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The final result is the flux of the target as a function of wavelength.
Fig. 1 Network deployment of a target and three different neighbors Fig. 2 The SPEB of target as a function of the information angle of mobile anchor.
Figure 3 displays the temporal profile of ion dose on the target as a function of gas pressure and collision power parameter.
The bidirectional reflectance distribution function (BRDF) gives the reflectance of a target as a function of illumination geometry and viewing geometry, hence carries information about the anisotropy of the surface.
The HRRP is the amplitude of radar-returned echoes from target as a function of range cell, which represents the distribution of projection of target radar scattering centers along the radar line of sight.
The constant parameters are the same as Fig. 2 Open image in new window Fig. 5 Temporal variations of ion incident angle on the target as a function of ion collision parameters P g and β.
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Figure 13 (a) Misidentification of the seven targets as a function of the pixel resolution.
Figure 11 Misidentification of the four targets as a function of the pixel resolution.
Figure 9 Ability to detect and identify targets as a function of resolution and coverage rate (Nm/h: nautical mile per hour) for the best sidescan and synthetic aperture sonars.
Open image in new window Fig. 9 The random drift as a function of the deterministic drift targeted in each period Open image in new window Fig. 10 The volatility targeted as a function of the mean return targeted in each period.
The model enables rapid parametric analysis of magnetic targeting as a function of key variables including the size of the carrier particle, the properties and volume fraction of the embedded magnetic nanoparticles, the properties of the magnet, the microvessel, the hematocrit of the blood and its flow rate.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com