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Online proceedings - EDA Publishing Association

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increased.<br />

11-13 <br />

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

<br />

Power meter<br />

LD@1553nm<br />

collimator<br />

3.6μm<br />

2.5μm<br />

MMF-fiber<br />

(a)<br />

1mm/s<br />

(b)<br />

2mm/s<br />

(c)<br />

3mm/s<br />

Fig. 4 Fabrication with various scanning speeds at E = 170 mW and<br />

d = 10 μm<br />

3.6μm<br />

(a)<br />

5mm/s<br />

3.7μm<br />

(d)<br />

8mm/s<br />

3.3μm<br />

(b)<br />

6mm/s<br />

3.3μm<br />

(e)<br />

9mm/s<br />

2.3μm<br />

(c)<br />

7mm/s<br />

2.5μm<br />

(f)<br />

10mm/s<br />

Fig. 5 Fabrication with various scanning speeds at E = 170<br />

mW and d = 0 μm<br />

The laser power was increased to 230 mW to modify fused<br />

silica 10 μm in depth. Scanning speed should be increased to<br />

avoid surface ablation. The results in Fig. 5 show that the<br />

fused silica is ablated given scanning speeds between 5 mm/s<br />

and 7 mm/s; and modified widths of3.7μm, 3.3μm and 2.5μm<br />

correspond to scanning speeds of 8 mm/s, 9 mm/s and 10<br />

mm/s, proving that the fused silica can be modified at different<br />

depths through focusing and tuning the laser power and<br />

scanning speed.<br />

2. Waveguide propagating loss measurement<br />

Fig. 6 shows the system for measuring waveguide<br />

propagating loss. The system conducts the laser diode (LD,<br />

center wavelength = 1553 nm) to the waveguide layer on the<br />

XYZ-rotation stage. In the end of waveguide layer, the<br />

collimator couples the multi-mode optic fiber to the power<br />

meter for acquiring and analyzing signal. The results show<br />

that the propagating loss are 4.6 dB/cm、4.8 dB/cm、6.2<br />

dB/cm as the scanning velocities are 8 mm/s, 9 mm/s and 10<br />

mm/s, respectively, with 230 mW and 10 μm of depth. It<br />

indicates that the increased scanning velocity causes the<br />

larger energy loss due to the low absorbing energy of fused<br />

silica.<br />

XYZ-rotation<br />

stage<br />

Transmission (dBm)<br />

0<br />

-5<br />

-10<br />

-15<br />

-20<br />

-25<br />

-30<br />

-35<br />

-40<br />

LD<br />

-45<br />

1553.2 1553.4 1553.6 1553.8 1554.0 1554.2<br />

Wavelength (nm)<br />

Fig. 6 The system for measuring waveguide propagating loss<br />

Table 2 Fabrication parameters of waveguide using<br />

femtosecond laser<br />

Laser<br />

power<br />

E<br />

(mW)<br />

170<br />

230<br />

Scanning focusing<br />

velocity depth<br />

NF<br />

results<br />

v<br />

s d<br />

(KJ/cm 2 )<br />

(mm/s) (μm)<br />

1<br />

ablation 7.191<br />

2 ablation 3.596<br />

3 ablation 2.397<br />

4 0 ablation 1.798<br />

5 waveguide 1.438<br />

6 waveguide 1.198<br />

7 waveguide 1.027<br />

5<br />

ablation 1.946<br />

6 ablation 1.621<br />

7 ablation 1.390<br />

10<br />

8 waveguide 1.216<br />

9 waveguide 1.081<br />

10 waveguide 0.973<br />

3. Waveguide discussion<br />

The laser power, the diameter of the laser beam, the<br />

scanning speed and the rate of repetition are all very<br />

influential factors in laser machining. This study analyzes the<br />

machining performance with NF factor [10], as shown below.<br />

2ω0<br />

PRF<br />

NF =<br />

(5)<br />

vs<br />

where ω is the minimal radius of the laser beam, R = 1<br />

0<br />

MHz is the repetition rate, and E<br />

F p<br />

= is the average<br />

2<br />

Rπω 0<br />

fluence per lasing. In this study, the laser wavelength, λ , is<br />

532 nm. The focus distance of the lens, f , is 20 mm. The<br />

diameter of the incident laser, D, is 5 mm. The ω is 1.5 μm,<br />

0<br />

estimated by the 1.05 of the measured laser beam quality<br />

factor ( D<br />

M<br />

2 πω0<br />

= ). E is the laser power. Substituting these<br />

2λf<br />

parameters into Eq.(5), the range of the NF value is 1.438 –<br />

0.973 KJ/cm 2 , indicating the range of fabrication energy of<br />

247

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