A high brightness 1064nm MOPA pulsed fiber laser with controlled pulse width, peak power, and pulse energy is used to investigate the effects of changing the peak power and pulse width on the ablation process. Pulses of 10ns to 250ns are applied, with peak powers up to 10kW while maintaining average power. This corresponds to over 3 GW/cm2 fluence levels. The materials used in these experiments are mono and polycrystalline silicon, and aluminum coated silicon. Experimental results indicate that the material removal rates of a short pulse with high peak power is small, and that the material ablation benefits from a leading peak pulse shape at longer pulses of 100 to 150ns. These longer pulses accelerate the material removal by first heating and subsequently melting the substrate material. Material removal rate of about 13µm per scribe, single-pass, is obtained on mono silicon for 10W incident beam, 1m/s scan speed, 100 kHz rep rate and 20 µm spot size with 50% spot overlap. Percussion drilled holes are also demonstrated for 200 µm thick polycrystalline silicon wafer. Through holes are drilled in 1msec using pulses of >50ns. Entry and exit diameters are typically 30 and 20µm, respectively.A high brightness 1064nm MOPA pulsed fiber laser with controlled pulse width, peak power, and pulse energy is used to investigate the effects of changing the peak power and pulse width on the ablation process. Pulses of 10ns to 250ns are applied, with peak powers up to 10kW while maintaining average power. This corresponds to over 3 GW/cm2 fluence levels. The materials used in these experiments are mono and polycrystalline silicon, and aluminum coated silicon. Experimental results indicate that the material removal rates of a short pulse with high peak power is small, and that the material ablation benefits from a leading peak pulse shape at longer pulses of 100 to 150ns. These longer pulses accelerate the material removal by first heating and subsequently melting the substrate material. Material removal rate of about 13µm per scribe, single-pass, is obtained on mono silicon for 10W incident beam, 1m/s scan speed, 100 kHz rep rate and 20 µm spot size with 50% spot overlap. Percussion drilled holes are als...
[1]
François Gallaire,et al.
Time-resolved temperature rise in a thin liquid film due to laser absorption.
,
2009,
Physical review. E, Statistical, nonlinear, and soft matter physics.
[2]
Hans Herfurth,et al.
Micromachining with tailored nanosecond pulses
,
2007,
Photonics North.
[3]
R. Russo,et al.
Experimental investigation of ablation efficiency and plasma expansion during femtosecond and nanosecond laser ablation of silicon
,
2005
.
[4]
Barry Luther-Davies,et al.
Picosecond high-repetition-rate pulsed laser ablation of dielectrics: the effect of energy accumulation between pulses
,
2005
.
[5]
Pascal Deladurantaye,et al.
Material micromachining using a pulsed fiber laser platform with fine temporal nanosecond pulse shaping capability
,
2009,
LASE.
[6]
Andreas Ruf,et al.
Fundamental aspects in machining of metals with short and ultrashort laser pulses
,
2004,
SPIE LASE.
[7]
B. R. Campbell,et al.
A study of material removal rates using the double pulse format with nanosecond pulse laser on metals
,
2008
.
[8]
A. Tünnermann,et al.
Plasma evolution during metal ablation with ultrashort laser pulses.
,
2005,
Optics express.