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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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MATRICES AND VECTOR SPACESUsing the unitarity of the matrices U <strong>and</strong> V, we find thatAˆx − b = USSU † b − b = U(SS − I)U † b. (8.142)The matrix (SS − I) is diagonal <strong>and</strong> the jth element on its leading diagonal isnon-zero (<strong>and</strong> equal to −1) only when s j = 0. However, the jth element of thevector U † b is given by the scalar product (u j ) † b;ifb lies in the range of A, thisscalar product can be non-zero only if s j ≠ 0. Thus the RHS of (8.142) mustequal zero, <strong>and</strong> so ˆx given by (8.141) is a solution to the equations Ax = b. Wemay, however, add to this solution any linear combination of the N − r vectors v i ,i = r+1,r+2,...,N, that <strong>for</strong>m an orthonormal basis <strong>for</strong> the null space of A; thus,in general, there exists an infinity of solutions (although it is straight<strong>for</strong>ward toshow that (8.141) is the solution vector of shortest length). The only way in whichthe solution (8.141) can be unique is if the rank r equals N, so that the matrix Adoes not possess a null space; this only occurs if A is square <strong>and</strong> non-singular.If b does not lie in the range of A then the set of equations Ax = b doesnot have a solution. Nevertheless, the vector (8.141) provides the closest possible‘solution’ in a least-squares sense. In other words, although the vector (8.141)does not exactly solve Ax = b, it is the vector that minimises the residualɛ = |Ax − b|,where here the vertical lines denote the absolute value of the quantity theycontain, not the determinant. This is proved as follows.Suppose we were to add some arbitrary vector x ′ to the vector ˆx in (8.141).This would result in the addition of the vector b ′ = Ax ′ to Aˆx − b; b ′ is clearly inthe range of A since any part of x ′ belonging to the null space of A contributesnothing to Ax ′ . We would then have|Aˆx − b + b ′ | = |(USSU † − I)b + b ′ |= |U[(SS − I)U † b + U † b ′ ]|= |(SS − I)U † b + U † b ′ |; (8.143)in the last line we have made use of the fact that the length of a vector is leftunchanged by the action of the unitary matrix U. Now, the jth component of thevector (SS − I)U † b will only be non-zero when s j = 0. However, the jth elementof the vector U † b ′ is given by the scalar product (u j ) † b ′ , which is non-zero only ifs j ≠0,sinceb ′ lies in the range of A. Thus, as these two terms only contribute to(8.143) <strong>for</strong> two disjoint sets of j-values, its minimum value, as x ′ is varied, occurswhen b ′ = 0; this requires x ′ = 0.◮Find the solution(s) to the set of simultaneous linear equations Ax = b, whereA is givenby (8.137) <strong>and</strong> b = (1 0 0) T .To solve the set of equations, we begin by calculating the vector given in (8.141),x = VSU † b,306

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