By Erik W Grafarend; Joseph L Awange

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**Sample text**

90, right) take the canonical left and right quadratic form. The transformations x 7 ! x as well as y 7 ! 92, right) are special versions of the left and right polar decomposition: a rotation constituted by the matrices U; V is followed 1=2 by a stretch constituted by the matrices fƒ1=2 x ; ƒy g as diagonal matrices. The forward transformations x 7 ! x and y 7 ! y are computed by the backward transformations x 7 ! x and y 7 ! y. fƒ1=2 and ƒ1=2 x y g, respectively, denote those diagonal matrices which are generated by the positive roots of the left and right eigenvalues, respectively.

Or e`1 , e`2 , respectively. Those integrals are divided by the length s of a total arc of S1r . Alternative representations of < xjy > and < e`1 je`2 > (Dirac’s notation of brackets, decomposed into “bra” and “ket”) based upon ds D rd , s D 2 r, lead us directly to the integration over S1 , the unit circle. 14 as a summary of the most essential features of the Fourier space. 14. (Fourier space): The base functions e` . /; ` 2 f L; L C 1; : : : ; 1; 0; C1; : : : ; L 1; Lg, span the Fourier space L2 Œ0; 2 : they generate a complete orthogonal (orthonormal) system of trigonometric functions.

128). 128) Proof. 58) and replace the matrix A 2 m by its canonical representation, namely eigenspace synthesis. 133) x2 0 0 0 The pair of eigensystems AA# L D Lƒ2 ; A# AR1 D R1 ƒ2 is unfortunately based upon non-symmetric matrices AA# D AGx 1 A0 Gy and A# A D Gx 1 A0 Gy A which make the left and right eigenspace analysis numerically more complex. It appears that we are forced to use the Arnoldi method rather than the more efficient Lanczos method used for symmetric matrices. In this situation we look out for 1=2 1=2 an alternative.