Self-induced birefringence of white-light continuum generated by interaction of focused femtosecond laser pulses with fused silica Download: 527次
1 Introduction
White-light continuum generation is a universal process that occurs when intense ultrashort laser pulses interact with transparent gases[1], liquids[2, 3] and solids[4, 5]. A white-light continuum is characterized by intense ultrafast broadband with frequencies ranging from the near-UV to near-IR. The multicolored light possesses many of the same desirable properties as conventional laser: intense, collimated and coherent. Therefore it has found wide applications ranging from frequency metrology[6], spectroscopy of semiconductor microstructures and photonic structures[7], optical coherence tomography[8] to time-resolved spectroscopy[9], etc.
Since the discovery of white-light continuum by Robert R. Alfano and Stanley Shapiro in 1969, extensive progress has been achieved on the experimental and theoretical understanding of ultrafast nonlinear and linear processes responsible for white-light continuum generation[7]. It seems that the mystery of white-light continuum has all been decoded. Therefore, recent research activity cares little about the intrinsic properties of white-light continuum, but mainly focuses on how to generate intense and high-efficiency white-light continuum[10, 11] and synthesize it for reproducible few-cycle light waveforms[12–14], which fulfill a central role in attosecond science.
A white-light continuum is believed to be polarized in the direction of the incident pump laser polarization for an isotropic medium[5]. However, in optically isotropic cubic crystals of CaF2 and LiF, Midorikawa et al. observed angular-dependent polarization change of the continuum[15]. Later, a depolarization of the continuum was also reported in the isotropic medium BK-7 glass[16]. By rotating CaF2 and LiF around the optical axis, the transmitted continuum intensity behind the analyzer prism varies cyclically. However, in BK-7 glass, the significant depolarization appears at very high incident laser powers, and plasma effects are assumed to be relevant to the depolarization. In addition to the angular-dependent and laser intensity-relevant properties, depolarization of continuum is still far from being understood.
In this paper, we focus a femtosecond laser into bulk fused silica to induce white-light continuum and also use two orthogonal polarizers to analyze the continuum. As expected, continuum signals can still be detected behind the second polarizer. We name such a phenomenon as self-induced birefringence of continuum. In contrast to previous work, a deeper study of depolarization is presented by exploring the time evolution of the transmitted continuum signal as well as imaging the induced structures. In the following sections, we will find more characteristics of self-induced birefringence of continuum and decode how self-induced birefringence of continuum proceeds in fused silica.
2 Experiment
The laser source is an amplified Ti:sapphire mode-locked laser system (Legend Elite Series, Coherent) with a pulse duration of 50 fs operating at 800 nm with a measured bandwidth of 10 nm and a frequency of 1 kHz. The single pulse energy is varied from 20 to 850 μJ. In this work, commercially available fused silica glass (JGS1) samples with the dimension of 10 mm × 10 mm × 2 mm are used, and their six surfaces are polished to optical grade. The apparatus used in the experiment is depicted in Figure
3 Filamentation without polarizers
When the two lenses shown in Figure
Fig. 2. Original color photographic image of continuum taken at a distance of 180 mm from the focus center when the laser pulse energy is (a) 10 μJ and (b) 550 μJ.
Fig. 3. Beam profile evolution of the transmitted light signal with varied pulse energy and laser exposure time.
Fig. 4. Time evolution of the transmitted signal of the generated continuum at varied pulse energy. Inset of (a): saturation value of the transmitted signal as a function of the pump energy.
Fig. 5. Optical images of the femtosecond laser induced structure under the illumination of light on a transmission microscope with (a) parallel polarizer and (b) crossed polarizer on both sides of the samples. Time evolution of the birefringence structure under cross-polarization illumination at pulse energy of (c) 90 μJ and (d) 550 μJ. represents the laser propagation direction. The red dashed line indicates the focal depth.
4 Time evolution and pulse energy dependence of white-light continuum
When white-light continuum is generated, we can detect the transmission signal behind the second polarizer, which indicates that the polarization of the continuum is changed. A laser beam profiler is used to record the beam profile. Figure
For a more accurate demonstration, we also recorded the power evolution of the probe signal in Figure
Fused silica is an isotropic material. Though depolarization of continuum has been demonstrated in isotropic medium such as BK-7 glass[16], however, the previous BK-7 study looked at the intensity dependence and onset of the induced birefringence, and time evolution property of transmitted continuum signal has not been observed before. In Figures
Laser irradiated bulk fused silica was then viewed under microscope. In Figure
Femtosecond laser induced birefringence in glass is not a new phenomenon. Previous work has indicated that when a femtosecond laser focuses into a bulk glass, optical anisotropy can be created due to anisotropic refractive-index change[23, 24] or self-organized nanograting[25–27]. Yamada et al. found that femtosecond laser induced refractive-index change has an elliptical structure by hydrofluoric acid solution etching the cross-section, and the long axis is parallel to the polarization of incident laser pulses[23]. Shimotsuma et al. found nanogratings were generated inside silica glass after irradiation by a focused linearly polarized femtosecond laser, and revealed that the nanogratings were aligned perpendicularly to the laser polarization direction[26]. Though the laser induced birefringence has been observed in above mentioned work, however, the time evolution feature of self-induced birefringence of white-light continuum has not been reported.
Figures
In Figure
Fig. 6. The dependence of the transmitted continuum behind the second polarizer (a) on the laser exposure time at pulse energy of 550 μJ and (b) on the pulse energy at laser exposure time of 400 s.
Finally, the transmitted spectra behind the second polarizer are also measured in Figure
5 Conclusion
In conclusion, we have recorded the time evolution of self-induced birefringence of white-light continuum in fused silica. This indicates that white-light continuum is synchronously modulated anisotropically in the interaction process of a focused femtosecond laser with fused silica. The birefringence signal of the generated continuum has a growth–saturation property with time evolution, and it becomes more intense for higher laser pulse energies. Optical morphology analysis finally demonstrates that time-evolved anisotropic structures are responsible for self-induced birefringence of the continuum. These properties may be useful for fabrication of polarization-dependent devices.
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Article Outline
J. Qian, G. D. Wang, K. Y. Lou, D. Y. Shen, Q. Fu, Q. Z. Zhao. Self-induced birefringence of white-light continuum generated by interaction of focused femtosecond laser pulses with fused silica[J]. High Power Laser Science and Engineering, 2020, 8(2): 02000e19.