The 82nd JSAP Autumn Meeting 2021

Presentation information

Oral presentation

3 Optics and Photonics » 3.7 Laser processing

[11a-N321-1~11] 3.7 Laser processing

Sat. Sep 11, 2021 9:00 AM - 12:00 PM N321 (Oral)

Mizue Mizoshiri(Nagaoka Univ. of Tech.)

11:30 AM - 11:45 AM

[11a-N321-10] Femtosecond laser pulses with GHz bursts in MHz burst for ablation enhancement circumventing air ionization

〇(P)Francesc CaballeroLucas1, Shota Kawabata1,2, Kotaro Obata1, Godai Miyaji2, Koji Sugioka1 (1.RIKEN RAP, 2.Tokyo Univ. of A. & T.)

Keywords:GHz burst mode, laser ablation, surface microfabrication

Ultrashort laser pulses are extending in an increasing variety of applications as a high precision microfabrication technique owing to the great confinement of the processing within the irradiated zone. This enables handling a broad extent of materials with little heat diffusion, ensuring precise material ablation. However, ultrashort pulsed lasers face serious challenges for attaining high-throughput material removal. The use of higher laser powers for increasing ablation rates can lead to detrimental effects due to heat accumulation and air ionization. Recently, GHz burst mode laser ablation has been proposed to overcome these limitations thanks to ablation cooling. Bursts of ultrafast laser pulses contribute to material ablation before the residual heat generated by preceding pulses diffuses away from the irradiated region. In addition, reduction of the pulse energy needed for material ablation is also observed. Owing to that, increased ablation efficiencies have been reported. Following this approach, we study the influence of different configurations of the burst mode on ablation of crystalline silicon samples. To this end, multiple bursts (2-5 bursts) at a repetition rate of 64 MHz, each containing various pulses (2-25 pulses) at an ultrafast repetition rate of 5 GHz, were focused onto the sample surface. Results give evidence of the distinct outcomes in ablation among the different burst mode configurations in contrast to single shot ablation. Specifically, the distribution of the total delivered energy in the burst mode allows not to induce air breakdown by the high intensity of single-mode, resulting in better surface smoothness of the ablated area and an increased ablated volume. Thanks to that, the ablated volume increased from 82 μm3 with a depth of 2.9 μm for single shot ablation to 90 μm3 with 4.0 μm depth for burst mode (5 bursts with 25 intrapulses) even at the same total accumulated energy.