2008
DOI: 10.1109/lsp.2007.913588
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Frequency implementation of the Euler-Lagrange equations for variational image registration

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Cited by 12 publications
(6 citation statements)
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“…As stated in [15], this strategy allows for an efficient implementation, which runs twice faster than most state-ofart approaches [17]. To avoid too high values of the step (learning parameter), every time the derivative direction changes abruptly, the optimizer assumes that a local maximum or minimum has been passed by and reacts halving the size of the step.…”
Section: Image Registration Proceduresmentioning
confidence: 99%
“…As stated in [15], this strategy allows for an efficient implementation, which runs twice faster than most state-ofart approaches [17]. To avoid too high values of the step (learning parameter), every time the derivative direction changes abruptly, the optimizer assumes that a local maximum or minimum has been passed by and reacts halving the size of the step.…”
Section: Image Registration Proceduresmentioning
confidence: 99%
“…is the 3D Fourier transform of the so-called external forces field, ( ) f x (please refer to Appendix A, Eqs. (A.1)-(A.2) for a definition of this field), and A  is a diagonal 3×3 matrix whose elements are scalar functions which implement the spatial derivatives in the frequency domain, 22 allowing for their computation by means of products:…”
Section: Methodsmentioning
confidence: 99%
“…Equation (5) provides a stable implementation for the computation of a numerical solution for the displacement field, and in a more efficient way than existing approaches if the 3D fast Fourier transform (FFT) is used. 22 In order to solve (5) in its current state (i.e., formulated in the frequency domain), a timemarching scheme can be employed, yielding the following equation:…”
Section: Methodsmentioning
confidence: 99%
“…The second registration step is based on a variational approach which has been formulated in the frequency domain [35,36], and also implemented in the frequency domain [37] providing a fast and efficient registration method.…”
Section: Intensity-based Registrationmentioning
confidence: 99%
“…where ξ ∈ N is the iteration index, l = {1, 2} in this 2D problem, H(ω) is a low pass filter in the frequency domain andf (ω) = (f 1 (ω),f 2 (ω)) is the Fourier transform of the external forces field. For further details, please refer to [35,36].…”
Section: Intensity-based Registrationmentioning
confidence: 99%