Physics-based derivation of a formula for the mutual depolarization of two post-like field emitters

Abstract

Recent analyses of the field enhancement factor (FEF) from multiple emitters have revealed that the depolarization effect is more persistent with respect to the separation between the emitters than originally assumed. It has been shown that, at sufficiently large separations, the fractional reduction of the FEF decays with the inverse cube power of separation, rather than exponentially. The behavior of the fractional reduction of the FEF encompassing both the range of technological interest $0<c/h\lesssim 5$ ($c$ being the separation and $h$ is the height of the emitters) and $c\to \infty$, has not been predicted by the existing formulas in field emission literature, for post-like emitters of any shape. In this letter, we use first principles to derive a simple two-parameter formula for fractional reduction that can be of interest for experimentalists to modeling and interpret the FEF from small clusters of emitters or arrays in small and large separations. For the structures tested, the agreement between numerical and analytical data is $\sim 1\%$.

References in corpus (2)

• Physical electrostatics of small field emitter arrays/clusters
• Origin of the literature discrepancies in the fractional reduction of the apex-field enhancement factor considering small clusters of field emitters

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• Analytical Advances about the apex Field Enhancement Factor of a Hemisphere on a Post Model