Abstract

This work presents a theoretical explanation for a crossover in the linear behavior in Fowler–Nordheim (FN) plots based on orthodox cold field electron emission (CFE) experimental data. It is characterized by a clear change in the decay rate of usually single-slope FN plots, and has been reported when non-uniform nano-emitters are subject to high macroscopic electric field FM. We assume that the number of emitting spots, which defines an apparent formal area efficiency of CFE surfaces, depends on the macroscopic electric field. Non-uniformity is described by local enhancement factors , which are randomly assigned to each distinct emitter of a conducting CFE surface, from a discrete probability distribution , with j = 1, 2. It is assumed that , and that . The local current density is evaluated by considering a usual Schottky–Nordheim barrier. The results reproduce the two distinct slope regimes in FN plots when [2, 20] V μm−1 and are analyzed by taking into account the apparent formal area efficiency, the distribution ρ, and the slopes in the corresponding FN plot. Finally, we remark that our results from numerical solution of Laplace’s equation, for an array of conducting nano-emitters with uniform apex radii 50 nm but different local height, supports our theoretical assumptions and could used in orthodox CFE experiments to test our predictions.

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