1961
DOI: 10.1049/pi-c.1961.0018
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Unstable electron flow in a diode

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Cited by 9 publications
(11 citation statements)
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“…In accordance with earlier studies, we find that the C-overlap branch is unstable to linear perturbations, and we follow these into non-linear regime [3,17,18].…”
Section: Equilibrium Solutionssupporting
confidence: 92%
“…In accordance with earlier studies, we find that the C-overlap branch is unstable to linear perturbations, and we follow these into non-linear regime [3,17,18].…”
Section: Equilibrium Solutionssupporting
confidence: 92%
“…In this work, we extend previous analysis [1][2][3][4] of the linear stability of the space charge limited flow to the case when the current is determined by a current-field relation at the emitter. We consider a planar diode with flat parallel electrodes, which allows a one dimensional treatment.…”
Section: Introductionmentioning
confidence: 73%
“…This allows to find uniquely the electric field E(τ, t) as well as ϕ(τ, t) and current density j(τ, t) at the point x, t. (This somewhat sloppy use of the same notation in the new units will not lead to confusion). A straightforward analysis in these variables [3] shows that if T is the time needed for an electron, emitted at τ , to cross the diode then this electron is located at…”
Section: Main Equations and Setup Of 1d Flow Modelmentioning
confidence: 99%
“…While the main features of the steady flow in a diode have been known for a century [1], [2] an important step in studying time dependent states was made by Lomax [3] in 1960, who applied the Lagrange formulation of flow dynamics. This approach has been developed in many works, in particular in [4]- [8], where the authors found conditions for flow stability and modes of oscillations.…”
Section: Introductionmentioning
confidence: 99%
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