Modern Characterization of Electromagnetic Systems and its Associated Metrology. Magdalena Salazar-Palma

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Название Modern Characterization of Electromagnetic Systems and its Associated Metrology
Автор произведения Magdalena Salazar-Palma
Жанр Физика
Серия
Издательство Физика
Год выпуска 0
isbn 9781119076537



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are also unitary matrices which means that [U]*[U] =[I] and [V]*[V] = [I]. In other words, they are orthogonal where * denoted complex conjugate transpose. The σ’s are the singular values which also so happen to be the square roots of the eigenvalues of both [A][A]* and [A]*[A]. We are not totally finished however because [U] and [V] are not square matrices. While (1.19) is the diagonalization of [A], the matrix equation is technically not valid since we cannot multiply these rectangular matrices of different sizes. To make them square we will need nr more v’s and mr more u’s. We can get these required u’s and v’s from the nullspace N(A) and the left nullspace N(A*). Once the new u’s and v’s are added, the matrices are square and [A] will still equal [U][][V]T. The true SVD of [A] will now be

      The new singular value matrix [∑] is the same matrix as the old r × r matrix but with m – r new rows of zero and n – r columns of new zero added. The theory of total least squares (TLS) heavily utilizes the SVD as will be seen in the next section.

Schematic illustration of the discretization of the letter X on a 20 cross 20 grid.
16.9798798959208 4.57981833410903 3.55675452579199 2.11591593148044 1.74248432449203 1.43326538670857 0.700598651862344 8.40316310453450×10–16 2.67120960711993×10–16 1.98439889201509×10–16 1.14953653060279×10–16 4.74795444425376×10–17 1.98894713470634×10–17 1.64625309682086×10–18 5.03269559457945×10–32 1.17624286081108×10–32 4.98861204114981e×10–33 4.16133005156854×10–49 1.35279056788548×10–80 1.24082758075064×10–112

      To illustrate the point, we now perform a rank‐1 approximation for the matrix and we will require

      (1.22)equation

      The advantage of the SVD is that an error in the reconstruction of the image can be predicted without actually knowing the actual solution. This is accomplished by looking at the second largest singular value. The result is not good and we did not expect it to be. So now if we perform a Rank‐2 reconstruction for the image, it will be given by

      (1.23)equation

Schematic illustration of a grid describing the rank-1 approximation of the image X.