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Fig. 5 Left: Cerenkov production range simulated by [32], considering only the contribution of the primary β particles (1) in Fig. 3. Right: simulated spread in the Cerenkov light production as a function of the β-particle endpoint energy, for a few radionuclides (both with permission by [32]).

Right: Simulated over measured Cerenkov count rate with different acquisition settings (top) and as a function of activity, for two combinations of acquisition settings (bottom); both figures were adapted from [125].

Right: Simulated evolution of the normalized PL spectra for ratio's of excitation power identical to that of Figure 2. Inset: Comparison of experimental and simulated peak wavelengths for the different excitation powers.

(Left) Simulated histories of the slider displacement δ (top), the slider velocity normalized by the load point velocity V/V∗ (middle), the state Φ and the shear stress τ (bottom) for the the Nagata RSF, where Φ∗ and τ∗ are reference values from steady-state sliding at V∗. (Right) Simulated histories for 2 years prior to instability at t=0.

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Shown are the results for January (left column) and April (right column), simulated by MUAM.

Right: plasticity simulated with the centroidchasing algorithm, crowns are displaced into less contested spaces.

(Right panel) Simulated spatial distribution of Smad2 activation in a one-dimensional column of cells from 3.5 to 5 hpf in response to Nodal production from a source that extends from L = 0 to 25 µm.

Continuous lines on the right are simulated flash response profiles of mixed S/M cones at four retinal latitudes (1 4, from dorsalmost to ventralmost; inset in lower graph) and pure S cones, based on recently published models (Daniele et al., 2011 ; Wang et al., 2011 ; see 'Materials and methods').

As shown in Figure 3 (Right), the simulated ERK activation peaks at about 7 min and decays within 25 min, which is consistent with the observation that the amount of phosphorylated ERK-1/2 reaches maximum value at 5-10 min after administration of VEGF and decreases back to the control level 30 min afterward [ 58].

T2-weighted, fat-saturated axial MR image shows protrusion of the implant shell through a focally weakened part of the fibrous capsule at medial aspect of right breast, simulating a rat tail (arrow)   3.

This is a pretty fussy bit of technology, as there's only so much depth that can be simulated right now, and there's definitely a "sweet spot" for viewing distance and angle.

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