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Results are given as optical density (OD).
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The IOD of each image (region) is given as the average of optical densities of each molecule (pixel) within the region.
To summarize, the procedure for a numerical solution of the cDA is given as For a given optical parameters μ a and μ s, compute the asymptotic parameter ε using Eq. (50) and scaled optical parameters α and σ using Eq. (6).
According to the Burstein-Moss effect, the broadening of the optical bandgap is given as follows: Δ E g = h 2 2 m vc ∗ 3 π 2 n 2 / 3, (4).
The vector potential of optical field is given as follows: A_{text{s}} (z,t) = (B_{text{s}} /k_{text{s}} )[hat{e}_{x} cos (k_{text{s}} z - w_{text{s}} t + varphi_{text{s}} (t)) - hat{e}_{y} sin (k_{text{s}} z - w_{text{s}} t + varphi_{text{s}} (t))], (2 where, k s is optical wave number, B s is the field strength and φ s(t) is initial of optical phase, which is usually looked as zero.
The immunostaining intensities (optical density) are given as means ± SD.
These optical properties are given as those of breast in the NIR wavelength range by referring a literature [ 6].
After passing through the optical channel ho(t), the optical signal y(t) received is given as follows: y t = X t ∗ h o t + n o t, (3).
The results are given as the median ± interquartile range of the optical density values (450 nm) of each group.
Values are given as mean ± SEM pg/ml × 25 µg × 150 min for sAPPβ, optical density (OD) for APP and ng/mg protein for serotonin.
A complete description of the receiver function is given as the convolution of this pinhole function with the incoherent-PSF of the optical system.
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