2001
DOI: 10.1116/1.1415515
|View full text |Cite
|
Sign up to set email alerts
|

Interplay of current crowding and current self-quenching effects in planar cold cathodes

Abstract: Articles you may be interested inElectron beam prebunching in planar cold cathodes with surface current carrying thin films Emission uniformity enhancement between microfabricated tips in cold cathode arrays Nongeometric field enhancement in semiconducting cold cathodes and in metal-insulator-semiconductor structures Appl.Space-charge effects and current self-quenching in a metal/CdS/LaS cold cathode

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

2004
2004
2011
2011

Publication Types

Select...
2

Relationship

1
1

Authors

Journals

citations
Cited by 2 publications
(2 citation statements)
references
References 9 publications
(11 reference statements)
0
2
0
Order By: Relevance
“…With enough forward bias on the emitter fingers, electrons emitted from the InP substrate tunnel through the CdS layer and are emitted into vacuum as a result of NEA at the CdS/LaS interface. However, there can be partial trapping of electrons by the LaS semimetallic thin film, which can lead to a lateral current flow and current crowding 11,12 and self-heating effects 13 in the cathode.…”
Section: Our Work Was Motivated By the Original Proposal By Walter Frmentioning
confidence: 99%
“…With enough forward bias on the emitter fingers, electrons emitted from the InP substrate tunnel through the CdS layer and are emitted into vacuum as a result of NEA at the CdS/LaS interface. However, there can be partial trapping of electrons by the LaS semimetallic thin film, which can lead to a lateral current flow and current crowding 11,12 and self-heating effects 13 in the cathode.…”
Section: Our Work Was Motivated By the Original Proposal By Walter Frmentioning
confidence: 99%
“…II, we develop a small ac signal equivalent circuit of the InP/CdS/LaS cold cathode structure depicted in Fig. 15 If we call W E Ј the width of the Au fingers on either sides of the emission window and W E the width of the emission window, the amount of base current is then simply given by A small signal equivalent circuit of the cathode is derived.…”
Section: Introductionmentioning
confidence: 99%