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For these calculations a Gaussian pump light beam with a wavelength of 1064 nm was assumed. This beam had a beam diameter of 40 mm inside the cell 80 mm behind the entrance window. Such a beam would follow, for example, by focusing a 2-mm waist diameter with a focal length of 120 mm positioned 40 mm in front of the entrance window of the cell. As SBS material, SF6 with a pressure of 20 bars was assumed. As can be seen from these calculations, all of the SBS re ection takes place in front of the waist of the focused pump light, and thus the re ected light occurs on the left side of the cell. In this case the sound wave was very highly concentrated around the focus of the beam. The calculations were done for a pump pulse energy of 41 mJ for a pulse duration of 30 ns (FWHM). As can be seen from the pump light graph, the leading edge of the pulse is needed to establish the sound wave inside the cell. This leading edge of the pump pulse transmits through the SBS cell virtually undepleted. But from a certain time on the sound wave amplitude is strong enough to re ect the light, and therefore the following pump light is depleted strongly and a strong re ected Stokes light can be obtained. This temporally onset behavior of the SBS c# upc-a reader C# UPC-A Barcode Scanner Library - Read & Scan UPC-A Using ...
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