Electron beams: partially flat solutions of a nonlinear elliptic equation with a singular absorption term
Jesús Ildefonso Díaz
TL;DR
The paper analyzes 2D space-charge-limited electron beams between parallel plates with edge effects, formulating a singular semilinear elliptic problem $- abla^{2}u=\frac{j(x)}{\sqrt{u}}$ on a strip and imposing partially flat boundary behavior to reflect vanishing flux on part of the cathode. Using a sophisticated sub-/super-solution strategy and domain decomposition, it constructs a weak, nondegenerate solution under a near-edge singular current density $j(x)\sim\frac{A}{(-x)^{\beta}}$ with $0<\beta<\tfrac{1}{2}$ and $j(x)=0$ on the complementary side; the solution satisfies sharp near-boundary estimates $u(x,y)\gtrsim \delta^{4/3}$ and $u(0,y)\gtrsim y^{\alpha}$ with $\alpha=\tfrac{2}{3}(2-\beta)$. A key part is the analysis of an auxiliary nonlinear eigenvalue problem $-U''+\frac{V_0}{\sqrt{U}}=\lambda U$ on a finite interval, which exhibits a bifurcation from infinity and a non-smooth flat solution at a critical value, guiding the construction of subsolutions and the existence of a partially flat supersolution. The work proves existence of a global weak solution, nondegeneracy, and, via a parabolic comparison framework, uniqueness in the nondegenerate class, thereby rigorously justifying the formation of current wings near cathode edges and extending the one-dimensional Child-Langmuir theory to 2D with edge effects. These results provide a rigorous foundation for edge phenomena in space-charge-limited devices and offer a framework for further analysis of 2D electrostatic-flow problems with singular absorptions.
Abstract
In the so-called Child-Langmuir law, established since 1911, an electron beam is formed linking two electrodes, which are assumed to be two parallel plates of area $A$, separated to a finite distance $D.$ When $% D\ll \sqrt{A},$ \textquotedblleft edge effects\textquotedblright\ are negligible and the modelling is reduced to a nonlinear boundary problem for a singular ordinary differential equation\ in which a constant coefficient (the generated electric current $j$) must be found in order to get simultaneously Dirichlet and Neumann homogeneous boundary conditions in one of the extremes. If $D>\sqrt{A},$ then the problem becomes much more difficult since the \textquotedblleft edge effects\textquotedblright\ arise in the plane $(x,y)$ and the electric current (now $j(x)$ due to the presence of a very large perpendicular magnetic field) must be determined in order to get solutions $u(x,y)$ of a singular semilinear equation which are partially flat ($u=\frac{\partial u}{\partial n}=0$ on a part of the boundary). In this paper, we offer a rigorous mathematical treatment of some former studies (Joel Lebowitz and Alexander Rokhenko (2003) and Alexander Rokhenko (2006)), where several open questions were left open: for instance, the need for a singularity of $j(x)$ near the cathode edge to get such partially flat solutions.
