Kudryashov Sergey, Gulina Yulia, Danilov Pavel, Smirnov Nikita, Rimskaya Elena, Krasin George, Saraeva Irina, Shelygina Svetlana, Rupasov Alexey, Pershin Kirill, Tsygankov Alexander, Gorevoy Alexey
Opt Lett. 2025 Jan 1;50(1):129-132. doi: 10.1364/OL.547650.
Micromodification in bulk undoped polymethylmethacrylate (PMMA) by single focused (numerical aperture (NA) = 0.25), 1030-nm 250-fs laser pump pulses was explored by pump self-transmittance; optical, 3D-scanning confocal photoluminescence (PL); Raman micro-spectroscopy; and optical polarimetric and interferometric microscopy. Starting from the threshold pulse energy = 0.4 ± 0.1 μJ (peak laser intensity ≈ 8 TW/cm), visible bright micro-voxels emerged inside PMMA at the 100 ÷ 300-μm depth, with their PL-acquired dimensions increasing versus pulse energy. Optical phase change was interferometrically measured in the voxels at the 532-nm wavelength, exhibiting versus the pulse energy the isotropic refractive index increase Δ = +(4 ÷ 10) × 10, and a new 1640-cm peak of C=C vibrations emerged in the Raman spectra. Pump self-transmittance measurements demonstrated the predominating eight-photon absorption (excited energy level ≈ 9.7 eV, coefficient ≈ 3 × 10 cm/TW) at the sub-threshold < , implying photoionization of the PMMA chains (the ionization potential of MMA molecule ≈ 9.7 eV). At higher peak intensities > , inverse brems-strahlung absorption (coefficient ∼10cm) of near-critical micro-plasma (density >5 × 10 cm) predominates over the multi-photon PMMA absorption, providing the bulk energy density >6 × 10 J/cm and the temperature rise Δ > 2.2 × 10 K, which are sufficient for PMMA (de)polymerization near the equilibrium bulk temperature ≈ 220°C. These results uncover the quantitative mechanism of fs-laser modification of PMMA, justifying the previous qualitative findings and enabling controllable energy deposition during fs-laser PMMA micromachining of diverse functional applications.
通过泵浦自透过率、光学三维扫描共焦光致发光(PL)、拉曼显微光谱以及光学偏振和干涉显微镜,研究了用单聚焦(数值孔径(NA) = 0.25)、1030 nm、250 fs激光泵浦脉冲对块状未掺杂聚甲基丙烯酸甲酯(PMMA)进行的微改性。从阈值脉冲能量 = 0.4 ± 0.1 μJ(峰值激光强度 ≈ 8 TW/cm)开始,在PMMA内部100÷300 μm深度处出现了可见的明亮微体素,其通过PL获得的尺寸随脉冲能量增加。在532 nm波长下对微体素进行干涉测量光学相位变化,结果表明,随着脉冲能量增加,各向同性折射率增加Δ = +(4÷10)×10 ,并且在拉曼光谱中出现了新的1640 cm的C = C振动峰。泵浦自透过率测量表明,在低于阈值 < 时,主要是八光子吸收(激发能级≈9.7 eV,系数 ≈ 3×10 cm/TW),这意味着PMMA链发生了光电离(MMA分子的电离势≈9.7 eV)。在较高的峰值强度 > 时,近临界微等离子体(密度>5×10 cm)的逆轫致辐射吸收(系数~10 cm)在多光子PMMA吸收中占主导地位,提供了大于6×10 J/cm的体能量密度和大于2.2×10 K的温度升高Δ ,这足以在接近平衡体温度 ≈ 220°C时使PMMA发生(解)聚合。这些结果揭示了飞秒激光对PMMA改性的定量机制,证实了先前的定性研究结果,并使得在用于各种功能应用的飞秒激光PMMA微加工过程中实现可控的能量沉积成为可能。