Abstract

We consider a square matrix \(A\) with real or complex elements. We denote \(\mathbb{K}=\mathbb{R}\) or \(\mathbb{C}\) and we are interested in computing \(\lambda \in \mathbb{K}\) such that there exists \(v\in \mathbb{K}^{n}\) such that \(Av-\lambda v=0\), i.e. we are interested in computing the eigenpairs (eigenvalue +eigenvector) of the matrix \(A\). In this sense, we consider the nonlinear system of equations \(F(x) =0\), where \(F(x) =\)\({Av-\lambda v}\choose{Gv-1}\), where \(G\) is a convenient mapping.

In order to solve this system we consider the Newton and the Chebyshev methods, and at each iteration step, the order 1 derivative is approximated by the Schultz method; such an approach does not require the solving of a linear system at each step.

We conditions for local convergence and errors evaluations for the r-convergence order.

Authors

Keywords

eigenvalue and eigenvector of square matrix; eigenpair; Newton method; Chebyshev method; Schultz method; local convergence theorem; error estimation; linear systems solving-free iterative methods; r-convergence order.

Cite this paper as:

I. Păvăloiu, E. Cătinaş, Remarks on some Newton and Chebyshev-type methods for approximation eigenvalues and eigenvectors of matrices, Comput. Sci. J. Mold., 7 (1999) no. 1, pp. 3-15.

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Remarks on Some Newton and Chebyshev-type Methods for Approximating the Eigenvalues and Eigenvectors of Matrices

I. Pǎvǎloiu and E. Cǎtinaş

1 Introduction

It is well known that the Newton and the Chebyshev methods for nonlinear systems require the solving of a linear system at each iteration step. In this note we shall study two modified methods which avoid the solving of the linear systems by using the Schultz method to approximate the inverses of the Fréchet derivatives. At the same time we shall use the particularities of the nonlinear systems arising from eigenproblems, since the Fréchet derivatives of order higher than two are the null multilinear operators. Some numerical examples will be provided in the end of this note.

Denote V=𝕂n and let A=(ai⁢j)∈𝕂n×n, where 𝕂=ℝ or ℂ. We recall that the scalar λ∈𝕂 is an eigenvalue of A if there exists v∈V, v≠0 such that

A⁢v−λ⁢v=0⁢. (1)

The vector v is called an eigenvector corresponding to the eigenvalue λ. Since for an eigenvalue λ the eigenpair (v,λ) is not uniquely determined, it is necessary to impose a supplementary condition. Different Newton-type methods were studied in the papers [1]-[4], [6], [9]-[11], [16]-[18], [20], [21]. It is worth mentioning that the Rayleigh quotient method is equivalent with a certain Newton method (”the scaled Newton method” [10]).

We shall consider a ”norming” function G:V→𝕂, G⁢(0)≠1 and besides (1) the equation

G⁢(v)−1=0⁢.

The function G may be chosen in different ways (see [16] and [3]):

I ⁢G⁢(v) =12⁢‖v‖22⁢,
II ⁢G⁢(v) =12⁢n⁢‖v‖22⁢.

We shall consider in the theoretical results hereafter the choice II.

Let X=V×𝕂(=𝕂n+1) and for x=(vλ)∈X take

‖x‖=max⁡{‖v‖,|λ|}⁢,

where the norm on V is one of the usual norms.

Consider the system

F⁢(x)=0(here⁢ 0∈𝕂n+1) (2)

with the mapping F given by

F⁢(x)=(A⁢v−λ⁢vG⁢v−1)⁢,x=(vλ)∈X⁢.

Denoting v=(x(1),x(2),…,x(n)) and λ=x(n+1) then the system (2) can be written explicitly

F1⁢(x) =(a11−x(n+1))⁢x(1)+a12⁢x(2)+⋯+a1⁢n⁢x(n)=0
⋮
Fn⁢(x) =an⁢1⁢x(1)+an⁢2⁢x(2)+⋯+(an⁢n−x(n+1))⁢x(n)=0
Fn+1⁢(x) =12⁢n⁢(x(1))2+12⁢n⁢(x(2))2+⋯+12⁢n⁢(x(n))2−1=0.

It can be easily seen that the Fréchet derivatives of F are given by the following relations:

F′⁢(x0)⁢h=(A−λ0⁢I−v01n⁢v0t0)⁢(uα)
F′′⁢(x0)⁢h⁢k=(−α⁢w−β⁢u1n⁢wt⁢u)

for all x0=(v0λ0), h=(uα), k=(wβ)∈X.

Since the Fréchet derivative of order 2 does not depend on x0 it is obvious that the derivatives of order higher than 2 an the null multilinear operators, so for any fixed x0∈X

F⁢(x)=F⁢(x0)+F′⁢(x0)⁢(x−x0)+12⁢F′′⁢(x0)⁢(x−x0)2∀x∈X. (3)

It is easy to verify that when we use the max norm on V and G is given by choice II

‖F′′⁢(x)‖∞=2⁢,∀x∈X⁢.

The following result concerning the invertibility of F′ at a solution hold.

Lemma 1

Let x∗=(v∗,λ∗) be an eigenpair of a given matrix A∈𝕂n×n. Then the eigenvalue λ∗ is simple if and only if the Jacobian F′⁢(x∗) is nonsingular.

Proof. The corresponding result for the choice I of G was proved by Yamamoto [21], for which

F′⁢(x0)=(A−λ0⁢I−v0−v0t0)⁢.

The stated affirmation follows immediately observing that the two matrices differ by a nonzero factor in the last row. □

2 Some Newton and Chebyshev-type methods

We shall study first the convergence of the sequences (xk)k≥0⊂X and (Γk)⊂ℒ⁢(X)(=𝕂(n+1)×(n+1)) generated by the following Newton-type process applied to the nonlinear system (2), initially proposed by Ul’m [19] and studied by Diaconu and Pǎvǎloiu [7]:

xk+1 =xk−Γk⁢F⁢(xk) (4)
Γk+1 =Γk⁢(2⁢I−F′⁢(xk+1)⁢Γk), ⁢k=0,1,..

x0∈X and Γ0∈ℒ⁢(X) being given.

We shall need the following preliminary result.

Lemma 2

[4] If the sequences (δk)k≥0 and (ρk)k≥0 of real positive numbers satisfy

δk+1 ≤(δk+2⁢ρk)2 (5)
ρk+1 ≤ρk⁢δk+ρk2,k=0,1,..

with max⁡(δ0,ρ0)≤19⁢d for some d∈(0,1), then the following inequalities are true:

max⁡{δk,ρk}≤19⁢d2k⁢, ⁢k=0,1,..

Denoting B¯r⁢(x0)={x∈X:‖x−x0‖≤r} we can state the following result.

Theorem 3

Assume that the operator F and the elements x0∈X, Γ0∈ℒ⁢(X) and r>0 satisfy the following conditions

a)

there exists F′⁢(x0)−1 and ‖F′⁢(x0)−1‖≤β0;

b)

q=2⁢β0⁢r<1;

c)

denoting δ0=‖I−F′⁢(x0)⁢Γ0‖, ρ0=10081⁢β2⁢‖F⁢(x0)‖ and β=β01−q, suppose

max⁡{δ0,ρ0}≤19⁢d⁢ for some ⁢d∈(0,1);
d)

d10⁢(1−q)≤r.

Then the sequences (xk)k≥0, (Γk)k≥0 generated by (4) converge and (xk)k≥0⊂B¯r⁢(x0). Denoting x∗=limk→∞xk and Γ∗=limk→∞Γk, then x∗ is a solution of the nonlinear system (2) and Γ∗=F′⁢(x∗)−1. Moreover, the following estimations hold:

‖x∗−xk‖ ≤d2k10⁢β⁢(1−d2k)⁢, ⁢k=0,1,..
‖Γ∗−Γk‖ ≤d2k3⁢(1−d2k)⁢, ⁢k=0,1,...

Proof. It can be easily seen that in our hypotheses the derivatives F′⁢(x) are invertible for all x∈B¯r⁢(x0).

Using the inequality

‖I−F′⁢(x0)−1⁢F′⁢(x)‖≤2⁢β0⁢r=q<1⁢,

and applying the Banach lemma we get

‖F′⁢(x)−1‖≤β01−q=β⁢.

Taking into account b) and c) it follows that

‖Γ0‖ ≤‖F′⁢(x0)−1‖⁢(‖F′⁢(x0)⁢Γ0−I‖+1)
≤β0⁢(1+δ0)≤109⁢β0≤109⁢β⁢,

which together with relation (4) imply

‖x1−x0‖≤‖Γ0‖⁢‖F⁢(x0)‖<d10⁢β⁢(1−d)≤r⁢,

i.e. x1∈B¯r⁢(x0).

Denote ρ1=10081⁢β2⁢‖F⁢(x1)‖ and δ1=‖I−F′⁢(x1)⁢Γ1‖. If we take x=x1 in (3) then an elementary reasoning shows that

ρ1 ≤ρ02+δ0⁢ρ0
δ1 ≤(δ0+2⁢ρ0)2⁢,

whence, by lemma 2 it follows that max⁡{ρ1,δ1}≤19⁢d2.

It can be easily proved by induction that the following relations hold for k=0,1,..

  • •

    xk∈B¯r⁢(x0);

  • •

    δk:=‖I−F′⁢(xk)⁢Γk‖≤19⁢d2k;

  • •

    ρk:=10081⁢β2⁢‖F⁢(xk)‖≤19⁢d2k;

  • •

    ‖xk+1−xk‖≤d2k10⁢β.

From the above properties it results that the sequence (xk)k≥0 is Cauchy and therefore there exists x∗∈B¯r⁢(x0) such that x∗=limk→∞xk. The last inequality above implies that for all m∈ ℕ

‖xk+m−xk‖≤∑i=kk+m−1‖xi+1−xi‖≤d2k10⁢β⁢(1−d2k)⁢,k=0,1,..

which leads to the first estimation from the enounce.

The convergence of the sequence (Γk)k≥0 is infered from the inequalities

‖Γk+1−Γk‖ =‖I−F′⁢(xk+1)⁢Γk‖
≤‖I−F′⁢(xk)⁢Γk‖+‖F′⁢(xk)−F′⁢(xk+1)‖⁢‖Γk‖
≤δk+2⁢‖Γk‖2⁢‖F⁢(xk)‖
≤δk+2ρk≤13d2k, k=0,1,..,

which lead to the second stated estimation. □

As we can see, the Newton-type method (4) has the r-convergence order at least 2. The conditions from the above theorem assure that the eigenvalue λ∗=limk→∞xk(n+1) is simple, according to lemma 1.

We shall consider now the following sequences given by the Chebyshev-type method, initially proposed by Diaconu [8]

Ck =Bk⁢(2⁢I−F′⁢(xk)⁢Bk)
xk+1 =xk−Ck⁢F⁢(xk)−12⁢Ck⁢F′′⁢(xk)⁢(Ck⁢F⁢(xk))2 (6)
Bk+1 =Bk⁢[3⁢I−3⁢F′⁢(xk+1)⁢Bk+(F′⁢(xk+1)⁢Bk)2],k=0,1,..,

where x0∈X and B0∈ℒ⁢(X) are given.

For the study of the above method we need the following auxilliary result.

Lemma 4

[3] If the sequences of real positive numbers (δk)k≥0 and (ρk)k≥0 satisfy

δk+1 ≤(δk+2⁢ρk+2⁢ρk2)3
ρk+1 ≤ρkδk2+ρk2δk2+2ρk3+ρk4,k=0,1,..,

where max⁡{δ0,ρ0}≤17⁢d for some 0<d<1, then the following relation holds:

max⁡{δk,ρk}≤17⁢d3k⁢,k=0,1,...

As for the previous method, we shall consider the elements x0∈X and the ball B¯r⁢(x0).

Theorem 5

Assume that the operator F and the elements x0∈X, B0∈ℒ⁢(X) satisfy:

a)

there exists F′⁢(x0)−1 and ‖F′⁢(x0)−1‖≤β0;

b)

q=2⁢β0⁢r<1;

c)

denoting β=β01−q, a=6449⁢β, δ0=‖I−F′⁢(x0)⁢B0‖ and ρ0=a2⁢‖F⁢(x0)‖, suppose

max⁡{δ0,ρ0}≤17⁢dfor some ⁢d∈(0,1);
d)

8⁢d49⁢a⁢(1−d2)≤r.

Then the sequences (xk)k≥0, (Bk)k≥0, (Ck)k≥0 converge and (xk)k≥0⊂B¯r⁢(x0). Denoting x∗=limxk,B∗=limBk,C∗=limCk, then F⁢(x∗)=0 and B∗=C∗=F′⁢(x∗)−1. Moreover, the following estimations hold:

‖x∗−xk‖ ≤8⁢d3k49⁢a⁢(1−d2⋅3k);
‖F′⁢(x∗)−1−Bk‖ ≤1656⁢a⁢d3k2401⁢(1−d2⋅3k)⁢,k=0,1,...

Proof. From a), b) and the Banach lemma it easily follows that for any x∈B¯r⁢(x0) the Jacobian of Fis invertible and

‖F′⁢(x)−1‖≤β01−q=β⁢.

For the norms of B0 and C0, taking into account the hypotheses, we get

‖B0‖ ≤‖B0−F′⁢(x0)−1‖+‖F′⁢(x0)−1‖
≤‖F′⁢(x0)−1‖⁢(1+‖I−F′⁢(x0)⁢B0‖)
≤β0⁢(1+δ0)≤87⁢β0<87⁢β

and

‖C0‖ ≤‖B0‖+‖I−F′⁢(x0)⁢B0‖⋅‖B0‖
≤‖B0‖⁢(1+δ0)≤6449⁢β=a⁢,

so max⁡{‖B0‖,‖C0‖}≤a.

From (6) we have that

‖x1−x0‖ ≤a⁢(1+a2⁢‖F⁢(x0)‖)⁢‖F⁢(x0)‖
≤a⁢(1+ρ0)⁢‖F⁢(x0)‖
<87⁢a2⁢‖F⁢(x0)‖
≤ρ0a2⋅87⁢a=8⁢d49⁢a⁢,

whence, taking into account d) it follows that x1∈B¯r⁢(x0).

Further, by the identity (3) and by (6) one obtains

‖F⁢(x1)‖ ≤‖I−F′⁢(x0)⁢C0‖⁢(1+12⁢‖F′′⁢(x0)‖⁢‖C0‖2⁢‖F′⁢(x0)‖)⁢‖F⁢(x0)‖+
+12⁢‖F′′⁢(x0)‖2⁢‖C0‖4⁢‖F⁢(x0)‖3+18⁢‖F′′⁢(x0)‖3⁢‖C0‖6⁢‖F⁢(x0)‖4⁢,

whence

a2⁢‖F⁢(x1)‖ ≤a2⁢‖F⁢(x0)‖⋅‖I−F′⁢(x0)⁢C0‖⁢(1+a2⁢‖F⁢(x0)‖)+
+2⁢(a2⁢‖F⁢(x0)‖)3+(a2⁢‖F⁢(x0)‖)4⁢.

Denoting ρ1=a2⁢‖F⁢(x1)‖ and taking into account the inequality

‖I−F′⁢(x0)⁢C0‖≤‖I−F′⁢(x0)⁢B0‖2=δ02

it follows

ρ1≤ρ0⁢δ02+ρ02⁢δ02+2⁢ρ03+ρ04⁢.

From the third relation of (6) we get

‖I−F′⁢(x1)⁢B1‖ =‖(I−F′⁢(x1)⁢B0)3‖
≤‖I−F′⁢(x1)⁢B0‖3
≤(‖I−F′⁢(x0)⁢B0‖+2⁢‖B0‖⁢‖x1−x0‖)3
≤(δ0+2⁢ρ0+2⁢ρ02)3⁢,

i.e.,

δ1≤(δ0+2⁢ρ0+2⁢ρ02)3⁢.

By lemma 4 the above inequalities imply that max⁡{ρ1,δ1} ≤17⁢d3.

Assume now that the following properties hold:

  • •

    x0,x1,..,xk∈B¯r(x0);

  • •

    ρi:=a2⁢‖F⁢(xi)‖≤17⁢d3i and δi:=∥I−F′(xi)Bi∥≤17d3i,i=0,..,k.

It easily follows that max⁡{‖Bk‖,‖Ck‖}≤a and

‖xk+1−xk‖ ≤a⁢(1+a2⁢‖F⁢(xk)‖)⁢‖F⁢(xk)‖
≤a⁢(1+ρk)⁢‖F⁢(xk)‖
≤8⁢ρk7⁢a≤8⁢d349⁢a⁢.

From the above formula it follows that xk+1∈B¯r⁢(x0):

‖xk+1−x0‖≤8⁢d49⁢a⁢∑i=0kd3i−1≤8⁢d49⁢a⁢(1−d2)≤r⁢.

Denoting ρk+1=a2⁢‖F⁢(xk+1)‖ and δk+1=‖I−F′⁢(xk+1)⁢Bk+1‖, the following relations are obtained in the same manner as for ρ1 and δ1:

ρk+1 ≤ρk⁢δk2+ρk2⁢δk2+2⁢ρk3+ρk4
δk+1 ≤(δk+2⁢ρk+2⁢ρk2)3⁢,

whence, by lemma 4, we get that max⁡{ρk+1,δk+1}≤17⁢d3k+1 and the induction is proved.

We will show now that (xk)k≥0 is a Cauchy sequence. Indeed,

‖xk+m−xk‖≤8⁢d3k49⁢a⁢∑i=kk+m−1d3i≤8⁢d3k49⁢a⁢(1−d2⋅3k)⁢,

for all k,m∈ ℕ, which implies that (xk)k≥0 converges. Denoting x∗=limk→∞xk we obtain

‖x∗−xk‖≤8⁢d3k49⁢a⁢(1−d2⋅3k)⁢, ⁢k=0,1,...

The convergence of (Bk)k≥0 is obtained from the third relation of (6):

‖Bk+1−Bk‖ ≤‖Bk‖⋅‖2⁢I−F′⁢(xk+1)⁢Bk‖⋅‖I−F′⁢(xk+1)⁢Bk‖
≤a⁢(1+δk+2⁢ρk+2⁢ρk2)⁢(ρk+2⁢ρk+2⁢ρk2)
≤a⁢16562401⁢d3k⁢.

Denoting B∗=limBk it easily follows that B∗=F′⁢(x∗)−1 and that

‖F′⁢(x∗)−1−Bk‖≤1656⁢a⁢d3k2401⁢(1−d2⋅3k)⁢,k=0,1,...

The proof is completed. □

3 Numerical examples

We shall consider two test matrices111These matrices are available from MatrixMarket at the following address: http://math.nist.gov/MatrixMarket/. in order to study the behavior of the considered methods. The programs were written in Matlab222MATLAB is a registered trademark of the MathWorks, Inc. and were run on a PC.

Pores1 matrix. This matrix arise from oil reservoir simulation. It is real, unsymmetric, of dimension 30 and has 20 real eigenvalues. We have chosen to study the largest eigenvalue λ∗=−1.8363⁢e+1. The initial approximation was taken λ0=λ∗+0.5; for the initial vector v0 we perturbed the solution v∗ (computed by Matlab and then properly scaled to fulfill the norming equation) with random vectors having the components uniformly distributed on (-ε,ε), ε=0.2. The following results are typical for the runs made (we have considered here the same vector ε for the four initial approximations).

Choice I Choice II
k ‖x∗−xk‖ ‖F⁢(xk)‖ ‖x∗−xk‖ ‖F⁢(xk)‖
0 7.8042e-01 5.5828e+06 7.8042e-01 5.5828e+06
1 1.4111e-01 3.9355e-01 2.3565e-02 3.0227e-01
2 1.8788e-02 5.1300e-02 4.6685e-05 9.6691e-04
3 3.7663e-04 6.3248e-04 5.7799e-10 9.0156e-09
4 1.4161e-07 2.1373e-07
5 4.5991e-10 5.0482e-10

Table 1. Newton-type method for Pores1.

Choice I Choice II
k ‖x∗−xk‖ ‖F⁢(xk)‖ ‖x∗−xk‖ ‖F⁢(xk)‖
0 7.8042e-01 5.5828e+06 7.8042e-01 5.5828e+06
1 5.6679e-02 1.0406e-01 1.5461e-03 1.2236e-02
2 2.8973e-06 4.0907e-06 5.6407e-10 5.5530e-09
3 4.5959e-10 6.5014e-10

Table 2. Chebyshev-type method for Pores1.

Fidap002 matrix. This real symmetric matrix of dimension n=441 arise from finite element modeling. Its eigenvalues are all simple and range from −7⋅108 to 3⋅106. We have chosen to study the smallest eigenvalue, which is well separated. The initial approximation was taken λ0=λ∗+103=−6.9996⋅108+1000; for the initial vector v0 we perturbed the solution v∗ with random vectors having the components uniformly distributed on (-ε,ε), ε=0.1. The following results are typical for the runs made (we have considered a common vector ε).

Choice I Choice II
k ‖x∗−xk‖ ‖F⁢(xk)‖ ‖x∗−xk‖ ‖F⁢(xk)‖
0 1.0000e+3 8.5068e+8 1.0000e+3 8.5068e+8
1 2.3611e+2 1.5730e+3 3.3415e+0 1.2195e+3
2 2.5528e+2 8.8353e+2 8.4714e-3 1.0600e+0
3 4.3758e+1 8.2481e+1 5.9605e-7 4.1725e-6
4 1.3141e+0 2.0458e+0
5 9.9051e-4 1.4631e-3
6 5.9605e-7 1.0662e-7

Table 3. Newton-type method for Fidap002.

Choice I Choice II
k ‖x∗−xk‖ ‖F⁢(xk)‖ ‖x∗−xk‖ ‖F⁢(xk)‖
0 1.0000e+3 8.5068e+8 1.0000e+3 8.5068e+8
1 3.9756e+2 9.4690e+2 8.5282e-1 2.5509e+1
2 4.6275e-1 6.5442e-1 7.1526e-7 5.0390e-6
3 4.7684e-7 3.1597e-7

Table 4. Chebyshev-type method for Fidap002.

If ε was increased to 0.15 then the Newton-type method with choice I has not converged for some of the initial approximations, even if we took λ∗ for λ0. The Newton-type method with choice II and the Chebyshev-type method converged as above. The explanation seem to reside in the fact that the eigenvector v∗ has a larger norm with choice II than with choice I, the relative error of v∗+ε with the second choice being much smaller than of v∗+ε with the first choice.

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  • [21] T. Yamamoto, Error Bounds for Computed Eigenvalues and Eigenvectors, Numer. Math. 34 (1980), pp. 189-199.

”T. Popoviciu” Institute of Numerical Analysis

P.O. Box 68

3400 Cluj-Napoca 1

Romania

e-mail: pavaloiu@ictp.math.ubbcluj.ro

ecatinas@ictp.math.ubbcluj.ro

1999

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