Nanograting fabricated with femtosecond laser pulses
Nanograting fabricated with femtosecond laser pulses
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用飞秒激光脉冲制造纳米光栅
DOI:
10.1117/2.1201210.004516
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发表时间:
2012
期刊:
影响因子:
--
通讯作者:
G. Miyaji and K. Miyazaki
中科院分区:
文献类型:
--
作者:
Atsushi Sugita;Yasuaki Sato;Kazuma Ito;Kenta Murakami;Yasuaki Tamaki;Nobuyuki Mase;Yoshimasa Kawata and Shigeru Tasaka;Kenji Tamasaku;G. Miyaji and K. Miyazaki
Intense femtosecond laser pulses are a common tool in precision processing of a variety of materials, which are needed in the fabrication of, for example, electro-optical devices and microelectromechanical systems. The advantage of using femtosecond laser pulses for material processing is the ultrafast deposition of high-density energy onto the target and the resulting suppression of undesirable thermal and mechanical effects in the lightmatter interaction. In addition, observations of self-organized, surface nanostructure formations in femtosecond-laser ablation experiments have found the size of these structures is typically 1/10–1/5 of the laser wavelength, 1–4 which suggests that femtosecond lasers have the potential to sculpt, or ‘nanoprocess,’structures smaller than the diffraction limit. To find a new route to femtosecond-laser nano-processing, we focused our attention on the nanoscale, ultrafast light-matter interaction responsible for nanostructuring. We explored in particular the use of superimposed multiple shots of low-fluence femtosecond laser pulses. Our preliminary studies with dielectric and semiconductor materials have shown that the laserinduced near-field plays a fundamental role in the nanoscale ablation of a corrugated surface, 5, 6 and the origin of periodicity can be attributed to the excitation of surface plasmon polaritons (SPPs) in the surface layer. 7, 8Based on the model of nanostructuring, we successfully fabricated a nanograting with a uniform period on a crystalline gallium nitride (GaN) surface. We performed our experiment in air (as opposed to vacuum) using linearly polarized 800-nm, 100-fs laser pulses from a Ti: sapphire laser system operated at a repetition rate of 10Hz. In the first-step of a two-step process, we split the femtosecond laser output into two beams. As schematically illustrated in Figure 1 (a), Beam 1 is normally incident on the target while Beam 2 is incident at an angle  with respect to the normal. The two beams overlap on the target surface to create interference fringes in the direction perpendicular to the laser