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An IR or TH signal can influence the electron population in dark and bright levels, therefore absorption and transmission spectrum of probe field in the medium can be altered.
This ordering is consistent with the energy separations found in Table 1 and Table 2, with ΔBD being the splitting between ±2 and ±1 L, ΔU being the average distance of ±1 L to the upper levels and Δ1,2 being the separations of ±1 L to the two upper bright levels.
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This was carried out in order to pick a stable and bright level of fluorescence.
Moreover, for slightly oblate QDs, three levels fairly close in energy to each other lie several meV above the ±1 L, which are, in order of ascending separation from ±1 L, the F = 0 called 0 L dark level, the | F| = 1 called ±1 U upper bright level, and the F = 0 called 0 U upper bright level.
This procedure is repeated for the brightest levels.
For example, a gray image with 8 bits per pixel is represented by 256 intensity levels, where 0 usually corresponds to the darkest level and 255 corresponds to the brightest level.
Abeta42 staining density was identified by bright-level threshold, the level of which was maintained throughout the experiment for uniformity.
Areas with bright gray levels reflect matrix with high Ca content, whereas areas with dark gray levels indicate low Ca content.
Interior window treatments — blinds, shades, drapes — installed by occupants may further reduce the amount of available daylight, especially in the morning when exposure to bright light levels is most essential for waking the brain and triggering its daytime clock.
Three scenarios were considered: dark, dim, and bright lighting levels.
As reflections are more likely to happen outdoors, this work was concerned with simulating an outdoor environment with bright luminance levels.
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