Verification of shielding effect predictions for large area field emitters

A recent analytical model for large area field emitters [D. Biswas and R. Rudra, Phys. Plasmas 25, 083105 (2018)], based on the line charge model (LCM), provides a simple approximate formula for the field enhancement on hemiellipsoidal emitter tips in terms of the ratio of emitter height to pairwise...

Full description

Bibliographic Details
Main Authors: Rashbihari Rudra, Debabrata Biswas
Format: Article
Language:English
Published: AIP Publishing LLC 2019-12-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.5126674
id doaj-26a4623aac6f4f1383ee842138c392a2
record_format Article
spelling doaj-26a4623aac6f4f1383ee842138c392a22020-11-25T00:14:28ZengAIP Publishing LLCAIP Advances2158-32262019-12-01912125207125207-410.1063/1.5126674Verification of shielding effect predictions for large area field emittersRashbihari Rudra0Debabrata Biswas1Bhabha Atomic Research Centre, Mumbai 400 085, IndiaBhabha Atomic Research Centre, Mumbai 400 085, IndiaA recent analytical model for large area field emitters [D. Biswas and R. Rudra, Phys. Plasmas 25, 083105 (2018)], based on the line charge model (LCM), provides a simple approximate formula for the field enhancement on hemiellipsoidal emitter tips in terms of the ratio of emitter height to pairwise distance between neighboring emitters. The formula, verified against the exact solution of the linear LCM, was found to be adequate, provided that the mean separation between emitters is larger than half the emitter height, h. In this paper, we subject the analytical predictions to a more stringent test by simulating (i) an infinite regular array and (ii) an isolated cluster of 10 random emitters, using the finite element software COMSOL v5.4. In the case of the array, the error in the apex field enhancement factor (AFEF) is found to be less than 0.25% for an infinite array when the lattice constant c ≥ 1.5h, increasing to 2.9% for c = h and 8.1% for c = 0.75h. For an isolated random cluster of 10 emitters, the error in large AFEF values is found to be small. Thus, the error in the net emitted current is small for a random cluster compared to a regular infinite array with the same (mean) spacing. The LCM thus provides a reasonable analytical tool for optimizing a large area field emitter.http://dx.doi.org/10.1063/1.5126674
collection DOAJ
language English
format Article
sources DOAJ
author Rashbihari Rudra
Debabrata Biswas
spellingShingle Rashbihari Rudra
Debabrata Biswas
Verification of shielding effect predictions for large area field emitters
AIP Advances
author_facet Rashbihari Rudra
Debabrata Biswas
author_sort Rashbihari Rudra
title Verification of shielding effect predictions for large area field emitters
title_short Verification of shielding effect predictions for large area field emitters
title_full Verification of shielding effect predictions for large area field emitters
title_fullStr Verification of shielding effect predictions for large area field emitters
title_full_unstemmed Verification of shielding effect predictions for large area field emitters
title_sort verification of shielding effect predictions for large area field emitters
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2019-12-01
description A recent analytical model for large area field emitters [D. Biswas and R. Rudra, Phys. Plasmas 25, 083105 (2018)], based on the line charge model (LCM), provides a simple approximate formula for the field enhancement on hemiellipsoidal emitter tips in terms of the ratio of emitter height to pairwise distance between neighboring emitters. The formula, verified against the exact solution of the linear LCM, was found to be adequate, provided that the mean separation between emitters is larger than half the emitter height, h. In this paper, we subject the analytical predictions to a more stringent test by simulating (i) an infinite regular array and (ii) an isolated cluster of 10 random emitters, using the finite element software COMSOL v5.4. In the case of the array, the error in the apex field enhancement factor (AFEF) is found to be less than 0.25% for an infinite array when the lattice constant c ≥ 1.5h, increasing to 2.9% for c = h and 8.1% for c = 0.75h. For an isolated random cluster of 10 emitters, the error in large AFEF values is found to be small. Thus, the error in the net emitted current is small for a random cluster compared to a regular infinite array with the same (mean) spacing. The LCM thus provides a reasonable analytical tool for optimizing a large area field emitter.
url http://dx.doi.org/10.1063/1.5126674
work_keys_str_mv AT rashbiharirudra verificationofshieldingeffectpredictionsforlargeareafieldemitters
AT debabratabiswas verificationofshieldingeffectpredictionsforlargeareafieldemitters
_version_ 1725390276475748352