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PIC-simulation resolved period-doubling route to chaos in the classical pierce diode

机译:PIC模拟解决了经典穿孔二极管中周期到混沌的倍增路径

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The classical Pierce diode [J. R. Pierce, J. Appl. Phys. 15, 721 (1944)] is a one-dimensional, electrostatic plasma-filled system bounded by an emitter and a collector separated by a distance d and externally connected by a short circuit. A mono-energetic electron beam is emitted from the emitter with a constant current density j(0) = -en(0)u(0), where n(0) and u(0) are the initial electron density (corresponding to the plasma frequency omega(pe) = root n(0)e(2)/(epsilon(0)m(e)) and velocity, respectively. The immobile ions form a uniform neutralising background. In this work we use Particle-in-Cell (PIC) simulations performed with the BIT1 code [D. Tskhakaya jr. and S. Kuhn, Contrib. Plasma Phys. 42, 302 (2002)] to investigate the evolution of slightly perturbed uniform equilibria into the related non-linear attractor states for a broad range of a values, where alpha = w(pe)d/u(0) is the diode control parameter. First, to demonstrate the suitability of our code, the period-doubling route to chaos for alpha below 3 pi was re-investigated in detail. In both the linear and non-linear regimes, excellent agreement was found with the results obtained previously by Godfrey [Phys. Fluids 30, 1553 (1987)] from numerical integration of a genuine fluid model, and by Horhager and Kuhn [Phys. Fluids B 2, 2741 (1990)] from a three-harmonic fluid analysis. Having thus established that our method is perfectly adequate for these investigations, we present analogous results for linear and non-linear oscillations in alpha domains in which these phenomena have not been considered in detail before. The present kinetic approach to small-amplitude oscillations in a bounded system can be extended to more complex bounded plasma systems, e.g., for PIC simulations of turbulent fusion plasmas, in which small-amplitude oscillations are known to give rise to anomalous transport. (c) 2006 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.
机译:经典的皮尔斯二极管[J. R.Pierce,J.Appl。物理15,721(1944)]是一维静电等离子体填充的系统,该系统由发射器和集电极隔开一定距离d,并通过短路从外部连接。从发射器以恒定电流密度j(0)= -en(0)u(0)发射单能电子束,其中n(0)和u(0)是初始电子密度(对应于等离子体频率ω(pe)=根n(0)e(2)/(epsilon(0)m(e))和速度,固定的离子形成均匀的中和背景。用BIT1代码执行的单元(PIC)模拟[D. Tskhakaya jr。和S. Kuhn,Contrib。Plasma Phys。42,302(2002)],以研究微扰动的均匀平衡向相关非线性吸引子态的演化对于大范围的值,其中α= w(pe)d / u(0)是二极管控制参数。首先,为了证明我们的代码的适用性,对于低于3 pi的α,混沌的倍频途径是在线性和非线性范围内,Godfrey [Phys。Fluids 30,1553(1987)]先前从数值积分中获得的结果都发现了极好的一致性。真正的流体模型,由Horhager和Kuhn [Phys。流体B 2,2741(1990)]。因此,在确定我们的方法完全适合这些研究之后,我们给出了α域中线性和非线性振荡的类似结果,在这些情况下,以前没有详细考虑过这些现象。可以将有界系统中用于小振幅振荡的当前动力学方法扩展到更复杂的有界等离子体系统,例如,用于湍流聚变等离子体的PIC模拟,其中已知小振幅振荡会引起异常传输。 (c)2006威尼海姆威利威世私人有限公司。

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