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As mentioned earlier, the directional matrix ( {widehat{mathbf{Y}}}^Hleft(boldsymbol{Phi} right) ) in the VSBLKF algorithm is constructed on the uniform sampled angle grids Φ = {Φ1, ⋯, Φ G } with Φ g = (θ g, ϕ g ), g = 1, ⋯, G.
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For each trial during the actual self-motion conditions, each sampled pointing angle was converted to an estimate of perceived location.
Fig. 5 (Color online) The magnetoresistance varying as a function of sample angle at different temperatures.
The diverse display for the desired ones can be realized by exquisitely varying the incident light angle and rotating sample angle.
Generally, an orientation of polymer chain segments can be detected by a variation of the angle between the linearly polarized synchrotron light beam and the surface normal of the investigated sample (angle resolved NEXAFS spectroscopy).
Experiments were carried out at different wind speeds and various sampler angles.
The oxygen concentrations at sampling angles and the cylinder pressure were measured.
The oxidation rates of the in-cylinder soot during the late combustion phase were calculated according to the differences of spherules size distributions between two consecutive sampling angles.
Auxiliary experiments at constant irradiation energy and at different tilt sample angles were carried out to confirm the effect of the reflection of the incoming ions on the resilience of FLG.
It was defined as the square of vector sum of all sample angles divided by the sample size.
The scattering angle θ is sampled from The azimuthal angle ϕ is determined using rejection sampling from the conditional probability p = p/ p where p given by Eq. (9).
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