Advanced Search+
Suyun ZHOU (周素云), Hui CHEN (陈辉), Yanfang LI (李艳芳). Breaking of a Langmuir wave in cold electron–positron–ion plasmas[J]. Plasma Science and Technology, 2018, 20(1): 14008-014008. DOI: 10.1088/2058-6272/aa8cc0
Citation: Suyun ZHOU (周素云), Hui CHEN (陈辉), Yanfang LI (李艳芳). Breaking of a Langmuir wave in cold electron–positron–ion plasmas[J]. Plasma Science and Technology, 2018, 20(1): 14008-014008. DOI: 10.1088/2058-6272/aa8cc0

Breaking of a Langmuir wave in cold electron–positron–ion plasmas

Funds: This work is supported by National Natural Science Foundation of China (Nos. 11665012 and 11247016) and the Natural Science Foundation of Jiangxi Province, China (Nos. 2014ZBAB202001 and 2015ZBAB202006).
More Information
  • The space–time evolution of a given density perturbation in cold homogeneous electron–positron–ion plasma is investigated with an assumption of infinitely massive ions by employing a numerical calculation method. The phase-mixing time and wave-breaking time can be effectively distinguished with this method. It is found that an increase of the ratio of equilibrium ion density to equilibrium electron density can attenuate plasma oscillations, leading to a delay in wave breaking. The dependence of the phase-mixing and wave-breaking times on the amplitude of the initial perturbation is also discussed.
  • Related Articles

    [1]Monzurul K AHMED, Om P SAH. Solitary kinetic Alfvén waves in dense plasmas with relativistic degenerate electrons and positrons[J]. Plasma Science and Technology, 2019, 21(4): 45301-045301. DOI: 10.1088/2058-6272/aaf20f
    [2]Victor TARASENKO, Dmitry BELOPLOTOV, Mikhail LOMAEV, Dmitry SOROKIN. E-beam generation in discharges initiated by voltage pulses with a rise time of 200 ns at an air pressure of 12.5–100 kPa[J]. Plasma Science and Technology, 2019, 21(4): 44007-044007.
    [3]Wei ZHANG (张伟), Tongyu WU (吴彤宇), Bowen ZHENG (郑博文), Shiping LI (李世平), Yipo ZHANG (张轶泼), Zejie YIN (阴泽杰). A real-time neutron-gamma discriminator based on the support vector machine method for the time-of-fiight neutron spectrometer[J]. Plasma Science and Technology, 2018, 20(4): 45601-045601. DOI: 10.1088/2058-6272/aaaaa9
    [4]Monzurul K AHMED, Om P SAH. Solitary kinetic Alfvén waves in a dense electron–positron–ion plasma with degenerate electrons and positrons[J]. Plasma Science and Technology, 2017, 19(12): 125302. DOI: 10.1088/2058-6272/aa8765
    [5]Xiaoyan BAI (白小燕), Chen CHEN (陈晨), Hong LI (李弘), Wandong LIU (刘万东). Investigations on the time evolution of the plasma density in argon electron-beam plasma at intermediate pressure[J]. Plasma Science and Technology, 2017, 19(3): 35003-035003. DOI: 10.1088/2058-6272/19/3/035003
    [6]FU Qiang (付强), TANG Ying (唐影), ZHAO Jinsong (赵金松), LU Jianyong (吕建永). Low-Frequency Waves in Cold Three-Component Plasmas[J]. Plasma Science and Technology, 2016, 18(9): 897-901. DOI: 10.1088/1009-0630/18/9/04
    [7]M. L. SHAH, A. K. PULHANI, B. M. SURI, G. P. GUPTA. Time-Resolved Emission Spectroscopic Study of Laser-Induced Steel Plasmas[J]. Plasma Science and Technology, 2013, 15(6): 546-551. DOI: 10.1088/1009-0630/15/6/11
    [8]GAO Min (高敏), CHEN Shaoyong (陈少永), TANG Changjian (唐昌建). Electron Cyclotron Harmonic Wave Heating in Tokamak Plasmas with Different Polarization Modes[J]. Plasma Science and Technology, 2013, 15(4): 313-317. DOI: 10.1088/1009-0630/15/4/02
    [9]XIAO Dengming (肖登明), DENG Yunkun (邓云坤). Determination of Electron Swarm Parameters in Pure CHF3 and CF4 by a Time-Resolved Method[J]. Plasma Science and Technology, 2013, 15(1): 25-29. DOI: 10.1088/1009-0630/15/1/05
    [10]ZHU Xueguang(朱学光). Influence of the Phase of the Antenna Current Standing Wave on the Power Flux in Ion Cyclotron Heating[J]. Plasma Science and Technology, 2010, 12(5): 543-546.

Catalog

    Article views (190) PDF downloads (542) Cited by()

    /

    DownLoad:  Full-Size Img  PowerPoint
    Return
    Return