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E. Cătinaş, Institutul de Calcul Tiberiu Popoviciu

Emil Cătinaş

I. Păvăloiu, Institutul de Calcul Tiberiu Popoviciu

Ion Păvăloiu

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E. Cătinaş, I. Păvăloiu, Solving polynomial operator equations of degree 2 by Steffensen-type iterations with approximate inverses, Proceedings of the International Symposium on Numerical Analysis and Approximation Theory (NAAT), May 9-11, Cluj-Napoca, 2002, R. Trimbitas (ed.), pp. 101-113. ISBN 973-610-166-5

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Solving polynomial operator equations of degree 2 by Steffensen-type iterations with approximate inverses

Emil Cătinaş and Ion Păvăloiu
Abstract

We give a semilocal convergence theorem for a Steffensen-type method when the nonlinear equation to solve is a polynomial operators of degree 2 . We consider a sequence of linear operators approximating the inverses of the first order divided difference appearing at each iteration step.
We present some numerical results applying the studied method for solving matrix eigenproblems.

Proceedings of the International Symposium
Dedicated to the 75th Anniversary of D.D. Stancu
Cluj-Napoca, May 9-11, 2002, pp. 101-103.

1 Introduction

Let XX be a Banach space over the field 𝕂(𝕂=\mathbb{K}(\mathbb{K}=\mathbb{R} or ),F:XX\mathbb{C}),F:X\rightarrow X a polynomial operator of degree 2, and consider the equation

F(x)=0.F(x)=0. (1.1)
00footnotetext: *"T. Popoviciu" Institute of Numerical Analysis, Romanian Academy.

Such equations often appear in different problems, as eigenproblems for linear operators, Chandrasekhar integral equations, etc. This motivates the study of the iterative methods for solving (1.1), by enhancing the particularities appearing in the case of the second degree polynomials. The second order derivative is a constant bilinear operator, i.e. its expression does not depend on xx. This allows the obtaining of some simpler convergence conditions, compared to the general case (see also [19, [26, [36, [10]-[13]).

The solving of a linear equation at each iteration step is an important aspect when analyzing the iterative methods. From this standpoint, the methods which approximate at each step the inverse of the Frechét derivative of the first order divided differences are important to analyze.

Given x0Xx_{0}\in X and the linear continuous operator Γ0(X)\Gamma_{0}\in\mathcal{L}(X), we shall consider the sequences (xk)k0\left(x_{k}\right)_{k\geq 0} and (Γk)k0\left(\Gamma_{k}\right)_{k\geq 0} given by

xk+1\displaystyle x_{k+1} =xkΓkF(xk)\displaystyle=x_{k}-\Gamma_{k}F\left(x_{k}\right) (1.2)
Γk+1\displaystyle\Gamma_{k+1} =Γk(2I[xk+1,G(xk+1);F]Γk),k=0,1,,\displaystyle=\Gamma_{k}\left(2I-\left[x_{k+1},G\left(x_{k+1}\right);F\right]\Gamma_{k}\right),\quad k=0,1,\ldots,

where [x,y,F][x,y,F] denotes the first order divided difference of FF on xx and yy, and G:XXG:X\rightarrow X is an operator such that equation (1.1) is equivalent to

xG(x)=0x-G(x)=0 (1.3)

As it can be seen, the above method is a Steffensen type one, with the approximation of the inverse of the first order divided difference.

We shall consider in the following the application GG given by

G(x)=xγF(x),G(x)=x-\gamma F(x), (1.4)

with some γ𝕂(γ0)\gamma\in\mathbb{K}(\gamma\neq 0) fixed.
Since FF is a polynomial of degree 2, one has

[t,u,v,w;F]=θ3,t,u,v,wX[t,u,v,w;F]=\theta_{3},\quad\forall t,u,v,w\in X (1.5)

where θ3\theta_{3} denotes the trilinear null mapping, and [t,u,v,w;F][t,u,v,w;F] denotes the divided difference of order 3 of FF on the nodes t,u,v,wXt,u,v,w\in X. It is then obvious that the second order divided difference is a constant bilinear operator (it does not depend on the nodes). Denote

D=[u,v,w;F],u,v,wXD=[u,v,w;F],\quad\forall u,v,w\in X

2 A semilocal convergence result

We shall need the following auxiliary result.
Lemma 1 Let α,β,α,β>0\alpha,\beta\in\mathbb{R},\alpha,\beta>0 and (δk)k0,(ηk)k0+\left(\delta_{k}\right)_{k\geq 0},\left(\eta_{k}\right)_{k\geq 0}\subset\mathbb{R}_{+}obeying

δk+1δkηk+αδk2\displaystyle\delta_{k+1}\leq\delta_{k}\eta_{k}+\alpha\delta_{k}^{2}
ηk+1(ηk+βδk)2,k=0,1,\displaystyle\eta_{k+1}\leq\left(\eta_{k}+\beta\delta_{k}\right)^{2},\quad k=0,1,\ldots (2.1)

If δ0,η0uq\delta_{0},\eta_{0}\leq uq for some 0<q<10<q<1 and u=min{11+α,1(1+β)2}u=\min\left\{\frac{1}{1+\alpha},\frac{1}{(1+\beta)^{2}}\right\}, then

δk,ηkuq2k\delta_{k},\eta_{k}\leq uq^{2^{k}} (2.2)

Proof. Obviously, u(1+α)1u(1+\alpha)\leq 1 and u(1+β)21u(1+\beta)^{2}\leq 1. Relations 2.2. for k=0k=0 are verified by the assumption. Supposing now that 2.2 are satisfied for k=sk=s, then by 2.1 we obtain for k=s+1k=s+1

δs+1(u2+αu2)q2s+1=u2(1+α)q2s+1uq2s+1\displaystyle\delta_{s+1}\leq\left(u^{2}+\alpha u^{2}\right)q^{2^{s+1}}=u^{2}(1+\alpha)q^{2^{s+1}}\leq uq^{2^{s+1}}
ηs+1(u+βu)q2s+1=u2(1+β)2q2s+1uq2s+1\displaystyle\eta_{s+1}\leq(u+\beta u)q^{2^{s+1}}=u^{2}(1+\beta)^{2}q^{2^{s+1}}\leq uq^{2^{s+1}}

which ends the proof.
We shall assume that

D=a\|D\|=a (2.3)

and that, given x0Xx_{0}\in X, there exists r>0r>0 such that

[x,y;F]c,x,yB¯r(x0)\|[x,y;F]\|\leq c,\quad\forall x,y\in\bar{B}_{r}\left(x_{0}\right) (2.4)

where B¯r(x0)={xX:xx0r}\bar{B}_{r}\left(x_{0}\right)=\left\{x\in X:\left\|x-x_{0}\right\|\leq r\right\}.
We obtain the following result.
Theorem 2 Assume (1.5), (2.3), (2.4), and that the operator Γ0(X)\Gamma_{0}\in\mathcal{L}(X) is invertible, obeying

I[x0,G(x0);F]Γ0=η0uq\left\|I-\left[x_{0},G\left(x_{0}\right);F\right]\Gamma_{0}\right\|=\eta_{0}\leq uq (2.5)

where
0q<10\leq q<1,
b0=[x0,G(x0);F]1b_{0}=\left\|\left[x_{0},G\left(x_{0}\right);F\right]^{-1}\right\|,
ρ=b01q\rho=\frac{b_{0}}{1-q},
b=ρη0+1b=\rho\eta_{0}+1,
β=ab2(2+|γ|c)\beta=ab^{2}(2+|\gamma|c),
α=ab(b+|γ|)\alpha=ab(b+|\gamma|),
u=min{11+α,1(1+β)2}u=\min\left\{\frac{1}{1+\alpha},\frac{1}{(1+\beta)^{2}}\right\} and
p=b0a(2+|γ|c)rp=b_{0}a(2+|\gamma|c)r.
If x0,G(x0)Br(x0),F(x0)=δ0uqx_{0},G\left(x_{0}\right)\in B_{r}\left(x_{0}\right),\left\|F\left(x_{0}\right)\right\|=\delta_{0}\leq uq, and

|γ|F(x0)+buq1q\displaystyle|\gamma|\left\|F\left(x_{0}\right)\right\|+\frac{buq}{1-q} r,\displaystyle\leq r,
p\displaystyle p <1,\displaystyle<1,

then

  • the elements xk,G(xk)x_{k},G\left(x_{k}\right) remain in B¯r(x0)\bar{B}_{r}\left(x_{0}\right),

  • the sequences (xk)k0,(Γk)k0\left(x_{k}\right)_{k\geq 0},\left(\Gamma_{k}\right)_{k\geq 0} are Cauchy,

  • denoting x=limxkx^{*}=\lim x_{k}, one has the estimates

xxkbuq2k1q2k,k=0,1,\left\|x^{*}-x_{k}\right\|\leq\frac{buq^{2^{k}}}{1-q^{2^{k}}},\quad k=0,1,\ldots

limkΓk=[x,G(x);F]1-\lim_{k\rightarrow\infty}\Gamma_{k}=\left[x^{*},G\left(x^{*}\right);F\right]^{-1}, and

[x,G(x);F]1Γku(1+ab|γ|)q2k,k=0,1,\left\|\left[x^{*},G\left(x^{*}\right);F\right]^{-1}-\Gamma_{k}\right\|\leq u(1+ab|\gamma|)q^{2^{k}},\quad k=0,1,\ldots

Proof. Hypothesis p<1p<1 and the existence of [x0,G(x0);F]1\left[x_{0},G\left(x_{0}\right);F\right]^{-1} imply the existence of [x,G(x);F]1[x,G(x);F]^{-1} for all xB¯r(x0)x\in\bar{B}_{r}\left(x_{0}\right), and moreover

[x,G(x);F]1b01p=ρ,xB¯r(x0)\left\|[x,G(x);F]^{-1}\right\|\leq\frac{b_{0}}{1-p}=\rho,\quad\forall x\in\bar{B}_{r}\left(x_{0}\right) (2.6)

and

Γkρη0+1\left\|\Gamma_{k}\right\|\leq\rho\eta_{0}+1 (2.7)

Denoting ηk=I[xk,G(xk);F]Γk\eta_{k}=\left\|I-\left[x_{k},G\left(x_{k}\right);F\right]\Gamma_{k}\right\| and δk=F(xk),k=0,1,\delta_{k}=\left\|F\left(x_{k}\right)\right\|,k=0,1,\ldots, for xk,G(xk)B¯r(x0)x_{k},G\left(x_{k}\right)\in\bar{B}_{r}\left(x_{0}\right), we will show that the elements ηk\eta_{k} and δk\delta_{k} satisfy the assumptions of Lemma 2.1, which will imply

δk,ηkuq2k\delta_{k},\eta_{k}\leq uq^{2^{k}} (2.8)

Indeed, since FF is a polynomial operator of degree 2 we have

F(xk+1)=\displaystyle F\left(x_{k+1}\right)= F(xk)+[xk,G(xk);F](xk+1xk)+\displaystyle F\left(x_{k}\right)+\left[x_{k},G\left(x_{k}\right);F\right]\left(x_{k+1}-x_{k}\right)+
+[xk+1,xk,G(xk);F](xk+1xk)(xk+1G(xk))\displaystyle+\left[x_{k+1},x_{k},G\left(x_{k}\right);F\right]\left(x_{k+1}-x_{k}\right)\left(x_{k+1}-G\left(x_{k}\right)\right)

whence, by 1.2

F(xk+1)=\displaystyle F\left(x_{k+1}\right)= F(xk)[xk,G(xk);F]ΓkF(xk)\displaystyle F\left(x_{k}\right)-\left[x_{k},G\left(x_{k}\right);F\right]\Gamma_{k}F\left(x_{k}\right)-
DΓkF(xk)(ΓkF(xk)+γF(xk)),\displaystyle-D\Gamma_{k}F\left(x_{k}\right)\left(-\Gamma_{k}F\left(x_{k}\right)+\gamma F\left(x_{k}\right)\right),

and therefore

F(xk+1)\displaystyle\left\|F\left(x_{k+1}\right)\right\|\leq I[xk,G(xk);F]ΓkF(xk)+\displaystyle\left\|I-\left[x_{k},G\left(x_{k}\right);F\right]\Gamma_{k}\right\|\cdot\left\|F\left(x_{k}\right)\right\|+
+D(Γk2+|γ|Γk)F(xk)2\displaystyle+\|D\|\left(\left\|\Gamma_{k}\right\|^{2}+|\gamma|\left\|\Gamma_{k}\right\|\right)\left\|F\left(x_{k}\right)\right\|^{2}

i.e. δk+1ηkδk+αδk2\delta_{k+1}\leq\eta_{k}\delta_{k}+\alpha\delta_{k}^{2}, with α=ab(b+|γ|)\alpha=ab(b+|\gamma|).
From (1.2) we also get

I[xk+1,G(xk+1);F]Γk+1I[xk+1,G(xk+1);F]Γk2.\left\|I-\left[x_{k+1},G\left(x_{k+1}\right);F\right]\Gamma_{k+1}\right\|\leq\left\|I-\left[x_{k+1},G\left(x_{k+1}\right);F\right]\Gamma_{k}\right\|^{2}.

One can easily verify that

I[xk+1,G(xk+1);F]Γk\displaystyle\left\|I-\left[x_{k+1},G\left(x_{k+1}\right);F\right]\Gamma_{k}\right\|\leq
I[xk,G(xk);F]Γk\displaystyle\leq\left\|I-\left[x_{k},G\left(x_{k}\right);F\right]\Gamma_{k}\right\|
+DΓk2(2+|γ|[xk+1,xk;F]F(xk))\displaystyle\quad+\|D\|\cdot\left\|\Gamma_{k}\right\|^{2}\left(2+|\gamma|\left\|\left[x_{k+1},x_{k};F\right]\right\|\cdot\left\|F\left(x_{k}\right)\right\|\right)

whence, taking into account the notations we made, it follows

ηk+1(ηk+βδk)2\eta_{k+1}\leq\left(\eta_{k}+\beta\delta_{k}\right)^{2}

with β=ab2(2+|γ|c)\beta=ab^{2}(2+|\gamma|c).
Now we show that (xk)k0,(G(xk))k0B¯r(x0)\left(x_{k}\right)_{k\geq 0},\left(G\left(x_{k}\right)\right)_{k\geq 0}\in\bar{B}_{r}\left(x_{0}\right).
Assume that for some k0k\geq 0, xsB¯r(x0),s=0,k¯x_{s}\in\bar{B}_{r}\left(x_{0}\right),s=\overline{0,k}.
We have that

xs+1xs=ΓsF(xs)xs+1xsΓsF(xs)bδsbuq2s,s=0,k¯.\begin{gathered}x_{s+1}-x_{s}=-\Gamma_{s}F\left(x_{s}\right)\\ \left\|x_{s+1}-x_{s}\right\|\leq\left\|\Gamma_{s}\right\|\cdot\left\|F\left(x_{s}\right)\right\|\leq b\delta_{s}\leq buq^{2^{s}},\quad s=\overline{0,k}.\end{gathered}

Then

xk+1x0s=0kxs+1xss=0kbuq2sbuq1qr,\left\|x_{k+1}-x_{0}\right\|\leq\sum_{s=0}^{k}\left\|x_{s+1}-x_{s}\right\|\leq\sum_{s=0}^{k}buq^{2^{s}}\leq\frac{buq}{1-q}\leq r,

and

G(xk+1)x0\displaystyle\left\|G\left(x_{k+1}\right)-x_{0}\right\| G(xk+1)xk+1+xk+1x0\displaystyle\leq\left\|G\left(x_{k+1}\right)-x_{k+1}\right\|+\left\|x_{k+1}-x_{0}\right\|\leq
buq1q+|γ|F(xk)buq1q+|γ|F(x0)r\displaystyle\leq\frac{buq}{1-q}+|\gamma|\left\|F\left(x_{k}\right)\right\|\leq\frac{buq}{1-q}+|\gamma|\left\|F\left(x_{0}\right)\right\|\leq r

Using inequality 2.8 we shall show that the sequences (Γk)k0\left(\Gamma_{k}\right)_{k\geq 0} and (xk)k0\left(x_{k}\right)_{k\geq 0} are Cauchy, and therefore they converge.

Indeed,

xk+1xkbuq2k,k=0,1,\left\|x_{k+1}-x_{k}\right\|\leq buq^{2^{k}},\quad k=0,1,\ldots

Then,

xk+mxk\displaystyle\left\|x_{k+m}-x_{k}\right\| s=0m1xk+s+1xk+sbus=0m1q2k+s\displaystyle\leq\sum_{s=0}^{m-1}\left\|x_{k+s+1}-x_{k+s}\right\|\leq bu\sum_{s=0}^{m-1}q^{2^{k+s}}
buq2ks=0m1q2k+s2k=bu2ks=0m1q2k(2s1)\displaystyle\leq buq^{2^{k}}\sum_{s=0}^{m-1}q^{2^{k+s}-2^{k}}=bu2^{k}\sum_{s=0}^{m-1}q^{2^{k}\left(2^{s}-1\right)}
buq2k(1+q2k+q32k+)=buq2k1q2k,\displaystyle\leq buq^{2^{k}}\left(1+q^{2^{k}}+q^{3\cdot 2^{k}}+\cdots\right)=\frac{buq^{2^{k}}}{1-q^{2^{k}}},

which shows that (xk)k0\left(x_{k}\right)_{k\geq 0} is fundamental. Consequently, there exists x=limkxkx^{*}=\lim_{k\rightarrow\infty}x_{k} and

xxkbuq2k1q2k,k=0,1,\left\|x^{*}-x_{k}\right\|\leq\frac{buq^{2^{k}}}{1-q^{2^{k}}},\quad k=0,1,\ldots

Regarding the approximations Γk\Gamma_{k} we have

[x,G(x);F]1Γk\displaystyle\left\|\left[x^{*},G\left(x^{*}\right);F\right]^{-1}-\Gamma_{k}\right\| [x,G(x);F]1I[x,G(x);F]Γk\displaystyle\leq\left\|\left[x^{*},G\left(x^{*}\right);F\right]^{-1}\right\|\cdot\left\|I-\left[x^{*},G\left(x^{*}\right);F\right]\Gamma_{k}\right\|
ρI[x,G(x);F]Γk\displaystyle\leq\rho\left\|I-\left[x^{*},G\left(x^{*}\right);F\right]\Gamma_{k}\right\|

But

I[x,G(x);F]Γk\displaystyle\left\|I-\left[x^{*},G\left(x^{*}\right);F\right]\Gamma_{k}\right\|\leq
\displaystyle\leq I[xk,G(xk);F]Γk+\displaystyle\left\|I-\left[x_{k},G\left(x_{k}\right);F\right]\Gamma_{k}\right\|+
+Γk[xk,G(xk);F][x,G(x);F]\displaystyle+\left\|\Gamma_{k}\right\|\cdot\left\|\left[x_{k},G\left(x_{k}\right);F\right]-\left[x^{*},G\left(x^{*}\right);F\right]\right\|
\displaystyle\leq ηk+ΓkD|γ|δk\displaystyle\eta_{k}+\left\|\Gamma_{k}\right\|\|D\||\gamma|\delta_{k}

whence

[x,G(x);F]1Γkηk+ab|γ|δk\left\|\left[x^{*},G\left(x^{*}\right);F\right]^{-1}-\Gamma_{k}\right\|\leq\eta_{k}+ab|\gamma|\delta_{k}

which shows that limΓk=[x,G(x);F]1\lim\Gamma_{k}=\left[x^{*},G\left(x^{*}\right);F\right]^{-1}, and

[x,G(x);F]1Γk(u+ab|γ|u)q2k,k=0,1,\left\|\left[x^{*},G\left(x^{*}\right);F\right]^{-1}-\Gamma_{k}\right\|\leq(u+ab|\gamma|u)q^{2^{k}},\quad k=0,1,\ldots

3 Numerical examples: the approximation of the eigenpairs of matrices.

Denote V=𝕂nV=\mathbb{K}^{n} and let A𝕂n×nA\in\mathbb{K}^{n\times n} where 𝕂=\mathbb{K}=\mathbb{R} or \mathbb{C}.
For computing the eigenpairs of AA one may consider a mapping HH : V𝕂V\rightarrow\mathbb{K} with H(0)1H(0)\neq 1.

The eigenvalues and eigenvectors of AA are the solutions of

F(x)=(AvλvH(v)1)=0,F(x)=\binom{Av-\lambda v}{H(v)-1}=0,

where x=(vλ)V×𝕂=𝕂n+1x=\binom{v}{\lambda}\in V\times\mathbb{K}=\mathbb{K}^{n+1}.
Denoting v=(x(1),x(2),,x(n))v=\left(x^{(1)},x^{(2)},\ldots,x^{(n)}\right) and λ=x(n+1)\lambda=x^{(n+1)} then the first nn components of FF are
Fi(x)=F_{i}(x)=
ai1x(1)++ai,i1x(i1)+(aiix(n+1))x(i)+ai,i+1x(i+1)++ainx(n)a_{i1}x^{(1)}+\cdots+a_{i,i-1}x^{(i-1)}+\left(a_{ii}-x^{(n+1)}\right)x^{(i)}+a_{i,i+1}x^{(i+1)}+\cdots+a_{in}x^{(n)}.
If we take HH as

H(v)=αv2H(v)=\alpha\|v\|_{2}

for some fixed α\alpha\in\mathbb{R} then

Fn+1(x)=α((x(1))2++(x(n))2)1.F_{n+1}(x)=\alpha\left(\left(x^{(1)}\right)^{2}+\cdots+\left(x^{(n)}\right)^{2}\right)-1.

The matrices associated to the first order divided differences of FF at the points x1,x2𝕂n+1x_{1},x_{2}\in\mathbb{K}^{n+1} are

[x1,x2;F]=(b11a12a1na1,n+11a21b22a2na2,n+11an1an2bnnan,n+11an+1,1an+1,2an+1,n0)\left[x_{1},x_{2};F\right]=\left(\begin{array}[]{lllll}b_{11}&a_{12}&\cdots&a_{1n}&a_{1,n+1}^{1}\\ a_{21}&b_{22}&\cdots&a_{2n}&a_{2,n+1}^{1}\\ \vdots&\vdots&&\vdots&\vdots\\ a_{n1}&a_{n2}&\cdots&b_{nn}&a_{n,n+1}^{1}\\ a_{n+1,1}&a_{n+1,2}&\cdots&a_{n+1,n}&0\end{array}\right)

where bii=aii12(x2(n+1)+x1(n+1)),ai,n+1=12(x2(i)+x1(i))b_{ii}=a_{ii}-\frac{1}{2}\left(x_{2}^{(n+1)}+x_{1}^{(n+1)}\right),a_{i,n+1}=-\frac{1}{2}\left(x_{2}^{(i)}+x_{1}^{(i)}\right) and an+1,i=α(x1(i)+x2(i))a_{n+1,i}=\alpha\left(x_{1}^{(i)}+x_{2}^{(i)}\right), for i=1,,ni=1,\ldots,n.

The second order divided differences of FF at x1,x2,x3x_{1},x_{2},x_{3} are given by

[x1,x2,x3;F]hk=\left[x_{1},x_{2},x_{3};F\right]hk=
=(12k(n+1)0012k(1)012k(n+1)012k(2)0012k(n+1)12k(n)αk(1)αk(2)αk(n)0)(h(1)h(2)h(n)h(n+1))=\left(\begin{array}[]{ccccc}-\frac{1}{2}k^{(n+1)}&0&\cdots&0&-\frac{1}{2}k^{(1)}\\ 0&-\frac{1}{2}k^{(n+1)}&\cdots&0&-\frac{1}{2}k^{(2)}\\ \vdots&\vdots&&\vdots&\vdots\\ 0&0&\cdots&-\frac{1}{2}k^{(n+1)}&-\frac{1}{2}k^{(n)}\\ \alpha k^{(1)}&\alpha k^{(2)}&\cdots&\alpha k^{(n)}&0\end{array}\right)\left(\begin{array}[]{l}h^{(1)}\\ h^{(2)}\\ \vdots\\ h^{(n)}\\ h^{(n+1)}\end{array}\right)

for all h,k𝕂n+1h,k\in\mathbb{K}^{n+1}.
We shall consider the max norm on VV and taking x=max{v,|λ|}\|x\|=\max\left\{\|v\|_{\infty},|\lambda|\right\} for all x=(vλ)𝕂n+1x=\binom{v}{\lambda}\in\mathbb{K}^{n+1} we are led to the max norm on 𝕂n+1\mathbb{K}^{n+1}. It can be easily verified that [x1,x2,x3;F]max{1,n|α|}\left\|\left[x_{1},x_{2},x_{3};F\right]\right\|_{\infty}\leq\max\{1,n|\alpha|\}.

The classical choice for α\alpha is α=1/2\alpha=1/2. We have proposed in 11 the choice α=1/(2n)\alpha=1/(2n), which may lead to smaller bounds for the norm of the second order finite differences.

We shall consider the Fidap002 test matrix from the Harwell Boeing collection 1 in order to study the behavior of method (1.2) for approximating the eigenpairs. The program was written in Matlab; we took γ=0.05\gamma=0.05 and Γ0=[x0,G(x0);F]1\Gamma_{0}=\left[x_{0},G\left(x_{0}\right);F\right]^{-1}, computed with MatLab.

This real symmetric matrix of dimension n=441n=441 arise from finite element modeling. Its eigenvalues are all simple and range from 7108-7\cdot 10^{8} to 31063\cdot 10^{6}. We have chosen to study the smallest eigenvalue, which is well separated. The initial approximations were taken λ0=λ+1101\lambda_{0}=\lambda^{*}+1\cdot 10^{1} and for the initial vector v0v_{0} we perturbed the solution vv^{*} with random vectors having the components uniformly distributed on (ε,ε),ε=1104(-\varepsilon,\varepsilon),\varepsilon=1\cdot 10^{-4}; this value for ε\varepsilon had to be taken smaller than for other methods in order to obtain the attraction of the iterates (1.2); also, these iterates converged slower than others (see, e.g. [13]). The following results are typical for the runs made (we have considered a common vector ε\varepsilon ).

00footnotetext: 1 These matrices are available from MatrixMarket at the following address: http://math.nist.gov/MatrixMarket/.
Choice I Choice II
kk xxk\left\|x^{*}-x_{k}\right\| F(xk)\left\|F\left(x_{k}\right)\right\| xxk\left\|x^{*}-x_{k}\right\| F(xk)\left\|F\left(x_{k}\right)\right\|
0 1.000010+011.0000\cdot 10^{+01} 4.492210+44.4922\cdot 10^{+4} 1.000010+011.0000\cdot 10^{+01} 4.492310+44.4923\cdot 10^{+4}
1 1.352210+001.3522\cdot 10^{+00} 9.717510+39.7175\cdot 10^{+3} 1.998510+001.9985\cdot 10^{+00} 8.986310+38.9863\cdot 10^{+3}
2 6.327610016.3276\cdot 10^{-01} 1.110310+21.1103\cdot 10^{+2} 1.451410011.4514\cdot 10^{-01} 6.456210+26.4562\cdot 10^{+2}
3 1.502910011.5029\cdot 10^{-01} 8.461910+08.4619\cdot 10^{+0} 1.528710031.5287\cdot 10^{-03} 5.371510+05.3715\cdot 10^{+0}
4 6.923910036.9239\cdot 10^{-03} 1.04781011.0478\cdot 10^{-1} 5.404910065.4049\cdot 10^{-06} 6.86801046.8680\cdot 10^{-4}
5 6.796610056.7966\cdot 10^{-05} 1.04321041.0432\cdot 10^{-4} 1.397010091.3970\cdot 10^{-09} 6.77011086.7701\cdot 10^{-8}
6 3.073410083.0734\cdot 10^{-08} 4.29821084.2982\cdot 10^{-8} 4.656710104.6567\cdot 10^{-10} 4.44501084.4450\cdot 10^{-8}
7 4.656610104.6566\cdot 10^{-10} 3.51861093.5186\cdot 10^{-9} 2.790910122.7909\cdot 10^{-12} 5.43991085.4399\cdot 10^{-8}
Table 1: Table 1. Method (1.2) for Fidap002.

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