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min w , u i w i + β 2 i w i - D i u 2 + μ 2 K u - f 2 ,

where β 0 is a penalty parameter. It is well known that the solution of ( ) converges to that of ( ) as β . In the following, we concentrate on problem ( ).

Basic algorithm

The benefit of ( ) is that while either one of the two variables u and w is fixed, minimizing the objective function with respect to the other has a closed-form formula that we willspecify below. First, for a fixed u , the first two terms in ( ) are separable with respect to w i , and thus the minimization for w is equivalent to solving

min w i w i + β 2 w i - D i u 2 , i = 1 , 2 , ... , n 2 .

It is easy to verify that the unique solutions of ( ) are

w i = max D i u - 1 β , 0 D i u D i u , i = 1 , ... , n 2 ,

where the convention 0 · ( 0 / 0 ) = 0 is followed. On the other hand, for a fixed w , ( ) is quadratic in u and the minimizer u is given by the normal equations

i D i D i + μ β K K u = i D i w i + μ β K f .

By noting the relation between D and D i and a reordering of variables, ( ) can be rewritten as

D D + μ β K K u = D w + μ β K f ,

where

w w 1 w 2 R 2 n 2 and w j ( w 1 ) j ( w n 2 ) j , j = 1 , 2 .

The normal equation ( ) can also be solved easily provided that proper boundary conditions are assumed on u . Since both the finite difference operations and the convolution are notwell-defined on the boundary of u , certain boundary assumptions are needed when solving ( ). Under the periodic boundary conditions for u , i.e. the 2D image u is treated as a periodic function in both horizontal and vertical directions, D ( 1 ) , D ( 2 ) and K are all block circulant matrices with circulant blocks; see e.g. , . Therefore, the Hessianmatrix on the left-hand side of ( ) has a block circulant structure and thus can be diagonalized by the 2D discreteFourier transform F , see e.g. . Using the convolution theorem of Fourier transforms, the solution of( ) is given by

u = F - 1 F D w + ( μ / β ) K f diag F ( D D + ( μ / β ) K K ) ,

where the division is implemented by componentwise. Since all quantities but w are constant for given β , computing u from ( ) involves merely the finite difference operation on w and two FFTs (including one inverse FFT), once the constant quantities are computed.

Since minimizing the objective function in ( ) with respect to either w or u is computationally inexpensive, we solve ( ) for a fixed β by an alternating minimization scheme given below.

Algorithm :

  • Input f , K and μ > 0 . Given β > 0 and initialize u = f .
  • While“not converged”, Do
    • Compute w according to ( ) for fixed u .
    • Compute u according to ( ) for fixed w (or equivalently w ).
  • End Do

Optimality conditions and convergence results

To present the convergence results of Algorithm "Basic Algorithm" for a fixed β , we make the following weak assumption.

Assumption 1 N ( K ) N ( D ) = { 0 } , where N ( · ) represents the null space of a matrix.

Define

M = D D + μ β K K and T = D M - 1 D .

Furthermore, we will make use of the following two index sets:

L = i : D i u * < 1 β and E = { 1 , ... , n 2 } L .

Under Assumption 1, the proposed algorithm has the following convergence properties.

Theorem 1 For any fixed β > 0 , the sequence { ( w k , u k ) } generated by Algorithm "Basic Algorithm" from any starting point ( w 0 , u 0 ) converges to a solution ( w * , u * ) of ( ). Furthermore, the sequence satisfies

  • w E k + 1 - w E * ρ ( ( T 2 ) E E ) w E k - w E * ;
  • u k + 1 - u * M ρ ( T E E ) u k - u * M ;

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Source:  OpenStax, The art of the pfug. OpenStax CNX. Jun 05, 2013 Download for free at http://cnx.org/content/col10523/1.34
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