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10. Approximation of Eigenvalues
                              180
                              by translating A k  → A k − α k I n . The strategies for the choice of α k are
                              described in [25]. This procedure is called Rayleigh translation. It allows
                              for a observeable improvement of the convergence of the QR method. If
                              the eigenvalues of A are simple, a suitable translation allows us to restrict
                              ourselves to the case of distinct moduli. But this trick has a nonnegligible
                              cost if A is a real matrix with a pair of complex conjugate eigenvalues,
                              since it requires a translation by a nonreal number α. As mentioned above,
                              the computations become much more costly than they are in the domain
                              of real numbers.
                                As k increases, the triangular form of A k appears first at the last row.
                              In other words, the sequence (A k ) nn converges more rapidly thanother
                              sequences (A k ) jj . When the last row is sufficiently close to (0,... , 0,λ n ),
                              the Rayleigh translation must be selected in such a way as to bring λ n−1 ,
                              instead of λ n , to the origin; and so on.
                                With a clever choice of Rayleigh translations, the QR method, when it
                              converges, is of order two for a generic matrix, and is of order three for a
                              Hermitian matrix.


                              10.3 The Jacobi Method

                              The Jacobi method allows for the approximate computation of the whole
                              spectrum of a real symmetric matrix A ∈ Sym .As in the QR method,
                                                                        n
                              one constructs a sequence of matrices, unitarily similar to A.Inparticular,
                              the round-off errors are not amplified. Each iteration is cheap (O(n)opera-
                              tions), and the convergence is quadratic when the eigenvalues are distinct.
                              It is thus a rather efficient method.




                              10.3.1 Conjugating by a Rotation Matrix
                              Let 1 ≤ p, q ≤ n be two distinct indices and θ ∈ [−π, π)anangle. We
                              denote by R p,q (θ) the rotation matrix through the angle θ in the plane
                                         p
                                                q
                              spanned by e and e . For example, if p<q,then
                                                             . .            . .
                                                                                    
                                                     I p−1   .       0      .     0
                                                                                    
                                                    ···   cos θ    ···   sin θ  ···  
                                                                                    
                                                             .              .
                                                            .              .        
                                    R = R p,q (θ):=   0     .    I q−p−1   .     0   .
                                                                                    
                                                     ···            ···          ···
                                                          − sin θ        cos θ      
                                                             .              .
                                                                                    
                                                      0      . .     0      . .  I n−q
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