“…For a 36 cm long gain medium, a coherence radius of 550 mm measured at 1.5 m from the source that includes almost half of the entire laser power is obtained. The coherence radius was measured analyzing the fringe visibility of the interference fringes obtained when a mask with two pinholes at different separations was placed at selected distances from the source [65,66]. The coherence radius R c characterizes the transverse coherence of the laser beam, and was defined following the convention of coherence area used by Goodman [67].…”
“…For a 36 cm long gain medium, a coherence radius of 550 mm measured at 1.5 m from the source that includes almost half of the entire laser power is obtained. The coherence radius was measured analyzing the fringe visibility of the interference fringes obtained when a mask with two pinholes at different separations was placed at selected distances from the source [65,66]. The coherence radius R c characterizes the transverse coherence of the laser beam, and was defined following the convention of coherence area used by Goodman [67].…”
“…[18,19] The high temporal and spatial coherence of the table top SXR laser permits the recording of large NA holograms for high resolution holographic imaging. [20,21] Using the Gabor's geometry shown in figure 1 two holograms with two different NA were obtained varying the distance object-hologram z p . The two selected distances were z p ≈ 4 mm and z p ≈ 120 µm.…”
Sorf X-ray (SXR) Gabor's holograms recorded with a highly coherent table top λ = 46.9 nm laser were obtained with different numerical apertures yielding a spatial resolution of 164 nm. The holograms were recorded in a high resolution photoresist and digitized with an atomic force microscope. A detailed wavelet decomposition and correlation method was developed to assess the spatial resolution achieved in the numerical reconstruction of the holograms.
“…The 27 cm long capillary discharge plasma columns used in this experiment generates a laser beam that has a spatial coherence length of approximately 570μm measured at the experiment chamber located at 1.7 m from the exit of the laser. The spatial coherence length can be further increased using a longer plasma [17,18] IL was implemented by illuminating a flat mirror in the Lloyd's configuration with the EUV laser output. In this configuration, part of the laser beam impinges on the mirror at an incidence angle θ and is reflected to interfere with the remaining un-deflected portion of the beam, as illustrated in Fig.…”
Arrays of nanodots were directly patterned by interferometric lithography using a bright table-top 46.9 nm laser. Multiple exposures with a Lloyd's mirror interferometer allowed to print arrays of 60 nm FWHM features. This laser-based extreme ultraviolet interferometric technique makes possible to print different nanoscale patterns using a compact tabletop set up.
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