Chinese Journal of Lasers, Volume. 50, Issue 18, 1813005(2023)
Interaction Between Ultrafast Laser and Transparent Hard Materials: from Phase Change Mechanism to Eternal Optical Data Storage
Fig. 1. Interaction between femtosecond laser and material. (a) Timescale of a femtosecond laser exciting electron and lattice processes in solid[28]; (b) ionization rate for fused silica with a gap of 9 eV from Keldysh’s theory (solid line) as function of laser intensity, and their comparison between multiphoton ionization (dotted line) and tunnel ionization (dash-dotted line)[30]
Fig. 2. Forming mechanisms and applications of Type I structure. (a) Laser beam is used to modify the refractive index of the material to create the waveguide; (b) refractive index of Type Ⅰ material shows a uniform positive change accompanied by darkening[49]; (c) element distribution caused by the heat transfer induced by temperature-gradient-driven diffusion[52]; (d) the structure is formed after the laser with repetition of 25 MHz, pulse width of 30 fs, energy of 5 nJ is focused by an objective lens with a numerical aperture of 1.4[56]; (e) X directional coupler formed by Type Ⅰ modification[60]
Fig. 3. Ultrafast laser-induced Type Ⅲ/Ⅳ structures. (a) SEM images of the cross-section of nanopores in sapphires[63]; (b) storing binary data in molten silicon dioxide[73]; (c) storing images in molten silicon dioxide[73]; (d) ultrashort laser pulses triggering space-limited micro-explosion to form high density phases[67]; (e) optical preparation of three-dimensional photonic crystals in high refractive index LiNbO3 crystals[71]
Fig. 4. Formation mechanism of nano-grating. (a) SEM image of nano-grating[19]; (b) incident light-polaron interference model[19]; (c) anisotropic growth model of nano-plasma[76]; (d) surface plasmon resonance model[78]; (e) schematic diagram of electromagnetic formation mechanism of periodic nanostructures[81]
Fig. 6. Pulse width modulation effect[88]. (a) Retardance (left) and transmission (right) images of birefringent structures written at different durations; (b) refractive index changes of modified regions written with different pulse widths; (c) retardance and transmittance of modified regions corresponding to different pulse widths; (d) SEM images of Type X and Type Ⅱ structures after polishing and etching
Fig. 7. Thermal modulation of nanograting[90]. (a) Comparison of birefringence structures before and after modulating energy; (b) simulation of temperature evolution in the focus center; (c) simulation of laser intensity distribution around nanocrystals with different diameters; (d) birefringence photo of the structures induced by two seed pulses and eight subsequent pulses; (e) SEM images of nano-layered structures after polishing and KOH etching
Fig. 8. Solutions for the challenges which eternal optical storage is facing. (a) Simulations of the electric field intensity distribution[41]; (b) slow-axis orientation map of the free-form written nanogrooves by OFIB technology (the retardance at a wavelength of 546 nm is 9 nm)[41]; (c) schematic of picosecond laser space-time control optical path[92]; (d) relationship between retardance and pulse number[91]
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Ziting Liu, Yiming Yuan, Ziyue Li, Wei Gong, Xu Zhang, Xinjing Zhao, Yi Wang, Zhenze Li, Lei Wang. Interaction Between Ultrafast Laser and Transparent Hard Materials: from Phase Change Mechanism to Eternal Optical Data Storage[J]. Chinese Journal of Lasers, 2023, 50(18): 1813005
Category: micro and nano optics
Received: Apr. 18, 2023
Accepted: Jul. 3, 2023
Published Online: Sep. 12, 2023
The Author Email: Wang Lei (leiwang1987@jlu.edu.cn)