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Online proceedings - EDA Publishing Association

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11-13 <br />

May, 2011, Aix-en-Provence, France<br />

Table 1. Etching results of the 1 M HF<br />

<br />

Voltage Channel depth Etching rate<br />

(V) (μm) (μm/hr)<br />

0.8 18.94 3.788<br />

1 20 4<br />

1.2 19.31 3.862<br />

1.5 14.06 2.812<br />

(2) Etching results of the 2M HF<br />

Figure 7 and Table 2 illustrate the etching results of the<br />

2M HF. As shown in Table 2, the applied voltage of 1V rather<br />

than the 1.5 V produced the fastest etching. It is presumed that<br />

the 1.5 V potential might reduce the effect of the electric field<br />

concentration, resulting in the increasing of the electric hole on<br />

the pore wall. The increasing etching reactions on the pore wall<br />

produced rugged wall surface. Since the etching reactions did<br />

not rivet on the pore tip, the etching rate is thus reduced (Figure<br />

7D).<br />

Figure 8. SEM images of the 4M HF etching results, (A)0.8V; (B)1V; (C)1.2V;<br />

(D)1.5V<br />

Table 3. Etching results of the 4 M HF<br />

Voltage<br />

(V)<br />

Channel depth<br />

(μm)<br />

Etching rate<br />

(μm/hr)<br />

0.8 94.62 18.924<br />

1 56.9 11.38<br />

1.2 22.765 4.553<br />

1.5 36.216 7.2432<br />

Figure 7. SEM images of the 2M HF etching results, (A)0.8V; (B)1V; (C)1.2V;<br />

(D)1.5V<br />

Table 2. Etching results of the 2 M HF<br />

Voltage<br />

(V)<br />

Channel depth<br />

(μm)<br />

Etching rate<br />

(μm/hr)<br />

0.8 29.6 5.92<br />

1 58.984 11.7968<br />

1.2 50.52 10.104<br />

1.5 49.743 9.9486<br />

(3) Etching results of the 4M HF<br />

The 4M HF etching results are shown in Figure 8 and<br />

Table 3. Figure 8 indicates that only the applied voltage of 0.8<br />

V can conduct acceptable etching. Since the concentration of<br />

HF is 4M, a larger applied voltage will draw forth far enough<br />

electric holes on the wafer surface to react with the fluoric ions.<br />

The etching process thus starts randomly from the wafer<br />

surface rather than form the tip of the inverted pyramids (Figure<br />

8B-8D).<br />

3.2 Effect of the protective Si 3 N 4 layer<br />

Electric field concentration is the basic principle of anodic<br />

etching. In the study, the spots of electric field concentration<br />

consist of the tips of the inverted pyramids and the four corners<br />

of etch pre-etched pore. The protective Si 3 N 4 layer further<br />

enhances this phenomenon. It is also interesting to investigate<br />

the influence of the protective Si 3 N 4 layer. The parameters for<br />

Figure 7(B) (HF=2M, applied voltage=1V) which had better<br />

etching performance are used for the etching without a Si 3 N 4<br />

layer.<br />

Figure 9 compares the results of the with Si 3 N 4 layer and the<br />

without Si 3 N 4 layer etchings. The top row and the bottom row<br />

illustrate the results of the without Si 3 N 4 layer and with Si 3 N 4<br />

layer etching, respectively. The etching time of the without<br />

Si 3 N 4 layer etching is 3 hr. The etching rate, which is estimated<br />

to be 11.61 m/hr, is close to that of the with Si 3 N 4 layer etching.<br />

For the without Si 3 N 4 layer etching, randomly etched cavities<br />

due to the reactions between fluoric acids and electron holes on<br />

the silicon surface can be observed. It can also be found that the<br />

wet etched squares are widened. For the Si 3 N 4 layer protective<br />

etching, symmetrical cannelures stretching from the four<br />

corners of etch wet etched square. It is presumed that the<br />

electric field concentration at the corners of a wet etched square<br />

at the initial stage of etching leads to the directional etchings of<br />

the cannelures. However, vertical microchannels having the<br />

size close to the wet etched square were fabricated. It reveals<br />

that a Si 3 N 4 layer is desired for a successful etching of porous<br />

array in silicon.<br />

26

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