Volume 2010, Article ID 821928,13pages doi:10.1155/2010/821928
Research Article
Nonexpansive Matrices with Applications to Solutions of Linear Systems by Fixed Point Iterations
Teck-Cheong Lim
Department of Mathematical Sciences, George Mason University, 4400, University Drive, Fairfax, VA 22030, USA
Correspondence should be addressed to Teck-Cheong Lim,[email protected] Received 28 August 2009; Accepted 19 October 2009
Academic Editor: Mohamed A. Khamsi
Copyrightq2010 Teck-Cheong Lim. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
We characterizeimatrices which are nonexpansive with respect to some matrix norms, andii matrices whose average iterates approach zero or are bounded. Then we apply these results to iterative solutions of a system of linear equations.
Throughout this paper,Rwill denote the set of real numbers,Cthe set of complex numbers, andMnthe complex vector space of complexn×nmatrices. A function · :Mn → Ris a matrix norm if for allA, B∈Mn, it satisfies the following five axioms:
1A ≥0;
2A0 if and only ifA0;
3cA|c|Afor all complex scalarsc;
4AB ≤ AB;
5AB ≤ A B.
Let| · |be a norm onCn. Define · onMnby Amax
|x|1|Ax|. 1
This norm onMnis a matrix norm, called the matrix norm induced by| · |. A matrix norm on Mnis called an induced matrix norm if it is induced by some norm onCn. If · 1is a matrix norm onMn, there exists an induced matrix norm · 2onMnsuch thatA2 ≤ A1for all
A∈Mncf.1, page 297. Indeed one can take · 2to be the matrix norm induced by the norm| · |onCndefined by
|x|Cx1, 2
whereCxis the matrix inMnwhose columns are all equal tox. ForA∈Mn,ρAdenotes the spectral radius ofA.
Let | · |be a norm in Cn. A matrix A ∈ Mn is a contraction relative to | · |if it is a contraction as a transformation fromCnintoCn; that is, there exists 0≤λ <1 such that
Ax−Ay≤λx−y, x, y∈Cn. 3 Evidently this means that for the matrix norm · induced by| · |,A < 1. The following theorem is well knowncf.1, Sections 5.6.9–5.6.12.
Theorem 1. For a matrixA∈Mn, the following are equivalent:
aAis a contraction relative to a norm inCn; bA<1 for some induced matrix norm · ; cA<1 for some matrix norm · ;
dlimk→ ∞Ak0;
eρA<1.
Thatbfollows fromcis a consequence of the previous remark about an induced matrix norm being less than a matrix norm. Since all norms onMn are equivalent, the limit ind can be relative to any norm onMn, so thatdis equivalent to all the entries ofAkconverge to zero ask → ∞, which in turn is equivalent to limk→ ∞Akx0 for allx∈Cn.
In this paper, we first characterize matrices inMnthat are nonexpansive relative to some norm| · |onCn, that is,
Ax−Ay≤x−y, x, y∈Cn. 4
Then we characterize thoseA∈Mnsuch that
Ak 1 k
IAA2· · ·Ak−1
5
converges to zero ask → ∞, and those that{Ak:k0,1,2, . . .}is bounded.
Finally we apply our theory to approximation of solution ofAx busing iterative methodsfixed point iteration methods.
Theorem 2. For a matrixA∈Mn, the following are equivalent:
aAis nonexpansive relative to some norm onCn; bA ≤1 for some induced matrix norm · ; cA ≤1 for some matrix norm · ;
d{Ak:k0,1,2, . . .}is bounded;
eρA≤1, and for any eigenvalueλofAwith|λ|1, the geometric multiplicity is equal to the algebraic multiplicity.
Proof. As in the previous theorem,a,b, andcare equivalent. Assume thatbholds. Let the norm · be induced by a vector norm| · |ofCn. Then
Akx≤Ak|x| ≤ Ak|x| ≤ |x|, k0,1,2, . . . , 6
proving thatAkxis bounded in norm| · |for everyx∈Cn. Takingxei, we see that the set of all columns ofAk, k0,1,2, . . . ,is bounded. This proves thatAk, k0,1,2, . . . ,is bounded in maximum column sum matrix norm1, page 294, and hence in any norm inMn. Note that the last part of the proof also follows from the Uniform Boundedness Principlesee, e.g., 2, Corollary 21, page 66
Now we prove thatdimpliese. Suppose thatAhas an eigenvalueλwithλ > 1.
Letxbe an eigenvector corresponding toλ. Then
Akx|λ|kx −→ ∞ 7
ask → ∞, where · is any vector norm ofCn. This contradictsd. Hence|λ| ≤ 1. Now suppose thatλis an eigenvalue with|λ| 1 and the Jordan block corresponding toλis not diagonal. Then there exist nonzero vectorsv1, v2such thatAv1 λv1, Av2 v1λv2. Let uv1v2. Then
Akuλk−1λkv1λkv2, 8
and Aku ≥ kv1 − v1 − v2. It follows that Aku, k 0,1,2, . . . , is unbounded, contradictingd. Hencedimpliese.
Lastly we prove thateimpliesc. Assume thateholds.Ais similar to its Jordan canonical form J whose nonzero off-diagonal entries can be made arbitrarily small by similarity 1, page 128. Since the Jordan block for each eigenvalue with modulus 1 is diagonal, we see that there is an invertible matrix S such that the l1-sum of each row of SAS−1is less than or equal to 1, that is,SAS−1∞≤1, where · ∞is the maximum row sum matrix norm1, page 295. Define a matrix norm · byMSMS−1∞. Then we have A ≤1.
Letλbe an eigenvalue of a matrixA∈Mn. The index ofλ, denoted by indexλis the smallest value ofkfor which rankA−λIkrankA−λIk11, pages 148 and 131. Thus conditioneabove can be restated asρA≤1, and for any eigenvalueλofAwith|λ|1, indexλ 1.
LetA∈Mn. Consider
Ak 1 k
IA· · ·Ak−1
. 9
We callAk thek-average of A. As with Ak, we have Akx → 0 for every xif and only if Ak → 0 inMn, and thatAkxis bounded for everyxif and only ifAkis bounded inMn. We have the following theorem.
Theorem 3. LetA∈Mn. Then
aAk, k1,2, . . . ,converges to 0 if and only ifA ≤1 for some matrix norm · and that 1 is not an eigenvalue ofA,
bAk, k 1,2, . . . ,is bounded if and only ifρA≤ 1,indexλ≤2 for every eigenvalueλ with|λ|1 and that index1 1 if 1 is an eigenvalue ofA.
Proof. First we prove the sufficiency part ofa. Letxbe a vector inCn. Let yk 1
k
IA· · ·Ak−1
x. 10
ByTheorem 2for any eigenvaluesλofAeither|λ|<1 or|λ|1 and indexλ 1.
If Ais written in its Jordan canonical formA SJS−1, then the k-average ofA is SJS−1, whereJis thek-average ofJ.Jis in turn composed of thek-average of each of its Jordan blocks. For a Jordan block ofJof the form
⎛
⎜⎜
⎜⎜
⎜⎜
⎝ λ 1
λ 1
· ·
· 1 λ
⎞
⎟⎟
⎟⎟
⎟⎟
⎠
, 11
|λ|must be less than 1. Itsk-average has constant diagonal and upper diagonals. LetDjbe the constat value of itsjth upper diagonalD0being the diagonaland let Sj kDj. Then Cm, n 0 forn > m
S0 1−λk 1−λ , SjC
j, j C
j1, j
λ· · ·C
k−1, j
λk−1−j, j 1,2, . . . , n−1.
12
Using the relationCm1, j−Cm, j Cm, j−1, we obtain Sj−λSjSj−1−λk−jC
k, j
. 13
Thus, we haveS0 → 1/1−λask → ∞. By induction, using13above and the fact that λk−jCk, j → 0 ask → ∞, we obtainSj → 1/1−λj1ask → ∞. ThereforeDj Sj/k O1/kask → ∞.
If the Jordan block is diagonal of constant valueλ, thenλ /1,|λ| ≤1 and thek-average of the block is diagonal of constant value1−λk/k1−λ O1/k.
We conclude thatAkO1/kand henceyk ≤ AkxO1/kask → ∞.
Now we prove the necessity part of a. If 1 is an eigenvalue of A and x is a corresponding eigenvector, thenAkxx /0 for everykand of courseBkxfails to converge to 0. Ifλis an eigenvalue ofAwith|λ|>1 andxis a corresponding eigenvector, then
Akx λk−1
kλ−1
x ≥ |λ|k−1
k|λ−1| x. 14
which approaches to ∞ as k → ∞. If λ is an eigenvalue of A with |λ| 1, λ /1, and indexλ≥2, then there exist nonzero vectorsv1, v2such thatAv1 λv1, Av2 v1λv2. Then by using the identity
12λ3λ2· · · k−1λk−2 1−λk−1
1−λ2 −k−1λk−1
1−λ 15
we get
Akv2
1−λk−1 k1−λ2 −
1− 1
k λk−1
1−λ
v1 1−λk
k1−λv2. 16
It follows that limk→ ∞Akv2does not exist. This completes the proof of parta.
Suppose that A satisfies the conditions in b and that A SJS−1 is the Jordan canonical form of A. Let λ be an eigenvalue of A and let v be a column vector of S corresponding to λ. If |λ| < 1, then the restriction B of A to the subspace spanned by v, Av, A2v, . . . is a contraction, and we have Akv Bkv ≤ v. If |λ| 1, and λ /1, then by conditions in b either Av λv, or there exist v1, v2 with v v2 such that Av1 λv1, Av2 v1λv2. In the former case, we haveAk ≤ vand in the latter case, we see from16thatAkv Akv2is bounded. Finally ifλ1 then since index1 1, we haveAvvand henceAkvv. In all cases, we proved thatAkv, k0,1,2, . . . ,is bounded.
Since column vectors ofSform a basis forCn, the sufficiency part ofbfollows.
Now we prove the necessity part ofb. If Ahas an eigenvalue λ with|λ| > 1 and eigenvectorv, then as shown aboveAkv → ∞ask → ∞. IfAhas 1 as an eigenvalue and index1 ≥ 2, then there exist nonzero vectorsv1, v2 such thatAv1 v1 andAv2 v1v2. ThenAkv2 k−1/2v2which is unbounded. Ifλis an eigenvalue ofAwith|λ|1, λ /1 and indexλ≥3, then there exist nonzero vectorsv1, v2andv3such thatAv1λv1, Av2
v1λv2andAv3 v2λv3. By expandingAjv3, j0,1,2, . . . , k−1 and using the identity
k−1
j2
C j,2
λj−2 1 1−λ2
1−λk−2 1−λ 1
2k−2λk−2k−1λ−k1
, 17
we obtain
Akv3
1 1−λ2
1−λk−2 k1−λ1
2k−2λk−2 k−1
k λ−k1 k
v1
1−λk−1 k1−λ2 −
1− 1
k λk−1
1−λ
v2 1−λk k1−λv3
18
which approaches to∞ask → ∞. This completes the proof.
We now consider applications of preceding theorems to approximation of solution of a linear systemAxb, whereA∈Mnandba given vector inCn. LetQbe a given invertible matrix inMn.xis a solution ofAx bif and only ifxis a fixed point of the mappingT defined by
Tx
I−Q−1A
xQ−1b. 19
T is a contraction if and only if I −Q−1A is. In this case, by the well known Contraction Mapping Theorem, given any initial vector x0, the sequence of iterates xk Tkx0, k 0,1,2, . . . ,converges to the unique solution ofAx b. In practice, givenx0, each successive xkis obtained fromxk−1by solving the equation
Qxk Q−Axk−1b. 20
The classical methods of Richardson, Jacobi, and Gauss-Seidelsee, e.g.,3haveQ I, D, and L respectively, where I is the identity matrix, D the diagonal matrix containing the diagonal of A, andL the lower triangular matrix containing the lower triangular portion ofA. Thus byTheorem 1we have the following known theorem.
Theorem 4. LetA, Q ∈ Mn, with Qinvertible. Letb, x0 ∈ Cn. IfρI −Q−1A < 1, thenA is invertible and the sequencexk, k1,2, . . . ,defined recursively by
Qxk Q−Axk−1b 21
converges to the unique solution ofAxb.
Theorem 4fails ifρI−Q−1A 1, For a simple 2 × 2 example, letQI, b0, A2I andx0any nonzero vector.
We need the following lemma in the proof of the next two theorems. For a matrix A∈Mn, we will denoteRAandNAthe range and the null space ofArespectively.
Lemma 5. LetAbe a singular matrix inMnsuch that the geometric multiplicity and the algebraic multiplicity of the eigenvalue 0 are equal, that is, index0 1. Then there is a unique projection PAwhose range is the range ofAand whose null space is the null space ofA, or equivalently,Cn RA⊕NA. Moreover,Arestricted toRAis an invertible transformation fromRAontoRA.
Proof. IfASJS−1is a Jordan canonical form ofAwhere the eigenvalues 0 appear at the end portion of the diagonal ofJ, then the matrix
PAS
⎡
⎢⎢
⎢⎢
⎢⎢
⎢⎢
⎢⎢
⎢⎢
⎢⎢
⎢⎢
⎢⎣ 1
·
· 1
0
·
· 0
⎤
⎥⎥
⎥⎥
⎥⎥
⎥⎥
⎥⎥
⎥⎥
⎥⎥
⎥⎥
⎥⎦
S−1 22
is the required projection. ObviouslyAmapsRAintoRA. Ifz∈RAandAz 0, then z∈NA∩RA {0}and soz0. This proves thatAis invertible onRA.
Remark 6. Under the assumptions ofLemma 5, we will call the component of a vectorcin NAthe projection ofconNAalongRA. Note that by definition of index, the condition in the lemma is equivalent toNA2 NA.
Theorem 7. LetAbe a matrix inMnandba vector inCn. LetQbe an invertible matrix inMnand letB I−Q−1A. Assume thatρB ≤ 1 and that indexλ 1 for every eigenvalueλofBwith modulus 1, that is,Bis nonexpansive relative to a matrix norm. Starting with an initial vectorx0in Cndefinexkrecursively by
Qxk Q−Axk−1b 23
fork1,2, . . . .Let
yk x0x1· · ·xk−1
k . 24
IfAx bis consistent, that is, has a solution, thenyk, k 1,2, . . . ,converge to a solution vectorz with rate of convergenceyk−zO1/k. IfAxbis inconsistent, then limkxklimkyk
∞. More precisely, limkxk/kcand limkyk/kc/2, wherecQ−1bandcis the projection ofc onNA NQ−1AalongRQ−1A.
Proof. First we assume thatAis invertible so thatI−BQ−1Ais also invertible. LetTbe the mapping defined byTxBxc. ThenTkxBkxcBc· · ·Bk−1c. LetscBc· · ·Bk−1c.
Thens−Bsc−Bkcand hences I−B−1c−I−B−1Bkc I−B−1c−BkI−B−1c. Let z I−B−1cA−1b.zis the unique solution ofAxband
TkxBkxz−BkzBkx−z z. 25
Since the sequencexkin the theorem isTkx0, we have yk 1
k
IB· · ·Bk−1
x0−z zBkx0−z z. 26
SinceI−Bis invertible, 1 is not an eigenvalue ofB, and byTheorem 3 partayk−z Bkx0−z → 0 ask → ∞. Moreover, from the proof of the same theorem,yk−zO1/k.
Next we consider the case when Ais not invertible. Since Q is invertible, we have RQ−1A Q−1RAandNQ−1A NA. The index of the eigenvalue 0 ofQ−1Ais the index of eigenvalue 1 ofBI−Q−1A. Thus byLemma 5,CnQ−1RA⊕NA. For every vectorv ∈ Cn, let vr andvn denote the component ofvin the subspaceQ−1RAand NA, respectively.
Assume thatAxbis consistent, that is,b∈RA. Thenc∈RQ−1A. ByLemma 5, the restriction ofQ−1Aon its range is invertible, so there exists a uniquezinRQ−1Asuch thatQ−1Azc, or equivalently,I−Bzc. For any vectorx, we have
TkxBkxcBc· · ·Bk−1c BK
xrxn
IB· · ·Bk−1
I−Bz Bk
xr
xnz−Bk z Bk
xr−z
xnz.
27
SinceBmapsRQ−1AintoRQ−1AandI−BQ−1Arestricted toRQ−1Ais invertible, we can apply the preceding proof and conclude that the sequenceykas defined before converges tozx0nzandyk−zO1/k. NowAzAxn0 Az Az Qcb, showing thatzis a solution ofAxb.
Assume now thatb /∈RA, that is,Ax bis inconsistent. Thenc /∈RQ−1Aandc crcnwithcn/0.As in the preceding case there exists a uniquez∈RQ−1Asuch that I−Bz cr. Note that for ally∈NA,By I−Q−1Ay y. Thus for any vectorx and any positive integerj
xj Tjx
BjxcBc· · ·Bj−1c Bj
xrxn
IB· · ·Bj−1
I−Bzjcn Bj
xr
xnz−Bj z
jcn Bj
xr−z
xnzjcn, yk 1
k
xTx· · ·Tk−1x
Bk
xr−z
xnzk−1 2 cn,
28
whereBk IB· · ·Bk−1. As in the preceding case,Bkxr−z, k0,1,2, . . .is bounded andBkxr−z, k1,2, . . . ,converges to 0. Thus limk→ ∞xk/k cnand limk→ ∞yk/k cn/2, and hence limk→ ∞xklimk→ ∞yk∞. This completes the proof.
Next we consider another kind of iteration in which the nonlinear case was considered in Ishikawa 4. Note that the type of mappings in this case is slightly weaker than nonexpansivitysee conditioncin the next lemma.
Lemma 8. LetBbe ann×nmatrix. The following are equivalent:
afor every 0< μ <1, there exists a matrix norm · μsuch thatμI 1−μBμ≤1, bfor every 0< μ <1, there exists an induced matrix norm·μsuch thatμI1−μBμ≤1, cρB≤1 and index1 1 if 1 is an eigenvalue ofB.
Proof. As in the proof ofTheorem 2,aandbare equivalent. For 0 < μ < 1, denoteμI 1−μBbyBμ. Suppose now thataholds. Letλ be an eigenvalue ofB. Thenμ 1− μλ is an eigenvalue of Bμ. By Theorem 2 |μ 1 −μλ| ≤ 1 for every 0 < μ < 1 and hence|λ| ≤1. If 1 is an eigenvalue ofB, then it is also an eigenvalue ofBμ. ByTheorem 2, the index of 1, as an eigenvalue of Bμ, is 1. Since obviously B and Bμ have the same eigenvectors corresponding to the eigenvalue 1, the index of 1, as an eigenvalue ofB, is also 1. This provesc.
Now assumecholds. Since|μ 1−μλ| < 1 for|λ| 1, λ /1, every eigenvalue of Bμ, except possibly for 1, has modulus less than 1. Reasoning as above, if 1 is an eigenvalue ofBμ, then its index is 1. Therefore byTheorem 2,aholds. This completes the proof.
Theorem 9. LetA ∈ Mnandb ∈ Cn. LetQbe an invertible matrix inMn, andB I−Q−1A.
SupposeρB≤1 and that index1 1 if 1 is an eigenvalue ofB. Let 0< μ <1 be fixed. Starting with an initial vectorx0, definexk, yk, k0,1,2, . . . ,recursively by
y0x0, Qxk Q−A
yk−1 b, ykμyk−1
1−μ xk.
29
IfAxbis consistent, thenyk, k 0,1,2, . . . ,converges to a solution vectorzofAxbwith rate of convergence given by
yk−zo ζk
, 30
whereζis any number satisfying
maxμ 1−μ
λ:λan eigenvalue ofB, λ /1
< ζ <1. 31
IfAxbis inconsistent, then limk→ ∞yk∞; more precisely,
k→ ∞lim yk
k 1−μ
cn, 32
wherecnis the projection ofconNAalong RQ−1A.
Proof. Letc Q−1b, B1 μI 1−μB I−1−μQ−1A, andTx B1x 1−μc. Then ykTkx0.
First we assume thatAis invertible. ThenI−B1 1−μQ−1Ais invertible and 1 is not an eigenvalue ofB1; thusρB1<1. Letz 1−μI−B1−1cA−1b. We have
ykTkx0
Bk1x0 1−μ
cB1c· · ·Bk−11 c Bk1x0
1−μ 1 1−μ
IB1· · ·B1k−1
I−B1z Bk1x0−z z.
33
By a well known theoremsee, e.g.1,yk−zoζkfor everyζ > ρB1.
Assume now thatAis not invertible andb ∈ RA. Thenc is in the range ofQ−1A.
Since B I − Q−1A satisfies the condition in Lemma 8, Q−1A satisfies the condition in Lemma 5. Thus the restriction ofQ−1Aon its range is invertible and there existszinRQ−1A such that Q−1Az c, or equivalently, I −B1z 1−μc. For any vector x x0, we have
ykTkx B1kx
1−μ
cB1c· · ·Bk−11 c B1k
xrxn
IB1· · ·B1k−1
I−B1z B1k
xr
xnz−Bk1 z B1k
xr−z
xnz.
34
SinceB1mapsRQ−1AintoRQ−1AandI−BQ−1Arestricted toRQ−1Ais invertible, we can apply the preceding proof and conclude that the sequenceyk, k0,1,2, . . .converges toz xnzandyk−z oζk.zsolvesAx bsinceAz Axn Az Az Qcb.
Assume lastly thatb /∈RA, that is,Ax b is inconsistent. Thenc /∈RQ−1Aand ccrcnwithcn/0. As before there existsz∈RQ−1Asuch thatI−b1z 1−μcr. Note thatB1p pforp∈NA. Then
ykTkx Bk1x
1−μ
cB1c· · ·Bk−11 c Bk1
xrxn
IB1· · ·Bk−11
I−B1zk 1−μ
cn Bk1
xr−z
xnzk 1−μ
cn.
35
SinceBk1xr−z, k0,1,2, . . . ,converges to 0, we have
k→ ∞lim yk
k 1−μ
cn, 36
and hence limk→ ∞yk∞. This completes the proof.
By takingQIand considering only nonexpansive matrices in Theorems7and9, we obtain the following corollary.
Corollary 10. LetAbe ann×nmatrix such thatI−A ≤1 for some matrix norm · . Letbbe a vector inCn. Then:
astarting with an initial vectorx0inCndefinexkrecursively as follows:
xk I−Axk−1 b 37
fork1,2, . . . .Let
yk x0x1· · ·xk−1
k 38
fork 1,2, . . . .IfAxbis consistent, thenyk, k 1,2, . . . ,converges to a solution vectorzwith rate of convergence given by
yk−zO 1
k
. 39
IfAxbis inconsistent, then limk→ ∞xklimk→ ∞yk∞.
blet 0< μ <1 be a fixed number. Starting with an initial vectorx0, let y0x0,
xk I−A yk−1
b, ykμyk−1
1−μ xk.
40
IfAxbis consistent, thenyk, k 0,1,2, . . . ,converges to a solution vectorzofAxbwith rate of convergence given by
yk−zo ζk
41
whereζis any number satisfying maxμ
1−μ
λ:λan eigenvalue ofB, λ /1
< ζ <1. 42
IfAxbis inconsistent, then limk→ ∞yk∞.
Remark 11. If in the previous corollary,I−A<1, andμ0 in partb, the sequenceykxk
converges to a solution. This is the Richardson method, see for example,3. Even in this case, our method in partbmay yield a better approximation. For example if
A
1 0.9
−0.9 1
, 43
b 0, and x0 e1, then the nth iterate in the Richardson method is 0.9n away from the solution 0, while thenth iterate using the method in the corollary partbwithμ1/2 is less than0.5n/2.
Ann×nmatrixA aijis called diagonally dominant if
|aii| ≥ n
j1,j /i
aij 44
for alli1, . . . , n. IfAis diagonally dominant withaii/0 for everyiand ifQDorL, where D is the diagonal matrix containing the diagonal ofA, and Lthe lower triangular matrix containing the lower triangular entries of A, then it is easy to prove thatI−Q−1A∞ ≤ 1 where · ∞ denotes the maximum row sum matrix norm; see, for example,1,3. The following follows from Theorems7and9.
Corollary 12. LetAbe a diagonally dominantn×nmatrix withaii/0 for alli1, . . . , n. LetQD orL, whereDis the diagonal matrix containing the diagonal ofA, andLthe lower triangular matrix containing the lower triangular entries ofA. Letbbe a vector inCn. Then:
astarting with an initial vectorx0inCndefinexkrecursively as follows:
Qxk Q−Axk−1 b 45
fork1,2, . . . .Let
yk x0x1· · ·xk−1
k 46
fork 1,2, . . . .IfAx bis consistent, thenyk, k 1,2, . . .converges to a solution vectorzwith rate of convergence given by
yk−zO 1
k
. 47
IfAxbis inconsistent, then limk→ ∞xklimk→ ∞yk∞.
bLet 0< μ <1 be a fixed number. Starting with an initial vectorx0, let y0x0,
Qxk Q−A yk−1
b, ykμyk−1
1−μ xk.
48
IfAxbis consistent, thenyk, k 0,1,2, . . . ,converges to a solution vectorzofAxbwith rate of convergence given by
yk−zo ζk
, 49
whereζis any number satisfying maxμ
1−μ
λ:λan eigenvalue ofB, λ /1
< ζ <1. 50 IfAxbis inconsistent, then limk→ ∞yk∞.
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