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2. ρ(G)= ρ(J) ,
                                3. the Gauss–Seidel method converges if and only if the Jacobi method
                                   converges; moreover, in case of convergence, the Gauss–Seidel method
                                   converges twice as fast as the Jacobi method;
                                4. the spectrum of J is even: Sp J = − Sp J.
                                Proof        2                    9.4. The Tridiagonal Case  157
                                Formula (1) comes from Lemma 9.4.2. The spectrum of G is thus formed
                              of λ = 0 (which is of multiplicity [(n +1)/2] at least) and of squares of the
                              eigenvalues of J, which proves 2). Point 3 follows immediately. Finally, if
                                                                                  n
                                                                 2
                              µ ∈ Sp J,then P J (µ) = 0, and also P G (µ ) = 0, so that (−µ) P J (−µ)= 0.
                              Finally, either P J (−µ) = 0, or µ =0= −µ,inwhichcase P J (−µ)also
                              vanishes.
                                In fact, the comparison given in point 3 of the proposition holds under
                              various assumptions. For example (see Exercises 3 and 8), it holds true
                              when D is positive and E, F are nonnegative.
                                We go back to the SOR, with an additional hypothesis: The spectrum of
                              J is real, and the Jacobi method converges. This property is satisfied, for
                              instance, when A is Hermitian positive definite, since Theorem 9.3.1 and
                              Proposition 9.4.1 ensure the convergence of the Jacobi method, and since
                              J is similar to the Hermitian matrix D −1/2 (E + F)D −1/2 .
                                We also select a real ω,that is, ω ∈ (0, 2), taking into account Proposition
                              9.2.1. The spectrum of J is thus formed of the eigenvalues
                                          −λ r < ··· < −λ 1 ≤ λ 1 < ··· <λ r = ρ(J) < 1,

                              from Proposition 9.4.1. This notation does not mean that n be even: If n is
                              odd, λ 1 = 0. Aside from the zero eigenvalue, which does not enter into the
                              computation of the spectral radius, the eigenvalues of L ω are the squares
                              of the roots of
                                                      2
                                                     µ + ω − 1= µωλ a ,                   (9.3)
                              for 1 ≤ a ≤ r. Indeed, taking −λ a instead of λ a furnishes the sames squares.
                                                    2 2
                                Let us define ∆(λ):= ω λ +4(1−ω), the discriminant of (9.3). If ∆(λ a )
                              is negative, both roots of (9.3) are complex conjugate, hence have modulus
                                   1/2
                              |ω −1|  .The case λ = 0 furnishes the same modulus. If that discriminant
                              is strictly positive, the roots are real and of distinct modulus. One of them,
                                                    2
                              denoted by µ a ,satisfies µ > |ω − 1|, the other one satisfying the opposite
                                                    a
                              inequality.
                                From Proposition 9.2.1, ρ(L ω ) is thus equal to one of the following:
                                 •|ω − 1|,if ∆(λ a ) ≤ 0 for every a,that is, if ∆(ρ(J)) ≤ 0;
                                                      2
                                 • the maximum of the µ ’s defined above, otherwise.
                                                      a
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