1969•Physical Review LettersRequires access

New Ion-Electron Resonances in Bounded, Hot, Magnetized Plasmas

P. E. Vandenplas, André Messiaen, J.-L. Monfort, J. J. Papier

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Abstract

The present investigation of a hot (${T}_{e} \mathrm{and} {T}_{i}\ensuremath{\ne}0$) magnetized plasma cylinder shows that ${\stackrel{\ensuremath{\rightarrow}}{\mathrm{B}}}_{0}$ can introduce novel features in the ion thermal resonances. Furthermore, two new and strong main resonances are obtained which occur in the ion domain and are essentially due to a proper combination of ${T}_{e}$ and ${B}_{0}$. These resonances of a bounded plasma are only indirectly connected to the lower and upper hybrid resonances of an infinite plasma.

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What this paper is about

The present investigation of a hot (${T}_{e} \mathrm{and} {T}_{i}\ensuremath{\ne}0$) magnetized plasma cylinder shows that ${\stackrel{\ensuremath{\rightarrow}}{\mathrm{B}}}_{0}$ can introduce novel features in the ion thermal resonances. Furthermore, two new and strong main resonances are obtained which occur in the ion domain and are essentially due to a proper combination of ${T}_{e}$ and ${B}_{0}$. These resonances of a bounded plasma are only indirectly connected to the lower and upper hybrid resonances of an infinite plasma.

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Available abstract

The present investigation of a hot (${T}_{e} \mathrm{and} {T}_{i}\ensuremath{\ne}0$) magnetized plasma cylinder shows that ${\stackrel{\ensuremath{\rightarrow}}{\mathrm{B}}}_{0}$ can introduce novel features in the ion thermal resonances. Furthermore, two new and strong main resonances are obtained which occur in the ion domain and are essentially due to a proper combination of ${T}_{e}$ and ${B}_{0}$. These resonances of a bounded plasma are only indirectly connected to the lower and upper hybrid resonances of an infinite plasma.

Key concepts: Plasma, Physics, Ion, Atomic physics, Bounded function, Electron, Domain (mathematical analysis), Resonance (particle physics)

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