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Developments in Ceramic Materials Research

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Field Emission Display on <strong>Ceramic</strong> 255<br />

In this figure, the curve shows a gate potential voltage ramped from 80 V up to 150 V,<br />

with <strong>in</strong>crement of 1 V <strong>in</strong> step. The leakage current value was far below 1% of the emission<br />

current value for the whole course, <strong>in</strong>dicat<strong>in</strong>g a good quality of the dielectric <strong>in</strong>sulat<strong>in</strong>g layer.<br />

Field emission can be described <strong>in</strong> physics by the Fowler-Nordheim equation [37], which<br />

can be written <strong>in</strong> a simple form as:<br />

I = aV<br />

b<br />

−<br />

2 V<br />

e<br />

(1.1)<br />

where I – emission current<br />

V – applied electric field potential voltage<br />

a and b are treated as constants that are related with the emitt<strong>in</strong>g area and geometric<br />

factor of the emitter.<br />

Equation (1.1) can be rewritten <strong>in</strong> another mathematics function as the follow<strong>in</strong>g:<br />

⎛<br />

I ⎞ b<br />

ln⎜ = − ln a<br />

2 ⎟<br />

⎝V<br />

⎠ V<br />

(1.2)<br />

Ideally plott<strong>in</strong>g ln(I/V 2 ) versus 1/V should yield a straight l<strong>in</strong>e. In fact, this l<strong>in</strong>ear form of<br />

Fowler-Nordheim plot is widely used <strong>in</strong> practice to dist<strong>in</strong>guish field emission mechanism<br />

from other electron emission mechanisms. Convert<strong>in</strong>g the I-V curve <strong>in</strong>to the function ln(I/V 2 )<br />

versus 1/V gives Fowler-Nordheim plot. Figure 8 (b) shows the Fowler-Nordheim plot<br />

version of the I-V curve <strong>in</strong> Figure 8 (a). The l<strong>in</strong>ear curve proves the nature of field emission<br />

mechanism from the micro field emitters.<br />

To use the micro field emitters for display application, it is important to study the<br />

emission stability and life time characteristics. In the stability test, <strong>in</strong>dividual pixel of the<br />

micro field emitters was randomly chosen and was applied to a fixed gate potential voltage<br />

while the emission current was monitored over a period of time. A LabView test graph<br />

show<strong>in</strong>g an emission current trace for a length of 17.5 hours from a pixel is illustrated <strong>in</strong><br />

Figure 9. The data were acquired after a prelim<strong>in</strong>ary tip clean<strong>in</strong>g process at a high emission<br />

current of ~8×10 -5 A by keep<strong>in</strong>g the gate voltage at 155 V for 30 seconds, followed by<br />

reduc<strong>in</strong>g the gate potential down to a lower value of 150 V for this life time test. The<br />

emission current and the leakage current data were collected, averaged and stored <strong>in</strong> memory<br />

every m<strong>in</strong>ute under the control of the automatic data acquisition system. The leakage current<br />

value is well below 1% of the emission current over the entire test period, <strong>in</strong>dicat<strong>in</strong>g a high<br />

quality SiO2 <strong>in</strong>sulat<strong>in</strong>g layer.<br />

In order to <strong>in</strong>vestigate the uniformity of emission current from the micro field emitters on<br />

ceramic substrate, a comparison study with micro field emitters on silicon wafer was<br />

performed. To do this, an identical fabrication procedure to produce micro field emitters on<br />

ceramic substrate was applied to silicon wafers. The wafers were diced <strong>in</strong>to the same<br />

dimension as the ceramic substrate. After a surface clean<strong>in</strong>g treatment, a th<strong>in</strong> dielectric layer<br />

of SiO2 was deposited us<strong>in</strong>g PECVD onto the silicon substrates to <strong>in</strong>sulate the surface. Then<br />

the silicon substrates went through the same batch process along with the ceramic substrates<br />

for micro field emitters’ fabrication.

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