Formation of nanogratings on the surface of a ZnSe crystal irradiated by femtosecond laser pulses

Tianqing Jia(The University of Tokyo), H. X. Chen(State Key Laboratory of Optoelectronic Materials and Technology), Min Huang(The University of Tokyo), Fuli Zhao(Sun Yat-sen University), Jianrong Qiu(Shanghai Institute of Optics and Fine Mechanics), R. X. Li(Shanghai Institute of Optics and Fine Mechanics), Zhenzhu Xu(Shanghai Institute of Optics and Fine Mechanics), Xiyao He(The University of Tokyo), Jiaqi Zhang(The University of Tokyo), Hiroto Kuroda(The University of Tokyo)
Physical Review B
September 23, 2005
Cited by 322

Abstract

Two collinear femtosecond laser pulses, one at wavelength of $800\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$ and the other at $400\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$ (double frequency), simultaneously irradiated the surface of ZnSe crystal, which resulted in regular nanograting with period of $180\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$ on the whole ablation area. We attribute the formation of the nanograting to be due to the interference between the surface scattered wave of $800\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$ lasers and the $400\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$ light. The period of the nanograting $\ensuremath{\Lambda}$ is about $\ensuremath{\lambda}∕2n$, where $n$ is refractive index of the sample, and $\ensuremath{\lambda}$, the laser wavelength. This mechanism is supported by observation of rotation of the nanograting with the polarization of $400\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$ light, and by the dependence of $\ensuremath{\Lambda}\ensuremath{\sim}\ensuremath{\lambda}$ of the nanoripples on the surface of semiconductors and dielectrics.


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