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- W56515566 abstract "This chapter describes the architecture of N-slit interferometric laser optical systems. The expanded laser beam illuminates the N-slit array where subbeams are created and proceed to propagate toward the detection screen configured by a digital detector. It has been found that although the telescope-convex lens system is polarization neutral, the multiple-prism beam expander has a strong transmission preference for radiation polarized parallel to the plane of propagation. The first step is to match the polarization of the laser to the polarization preference of the multiple-prism beam expander. It has also been found that the focused, extremely elongated, near-Gaussian coherent illumination is used in applications requiring illumination of N-slit arrays with transverse microscopic dimensions, and the unfocused, elongated, near-Gaussian illumination is used in conventional interferometric measurements. In transmission gratings comprising imaging materials of a crystalline nature, the spatial resolution decreases as the spatial frequency increases. This is manifested in a deterioration of the light modulation as the spatial frequency increases. Additionally, for broadband ultrashort pulsed lasers, once the bandwidth of the emission is determined, an approximate estimate of the temporal pulse duration is possible using the time-frequency uncertainty relation." @default.
- W56515566 created "2016-06-24" @default.
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- W56515566 date "2003-01-01" @default.
- W56515566 modified "2023-09-23" @default.
- W56515566 title "Architecture of N-Slit Interferometric Laser Optical Systems" @default.
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- W56515566 doi "https://doi.org/10.1016/b978-012222696-0/50057-0" @default.
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