Developments in Ceramic Materials Research
Developments in Ceramic Materials Research
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.