finally, the space distributions of the electron pressure cooling the electron ohmic heating and the electron heating at 1/4 T, 2/4 T, 3/4 T, and 4/4 T in one RF-cycle are presented and compared.