2018
DOI: 10.1109/ted.2018.2824401
|View full text |Cite
|
Sign up to set email alerts
|

Nearly Ballistic Electron Transport in an Out-of-Plane Nanoscale Defect-Void Channel

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
5

Citation Types

0
9
0

Year Published

2019
2019
2022
2022

Publication Types

Select...
5
1

Relationship

2
4

Authors

Journals

citations
Cited by 14 publications
(9 citation statements)
references
References 34 publications
0
9
0
Order By: Relevance
“…Even at low bias voltages (<0.5 V), an intense electric field of 10 5 V/cm is formed between the top electrodes due to the narrow nanogap of ∼50 nm, which is sufficient to cause the dielectric breakdown of air and lower the potential barrier of the metal–air interface, ,,, resulting in electron emission from the cathode. Furthermore, the geometrical field enhancement effect of the two-dimensional electrode with a sharp edges or surface protrusions can significantly enhance the localized electric field around the edge to 10 7 V/cm, ,,,, which is sufficient to lower the potential barrier at the air–metal interface and initiate electron emission from the cathode edge. Figure b, top illustrates an energy band diagram of a lateral device.…”
Section: Resultsmentioning
confidence: 99%
“…Even at low bias voltages (<0.5 V), an intense electric field of 10 5 V/cm is formed between the top electrodes due to the narrow nanogap of ∼50 nm, which is sufficient to cause the dielectric breakdown of air and lower the potential barrier of the metal–air interface, ,,, resulting in electron emission from the cathode. Furthermore, the geometrical field enhancement effect of the two-dimensional electrode with a sharp edges or surface protrusions can significantly enhance the localized electric field around the edge to 10 7 V/cm, ,,,, which is sufficient to lower the potential barrier at the air–metal interface and initiate electron emission from the cathode edge. Figure b, top illustrates an energy band diagram of a lateral device.…”
Section: Resultsmentioning
confidence: 99%
“…10,18 In the electrical discharge plasma system, a highly localized E-field is crucial for the electron emissions process and, consequently, induced impact ionization. 14,16,19 Electrons with high kinetic energy can travel in the air within the length of the mean free path (~ 100 nm) 20,21 before colliding with the gas atoms, molecules, electrons, and ions, resulting in gas breakdown. Besides, electrons and ions within the gas can conduct a small current, disturbing the equilibrium and resulting in the generation of several active plasma chemical species (see Fig.…”
Section: Resultsmentioning
confidence: 99%
“…A large localized electric field naturally developed around the ground object (either operators or metal rod) and on the PP web mesh surface with its roughness in the micronanoscale size. Similar to nanoscale field emission devices and corona discharge plasma in the air medium [13,27,28], the nanoscale surface roughness of the insulator surface or metal edge with a microscale radius of curvature can result in a localized electric field of up to ~100 kV/cm [27][28][29]. Thus, we can exploit the benefit of highly localized electric field-assisted electron emissions from the PP surface to the surrounding ambient air to dissipate the accumulated electrostatic charges.…”
Section: Resultsmentioning
confidence: 99%
“…Thus, the energy barrier limits the electrons flowing out to the air ambient. However, when there is normalized electric field penetration, the energy barrier width becomes sufficiently lower and thin to cause an electron to escape from the emitter surface by thermionic emission, thermionic field emission, and Fowler-Nordheim (FN) tunneling (blue dashed line) [29]. The small radius of curvature of the PP fiber and metal edge is necessary for self-induced electric field focusing.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation