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<strong>Veritas</strong> <strong>et</strong> <strong>Visus</strong> <strong>Display</strong> <strong>Standard</strong> February 2009<br />
There is substantial crowding above 40% of maximum signal intensity, but note that on this 1000:1 logarithmic<br />
scale the diam<strong>et</strong>er of the round data points corresponds to a 6% shift in luminance.<br />
Figure 7: Magnified view of Figure 6 near peak luminance and signal intensity<br />
This figure enlarges the portion of Figure 6 at high peak luminance and signal intensity in order to show the<br />
significant differences b<strong>et</strong>ween the transfer functions on a magnified scale so they are easier to see. Note the<br />
significant convex curvature for the Samsung unit, which begins with a lower gamma of 2.00 b<strong>et</strong>ween 100 and 80%<br />
signal, and then steepens significantly to 2.38 b<strong>et</strong>ween 80 and 60% signal. The Sharp unit has the opposite concave<br />
curvature with its gamma shifting downward from 2.33 for 100 to 75% signal to 2.16 b<strong>et</strong>ween 75 to 50% signal.<br />
Referring back to Figure 6 the Sharp transfer function then steepens significantly b<strong>et</strong>ween 40 and 25% signal with<br />
a very high gamma of 3.25 before r<strong>et</strong>urning back to significant concave below 20% signal. These variations in the<br />
transfer functions affect not only the picture’s gray scale and contrast, but also the resulting hue and saturation for<br />
all color mixtures, because the individual R,G,B intensities simultaneously dip into different portions of the transfer<br />
function.<br />
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