2000
DOI: 10.1016/s0022-3093(00)00006-5
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Field emission studies of diamond-like films grown by RFCVD

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Cited by 18 publications
(5 citation statements)
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“…The curves illustrate that the emission currents are insensitive but detectable to be dependent on temperatures. This behaviour is quite different from the temperature dependence of the FE characteristic of diamond films or diamond-like (DLC) films [30][31][32], because structure and strong field emission on the sharp tip of CNTs is different from that of a flat emitter. It is suggested that the dominant contribution to field emission comes from the semiconducting amorphous carbon at the sharp tip of CNTs, which have a high aspect ratio.…”
Section: Resultsmentioning
confidence: 77%
“…The curves illustrate that the emission currents are insensitive but detectable to be dependent on temperatures. This behaviour is quite different from the temperature dependence of the FE characteristic of diamond films or diamond-like (DLC) films [30][31][32], because structure and strong field emission on the sharp tip of CNTs is different from that of a flat emitter. It is suggested that the dominant contribution to field emission comes from the semiconducting amorphous carbon at the sharp tip of CNTs, which have a high aspect ratio.…”
Section: Resultsmentioning
confidence: 77%
“…The surface morphology of the film indicated that the film surface is not flat and the roughness is about 0.8 μm on average. The emission is more likely to be a significant particular sites rather than over the entire surface (4), (8) . There seems to be the enhancement factor such as the surface roughness on the film with respect to the emission phenomenon.…”
Section: Resultsmentioning
confidence: 99%
“…Diamond like carbon (DLC) films are generally prepared from the various gas phase methods, such as ion-beam sputtering, laser ablation deposition and chemical vapor deposition techniques (1)- (8) .…”
Section: Introductionmentioning
confidence: 99%
“…The field emission was measured under a vacuum of 10 −6 torr with a Teflon spacer of 150 m and a Mo (thickness of 3 m) coated glass plate displaying as the anode. 16 The field emission properties do not follow the Fowler-Nordheim equation but comply with the metal-semiconductor tunneling theory. 17 18 The circuit for performing the micro-EDM is shown in Figure 2 where the integrated circuit SG3524 produces the controlling square clocks which are amplified by the high voltage transistor IRF640 to control the switching voltage for embarking the discharge electrodes D6 to start or close.…”
Section: Methodsmentioning
confidence: 95%