论文标题
负离子源蜘蛛中剖腹和H-/D-密度的表征
Characterization of cesium and H-/D- density in the negative ion source SPIDER
论文作者
论文摘要
ITER的加热中性束喷射器(HNB)将必须在1 MeV能量下输送16.7 MW的H/D颗粒。光束将是由H-/d-ions产生的,该横梁由与离子加速度系统耦合的射频等离子体源产生。在Consorzio RFX的ITER中性束测试设施的一部分蜘蛛实验中,正在测试ITER HNB离子源的原型。只有通过在源中蒸发剖宫产,尤其是在加速度系统的等离子体面板(PG)中,才有可能达到梁电流密度和共摘除电子的比例的设计目标。以这种方式,表面的工作函数降低,显着增加了将中性离子和正离子转化为H-/d-的表面反应量。那么,在PG接近度中监测负离子的密度和CS的密度至关重要。监测沿PG的CS空间分布对于确保梁电流的均匀性也至关重要。在蜘蛛中,由于腔度响应光谱(CRD)和激光吸收光谱诊断(LAS),这是可能的,这些诊断(LAS)分别提供了线集成的测量,分别对负离子密度和中性,基态CS密度。该论文讨论了CRD和LAS测量结果,这是输入功率的函数以及用于减少电子共萃取的磁场和电场的函数。负离子密度数据与无CS条件下的类似测量符合定性一致。与模拟一致,CS密度在来源的中心达到顶峰。也存在顶部/底部的非均匀性。提出了血浆对CS沉积和负离子产生的几种影响。
The Heating Neutral Beam Injectors (HNBs) for ITER will have to deliver 16.7 MW beams of H/D particles at 1 MeV energy. The beams will be produced from H-/D- ions, generated by a radiofrequency plasma source coupled to an ion acceleration system. A prototype of the ITER HNB ion source is being tested in the SPIDER experiment, part of the ITER Neutral Beam Test Facility at Consorzio RFX. Reaching the design targets for beam current density and fraction of coextracted electrons is only possible by evaporating cesium in the source, in particular on the plasma facing grid (PG) of the acceleration system. In this way the work function of the surfaces decreases, significantly increasing the amount of surface reactions that convert neutrals and positive ions into H-/D-. It is then of paramount importance to monitor the density of negative ions and the density of Cs in the proximity of the PG. Monitoring the Cs spatial distribution along the PG is also essential to guarantee the uniformity of the beam current. In SPIDER, this is possible thanks to the Cavity Ringdown Spectroscopy (CRDS) and the Laser absorption Spectroscopy diagnostics (LAS), which provide line-integrated measurements of negative ion density and neutral, ground state Cs density, respectively. The paper discusses the CRDS and LAS measurements as a function of input power and of the magnetic and electric fields used to reduce the coextraction of electrons. Negative ion density data are in qualitative agreement with the analogous measurements in Cs-free conditions. In agreement with simulations, Cs density is peaked in the center of the source; a top/bottom non uniformity is also present. Several effects of plasma on Cs deposition and negative ion production are presented.