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磁约束聚变等离子体中快阿尔文波的受激辐射

Stimulated Emission of Fast Alfvén Waves within Magnetically Confined Fusion Plasmas.

作者信息

Cook J W S, Dendy R O, Chapman S C

机构信息

Centre for Fusion, Space and Astrophysics, Department of Physics, Warwick University, Coventry CV4 7AL, United Kingdom.

First Light Fusion Ltd., Unit 10, Oxford Industrial Park, Yarnton OX5 1QU, United Kingdom.

出版信息

Phys Rev Lett. 2017 May 5;118(18):185001. doi: 10.1103/PhysRevLett.118.185001. Epub 2017 May 4.

Abstract

A fast Alfvén wave with a finite amplitude is shown to grow by a stimulated emission process that we propose for exploitation in toroidal magnetically confined fusion plasmas. Stimulated emission occurs while the wave propagates inward through the outer midplane plasma, where a population inversion of the energy distribution of fusion-born ions is observed to arise naturally. Fully nonlinear first-principles simulations, which self-consistently evolve particles and fields under the Maxwell-Lorentz system, demonstrate this novel "α-particle channeling" scenario for the first time.

摘要

结果表明,具有有限振幅的快阿尔文波通过一种受激辐射过程增长,我们提出该过程可用于环形磁约束聚变等离子体。当波向内传播通过外中平面等离子体时会发生受激辐射,在那里观察到聚变产生的离子的能量分布自然出现粒子数反转。在麦克斯韦 - 洛伦兹系统下自洽地演化粒子和场的全非线性第一性原理模拟首次证明了这种新颖的“α粒子通道化”情景。

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