Exact(15)
The mean co-registration error was significantly lower after calibration than before calibration for all point sources.
Thus, the power of Equation 10 is even and the coefficients are negative; thus, for all point (x 0,y 0) in the domain R 2 Open image in new window, Equation 5 is an elliptic equation.
The mean co-registration error was significantly lower for the parameter set estimated by the calibration method than for the parameter set acquired by direct physical measurement for all point sources, as shown in Table 4.
Thus, the power of Equation 10 is even, and thus for all point (x 0,y 0) in the domain R 2 Open image in new window, Equation 5 is a hyperbolic equation.
The coefficient of A 1 x,y)C 1 x,y) < B 1 x,y)2 under the condition max{|a αβ |,|c kl |} < |b ζη | and the coefficients are positive; thus, for all point (x 0,y 0) in the domain R 2 Open image in new window, Equation 5 is a hyperbolic equation.
We initially build a m × m pairwise matching probability table S p for all point pairs in P. Given a point pair (p i, p j ) in P, its matching probability is defined by S p ( p i, p j ) = 1 C exp - φ 1 | ℳ f ( p i ) | ⋅ | ℳ f ( p j ) | n 2 - φ 2 | | p i - p j | | d max q - φ 3 s c ( ( p i, p j ), ( q ̃ i, q ̃ ) ), (14).
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Indeed, once given the forces acting on a point mass, the three laws hold for all point-masses, including those that lie within bodies.
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