针对双等离子体离子源受气压、磁场强度和放电电流影响,产生的O-离子束亮度不稳定的问题,设计并搭建了一套用于测试离子束亮度的离子光学系统,以SHRIMP II上的双等离子体离子源为对象,通过实验和仿真模拟分别研究了气压、磁场强度和放...针对双等离子体离子源受气压、磁场强度和放电电流影响,产生的O-离子束亮度不稳定的问题,设计并搭建了一套用于测试离子束亮度的离子光学系统,以SHRIMP II上的双等离子体离子源为对象,通过实验和仿真模拟分别研究了气压、磁场强度和放电电流对O-离子束亮度的影响规律。结果表明：该离子源能够稳定地工作在放电电流大于50 m A,气压为110~170 m Torr（1Torr=133.322 Pa）的条件下;当气压为140 m Torr、放电电流为200 m A、磁场强度为0.25 T时,获得的O-离子束亮度能够达到52.4 A/（cm2·sr）。合理控制离子源工作参数,可以增大O-离子束亮度,提高二次离子质谱的横向分辨率和灵敏度。展开更多
An efficient method for attosecond extreme ultraviolet source generation under the two-color multi-cycle weak pulse has been theoretically presented by using the concept of the plasmonic field enhancement in the vicin...An efficient method for attosecond extreme ultraviolet source generation under the two-color multi-cycle weak pulse has been theoretically presented by using the concept of the plasmonic field enhancement in the vicinity of metallic nanostructures. The results show that by properly choosing the inhomogeneity of the two-color multi-cycle(20 fs) weak pulse(1013W/cm2), not only the harmonic cutoff has been extended, resulting in a broadband XUV continuum, but also the single short quantum path has been selected to contribute to the harmonic. As a result, two isolated XUV pulses with durations of 68 as and 66 as can be obtained.展开更多
文摘针对双等离子体离子源受气压、磁场强度和放电电流影响,产生的O-离子束亮度不稳定的问题,设计并搭建了一套用于测试离子束亮度的离子光学系统,以SHRIMP II上的双等离子体离子源为对象,通过实验和仿真模拟分别研究了气压、磁场强度和放电电流对O-离子束亮度的影响规律。结果表明：该离子源能够稳定地工作在放电电流大于50 m A,气压为110~170 m Torr（1Torr=133.322 Pa）的条件下;当气压为140 m Torr、放电电流为200 m A、磁场强度为0.25 T时,获得的O-离子束亮度能够达到52.4 A/（cm2·sr）。合理控制离子源工作参数,可以增大O-离子束亮度,提高二次离子质谱的横向分辨率和灵敏度。
基金Supported by the Scientific Research Fund of Liaoning University of Technology of China under Grant No.X201319the Scientific Research Fund of Liaoning Provincial Education Department under Grant No.L2014242
文摘An efficient method for attosecond extreme ultraviolet source generation under the two-color multi-cycle weak pulse has been theoretically presented by using the concept of the plasmonic field enhancement in the vicinity of metallic nanostructures. The results show that by properly choosing the inhomogeneity of the two-color multi-cycle(20 fs) weak pulse(1013W/cm2), not only the harmonic cutoff has been extended, resulting in a broadband XUV continuum, but also the single short quantum path has been selected to contribute to the harmonic. As a result, two isolated XUV pulses with durations of 68 as and 66 as can be obtained.
