research article faster multistep iterations for the ...fixed points applied to zamfirescu operators...
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Hindawi Publishing CorporationAbstract and Applied AnalysisVolume 2013 Article ID 464593 4 pageshttpdxdoiorg1011552013464593
Research ArticleFaster Multistep Iterations for the Approximation ofFixed Points Applied to Zamfirescu Operators
Shin Min Kang1 Ljubomir B SiriT2 Arif Rafiq3 Faisal Ali4 and Young Chel Kwun5
1 Department of Mathematics and RINS Gyeongsang National University Jinju 660-701 Republic of Korea2 Faculty of Mechanical Engineering University of Belgrade Kraljice Marije 16 Belgrade 11000 Serbia3 Department of Mathematics Lahore Leads University Lahore 54810 Pakistan4Centre for Advanced Studies in Pure and Applied Mathematics Bahauddin Zakariya University Multan 54000 Pakistan5 Department of Mathematics Dong-A University Pusan 614-714 Republic of Korea
Correspondence should be addressed to Young Chel Kwun yckwundauackr
Received 13 July 2013 Accepted 7 September 2013
Academic Editor Salvador Romaguera
Copyright copy 2013 Shin Min Kang et alThis is an open access article distributed under the Creative Commons Attribution Licensewhich permits unrestricted use distribution and reproduction in any medium provided the original work is properly cited
By taking a counterexample we prove that the multistep iteration process is faster than the Mann and Ishikawa iteration processesfor Zamfirescu operators
1 Introduction
Let 119862 be a nonempty convex subset of a normed space 119864 andlet 119879 119862 rarr 119862 be a mapping
(a) For arbitrary 1199090isin 119862 the sequence 119909
119899 defined by
119909119899+1
= (1 minus 119887119899) 119909119899+ 119887119899119879119909119899 119899 ge 0 (119872
119899)
where 119887119899 is a sequence in [0 1] is known as the Mann
iteration process [1](b) For arbitrary 119909
0isin 119862 the sequence 119909
119899 defined by
119909119899+1
= (1 minus 119887119899) 119909119899+ 119887119899119879119910119899
119910119899= (1 minus 119887
1015840
119899) 119909119899+ 1198871015840
119899119879119909119899 119899 ge 0
(119868119899)
where 119887119899 and 119887
1015840
119899 are sequences in [0 1] is known as the
Ishikawa iteration process [2](c) For arbitrary 119909
0isin 119862 the sequence 119909
119899 defined by
119909119899+1
= (1 minus 119887119899) 119909119899+ 1198871198991198791199101
119899
119910119894
119899= (1 minus 119887
119894
119899) 119909119899+ 119887119894
119899119879119910119894+1
119899
119910119901minus1
119899= (1 minus 119887
119901minus1
119899) 119909119899+ 119887119901minus1
119899119879119899119909119899 119899 ge 0
(119877119878119899)
where 119887119899 and 119887119894
119899 119894 = 1 2 119901 minus 2 (119901 ge 2) are sequences
in [0 1] and denoted by (119877119878119899) is known as the multistep
iteration process [3]
Definition 1 (see [4]) Suppose that 119886119899 and 119887
119899 are two real
convergent sequences with limits 119886 and 119887 respectively Then119886119899 is said to converge faster than 119887
119899 if
lim119899rarrinfin
10038161003816100381610038161003816100381610038161003816
119886119899minus 119886
119887119899minus 119887
10038161003816100381610038161003816100381610038161003816
= 0 (1)
Definition 2 (see [4]) Let 119906119899 and V
119899 be two fixed-point
iteration procedures which both converge to the same fixedpoint 119901 say with error estimates
1003817100381710038171003817119906119899 minus 1199011003817100381710038171003817 le 119886119899
1003817100381710038171003817V119899 minus 1199011003817100381710038171003817 le 119887119899 119899 ge 0 (2)
where lim 119886119899= 0 = lim 119887
119899 If 119886119899 converges faster than 119887
119899
then 119906119899 is said to converge faster than V
119899
Theorem 3 (see [5]) Let (119883 119889) be a complete metric spaceand let 119879 119883 rarr 119883 be a mapping for which there exist realnumbers 119886 119887 and 119888 satisfying 119886 isin (0 1) and 119887 119888 isin (0 12) suchthat for each pair 119909 119910 isin 119883 at least one of the following is true
(1199111) 119889(119879119909 119879119910) le 119886119889(119909 119910)
2 Abstract and Applied Analysis
(1199112) 119889(119879119909 119879119910) le 119887[119889(119909 119879119909) + 119889(119910 119879119910)](1199113) 119889(119879119909 119879119910) le 119888[119889(119909 119879119910) + 119889(119910 119879119909)]
Then119879 has a unique fixed point119901 and the Picard iteration119909119899 defined by
119909119899+1
= 119879119909119899 119899 ge 0 (3)
converges to 119901 for any 1199090isin 119883
Remark 4 An operator 119879 which satisfies the contractionconditions (1199111)ndash(1199113) of Theorem 3 will be called a Zam-firescu operator [4 6 7]
In [6 7] Berinde introduced a new class of operators ona normed space 119864 satisfying
1003817100381710038171003817119879119909 minus 1198791199101003817100381710038171003817 le 120575
1003817100381710038171003817119909 minus 1199101003817100381710038171003817 + 119871 119879119909 minus 119909 (4)
for any 119909 119910 isin 119864 0 le 120575 lt 1 and 119871 ge 0He proved that this class is wider than the class of
Zamfirescu operatorsThe following results are proved in [6 7]
Theorem5 (see [7]) Let119862 be a nonempty closed convex subsetof a normed space 119864 Let 119879 119862 rarr 119862 be an operator satisfying(4) Let 119909
119899 be defined through the iterative process (119872
119899) and
1199090isin 119862 If 119865(119879) = 0 and sum
infin
119899=0119887119899= infin then 119909
119899 converges
strongly to the unique fixed point of 119879
Theorem6 (see [6]) Let119862 be a nonempty closed convex subsetof an arbitrary Banach space 119864 and let 119879 119862 rarr 119862 be anoperator satisfying (4) Let 119909
119899 be defined through the iterative
process (119868119899) and 119909
0isin 119862 where 119887
119899 and 1198871015840
119899 are sequences of
positive numbers in [0 1] with 119887119899 satisfying suminfin
119899=0119887119899= infin
Then 119909119899 converges strongly to the fixed point of 119879
The following result can be found in [8]
Theorem 7 Let 119862 be a closed convex subset of an arbitraryBanach space 119864 Let theMann and Ishikawa iteration processeswith real sequences 119887
119899 and 1198871015840
119899 satisfy 0 le 119887
119899 1198871015840119899le 1 and
suminfin
119899=0119887119899= infin Then (119872
119899) and (119868
119899) converge strongly to the
unique fixed point of 119879 Let 119879 119862 rarr 119862 be a Zamfirescuoperator and moreover the Mann iteration process convergesfaster than the Ishikawa iteration process to the fixed point of119879
In [4] Berinde proved the following result
Theorem 8 Let 119862 be a closed convex subset of an arbitraryBanach space 119864 and let 119879 119862 rarr 119862 be a Zamfirescu operatorLet 119910
119899 be defined by (119872
119899) and 119910
0isin 119862 with a sequence 119887
119899
in [0 1] satisfying suminfin119899=0
119887119899= infin Then 119910
119899 converges strongly
to the fixed point of 119879 and moreover the Picard iteration 119909119899
converges faster than the Mann iteration
Remark 9 In [9] Qing and Rhoades by taking a counterex-ample showed that the Mann iteration process convergesmore slowly than the Ishikawa iteration process for Zam-firescu operators
In this paper we establish a general theorem to approxi-mate fixed points of quasi-contractive operators in a Banachspace through themultistep iteration process Our result gen-eralizes and improves upon amongothers the correspondingresults of Babu and Vara Prasad [8] and Berinde [4 6 7]
We also prove that the Mann iteration process and theIshikawa iteration process converge more slowly than themultistep iteration process for Zamfirescu operators
2 Main Results
We now prove our main results
Theorem 10 Let 119862 be a nonempty closed convex subset of anarbitrary Banach space 119864 and let 119879 119862 rarr 119862 be an operatorsatisfying (4) Let 119909
119899 be defined through the iterative process
(119877119878119899) and 119909
0isin 119862 where 119887
119899 and 119887119894
119899 119894 = 1 2 119901minus2 (119901 ge
2) are sequences in [0 1] with suminfin119899=0
119887119899= infin If 119865(119879) = 0 then
119865(119879) is a singleton and the sequence 119909119899 converges strongly to
the fixed point of 119879
Proof Assume that 119865(119879) = 0 and 119908 isin 119865(119879) Then using(119877119878119899) we have
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 =
10038171003817100381710038171003817(1 minus 119887
119899) 119909119899+ 1198871198991198791199101
119899minus 119908
10038171003817100381710038171003817
=10038171003817100381710038171003817(1 minus 119887
119899) (119909119899minus 119908) + 119887
119899(1198791199101
119899minus 119908)
10038171003817100381710038171003817
le (1 minus 119887119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 119887119899
100381710038171003817100381710038171198791199101
119899minus 119908
10038171003817100381710038171003817
(5)
Now for 119909 = 119908 and 119910 = 1199101
119899 (4) gives
100381710038171003817100381710038171198791199101
119899minus 119908
10038171003817100381710038171003817le 120575
100381710038171003817100381710038171199101
119899minus 119908
10038171003817100381710038171003817 (6)
By substituting (6) in (5) we obtain
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 le (1 minus 119887
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 120575119887119899
100381710038171003817100381710038171199101
119899minus 119908
10038171003817100381710038171003817 (7)
In a similar fashion again by using (119877119878119899) we can get
10038171003817100381710038171003817119910119894
119899minus 119908
10038171003817100381710038171003817le (1 minus 119887
119894
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 120575119887119894
119899
10038171003817100381710038171003817119910119894+1
119899minus 119908
10038171003817100381710038171003817 (8)
where 119894 = 1 2 119901 minus 2 (119901 ge 2) and
10038171003817100381710038171003817119910119901minus1
119899minus 119908
10038171003817100381710038171003817le (1 minus (1 minus 120575) 119887
119901minus1
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (9)
It can be easily seen that for 119894 = 1 2 119901 minus 2 (119901 ge 2) wehave
100381710038171003817100381710038171199101
119899minus 119908
10038171003817100381710038171003817le (1 minus 119887
1
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 1205751198871
119899
100381710038171003817100381710038171199102
119899minus 119908
10038171003817100381710038171003817
10038171003817100381710038171003817119910119901minus3
119899minus 119908
10038171003817100381710038171003817le (1 minus 119887
119901minus3
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 120575119887119901minus3
119899
10038171003817100381710038171003817119910119901minus2
119899minus 119908
10038171003817100381710038171003817
10038171003817100381710038171003817119910119901minus2
119899minus 119908
10038171003817100381710038171003817le (1 minus 119887
119901minus2
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 120575119887119901minus2
119899
10038171003817100381710038171003817119910119901minus1
119899minus 119908
10038171003817100381710038171003817
(10)
Abstract and Applied Analysis 3
Substituting (9) in (10) gives us
10038171003817100381710038171003817119910119901minus2
119899minus 119908
10038171003817100381710038171003817le (1 minus (1 minus 120575) 119887
119901minus2
119899(1 + 120575119887
119901minus1
119899))1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (11)
It may be noted that for 120575 isin [0 1) and 120578119899 isin [0 1] the
following inequality is always true
1 le 1 + 120575120578119899le 1 + 120575 (12)
From (11) and (12) we get
10038171003817100381710038171003817119910119901minus2
119899minus 119908
10038171003817100381710038171003817le (1 minus (1 minus 120575) 119887
119901minus2
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (13)
By repeating the same procedure finally from (7) and (10) weyield
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 le [1 minus (1 minus 120575) 119887
119899]1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (14)
By (14) we inductively obtain
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 le
119899
prod
119896=0
[1 minus (1 minus 120575) 119887119896]10038171003817100381710038171199090 minus 119908
1003817100381710038171003817 119899 ge 0 (15)
Using the fact that 0 le 120575 lt 1 0 le 119887119899le 1 andsuminfin
119899=0119887119899= infin it
results that
lim119899rarrinfin
119899
prod
119896=0
[1 minus (1 minus 120575) 119887119896] = 0 (16)
which by (15) implies that
lim119899rarrinfin
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 = 0 (17)
Consequently 119909119899rarr 119908 isin 119865 and this completes the proof
Now by a counterexample we prove that the multistepiteration process is faster than the Mann and Ishikawaiteration processes for Zamfirescu operators
Example 11 Suppose that 119879 [0 1] rarr [0 1] is defined by119879119909 = (12)119909 119887
119899= 0 = 119887
119901minus1
119899= 119887119894
119899 119894 = 1 2 119901 minus 1 (119901 ge
2) and 119899 = 1 2 15 119887119899= 4radic119899 = 119887
119901minus1
119899= 119887119894
119899 119894 =
1 2 119901 minus 1 (119901 ge 2) and 119899 ge 16 It is clear that 119879 is aZamfirescu operator with a unique fixed point 0 and that allof the conditions ofTheorem 10 are satisfied Also119872
119899= 1199090=
119868119899= 119877119878119899 119899 = 1 2 15 Suppose that 119909
0= 0 For the Mann
and Ishikawa iteration processes we have
119872119899= (1 minus 119887
119899) 119909119899+ 119887119899119879119909119899
= (1 minus4
radic119899)119909119899+
4
radic119899
1
2119909119899
= (1 minus2
radic119899)119909119899
= sdot sdot sdot =
119899
prod
119894=16
(1 minus2
radic119894) 1199090
119868119899= (1 minus 119887
119899) 119909119899+ 119887119899119879 ((1 minus 119887
1015840
119899) 119909119899+ 1198871015840
119899119879119909119899)
= (1 minus4
radic119899)119909119899+
4
radic119899
1
2(1 minus
2
radic119899)119909119899
= (1 minus2
radic119899minus4
119899)119909119899
= sdot sdot sdot =
119899
prod
119894=16
(1 minus2
radic119894minus4
119894) 1199090
119877119878119899= (1 minus 119887
119899) 119909119899+ 1198871198991198791199101
119899
119910119894
119899= (1 minus 119887
119894
119899) 119909119899+ 119887119894
119899119879119910119894+1
119899
119910119901minus1
119899= (1 minus 119887
119901minus1
119899) 119909119899+ 119887119901minus1
119899119879119909119899 119899 ge 0
(18)where 119894 = 1 2 119901 minus 2 (119901 ge 2) implies that
119877119878119899= (1 minus
119901
sum
119895=1
(2
radic119899)
119895
)119909119899
= sdot sdot sdot =
119899
prod
119894=16
(1 minus
119901
sum
119895=1
(2
radic119894)
119895
)1199090
(19)
Now consider
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119872119899minus 0
10038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
) 1199090
prod119899
119894=16(1 minus (2radic119894)) 119909
0
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
)
prod119899
119894=16(1 minus (2radic119894))
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=2(2radic119894)
119896
1 minus (2radic119894)
)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=2(2radic119894)
119896
radic119894
radic119894 minus 2)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
(20)
It is easy to see that
0 le lim119899rarrinfin
119899
prod
119894=16
(1 minus
sum119901
119896=2(2radic119894)
119896
radic119894
radic119894 minus 2)
le lim119899rarrinfin
119899
prod
119894=16
(1 minus1
119894)
= lim119899rarrinfin
15
119899
= 0
(21)
Hence
lim119899rarrinfin
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119872119899minus 0
10038161003816100381610038161003816100381610038161003816
= 0 (22)
4 Abstract and Applied Analysis
Thus theMann iteration process converges more slowly thanthe multistep iteration process to the fixed point 0 of 119879
Similarly
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119868119899minus 0
10038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
) 1199090
prod119899
119894=16(1 minus (2radic119894) minus (4119894)) 119909
0
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
)
prod119899
119894=16(1 minus (2radic119894) minus (4119894))
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
1 minus (2radic119894) minus (4119894)
)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
119894radic119894
119894radic119894 minus 2119894 minus 4radic119894)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
(23)
with
0 le lim119899rarrinfin
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
119894radic119894
119894radic119894 minus 2119894 minus 4radic119894)
le lim119899rarrinfin
119899
prod
119894=16
(1 minus1
119894)
= lim119899rarrinfin
15
119899
= 0
(24)
implies that
lim119899rarrinfin
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119868119899minus 0
10038161003816100381610038161003816100381610038161003816
= 0 (25)
Thus the Ishikawa iteration process converges more slowlythan the multistep iteration process to the fixed point 0 of 119879
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors would like to thank the editor and the refereesfor their useful comments and suggestions This study wassupported by research funds from Dong-A University
References
[1] W R Mann ldquoMean value methods in iterationrdquo Proceedings ofthe American Mathematical Society vol 4 pp 506ndash510 1953
[2] S Ishikawa ldquoFixed points by a new iteration methodrdquo Proceed-ings of the American Mathematical Society vol 44 pp 147ndash1501974
[3] B E Rhoades and S M Soltuz ldquoThe equivalence betweenMann-Ishikawa iterations and multistep iterationrdquo NonlinearAnalysis Theory Methods amp Applications vol 58 no 1-2 pp219ndash228 2004
[4] V Berinde ldquoPicard iteration converges faster than Mann iter-ation for a class of quasi-contractive operatorsrdquo Fixed PointTheory and Applications no 2 pp 97ndash105 2004
[5] T Zamfirescu ldquoFix point theorems inmetric spacesrdquoArchiv derMathematik vol 23 pp 292ndash298 1972
[6] V Berinde ldquoOn the convergence of the Ishikawa iteration inthe class of quasi contractive operatorsrdquoActaMathematica Uni-versitatis Comenianae vol 73 no 1 pp 119ndash126 2004
[7] V Berinde ldquoA convergence theorem for some mean value fixedpoint iteration proceduresrdquoDemonstratio Mathematica vol 38no 1 pp 177ndash184 2005
[8] G V R Babu and K N V V Vara Prasad ldquoMann iteration con-verges faster than Ishikawa iteration for the class of Zamfirescuoperatorsrdquo Fixed Point Theory and Applications vol 2006Article ID 49615 6 pages 2006
[9] Y Qing and B E Rhoades ldquoComments on the rate of con-vergence between Mann and Ishikawa iterations applied toZamfirescu operatorsrdquo Fixed PointTheory and Applications vol2008 Article ID 387504 3 pages 2008
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Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
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Stochastic AnalysisInternational Journal of
2 Abstract and Applied Analysis
(1199112) 119889(119879119909 119879119910) le 119887[119889(119909 119879119909) + 119889(119910 119879119910)](1199113) 119889(119879119909 119879119910) le 119888[119889(119909 119879119910) + 119889(119910 119879119909)]
Then119879 has a unique fixed point119901 and the Picard iteration119909119899 defined by
119909119899+1
= 119879119909119899 119899 ge 0 (3)
converges to 119901 for any 1199090isin 119883
Remark 4 An operator 119879 which satisfies the contractionconditions (1199111)ndash(1199113) of Theorem 3 will be called a Zam-firescu operator [4 6 7]
In [6 7] Berinde introduced a new class of operators ona normed space 119864 satisfying
1003817100381710038171003817119879119909 minus 1198791199101003817100381710038171003817 le 120575
1003817100381710038171003817119909 minus 1199101003817100381710038171003817 + 119871 119879119909 minus 119909 (4)
for any 119909 119910 isin 119864 0 le 120575 lt 1 and 119871 ge 0He proved that this class is wider than the class of
Zamfirescu operatorsThe following results are proved in [6 7]
Theorem5 (see [7]) Let119862 be a nonempty closed convex subsetof a normed space 119864 Let 119879 119862 rarr 119862 be an operator satisfying(4) Let 119909
119899 be defined through the iterative process (119872
119899) and
1199090isin 119862 If 119865(119879) = 0 and sum
infin
119899=0119887119899= infin then 119909
119899 converges
strongly to the unique fixed point of 119879
Theorem6 (see [6]) Let119862 be a nonempty closed convex subsetof an arbitrary Banach space 119864 and let 119879 119862 rarr 119862 be anoperator satisfying (4) Let 119909
119899 be defined through the iterative
process (119868119899) and 119909
0isin 119862 where 119887
119899 and 1198871015840
119899 are sequences of
positive numbers in [0 1] with 119887119899 satisfying suminfin
119899=0119887119899= infin
Then 119909119899 converges strongly to the fixed point of 119879
The following result can be found in [8]
Theorem 7 Let 119862 be a closed convex subset of an arbitraryBanach space 119864 Let theMann and Ishikawa iteration processeswith real sequences 119887
119899 and 1198871015840
119899 satisfy 0 le 119887
119899 1198871015840119899le 1 and
suminfin
119899=0119887119899= infin Then (119872
119899) and (119868
119899) converge strongly to the
unique fixed point of 119879 Let 119879 119862 rarr 119862 be a Zamfirescuoperator and moreover the Mann iteration process convergesfaster than the Ishikawa iteration process to the fixed point of119879
In [4] Berinde proved the following result
Theorem 8 Let 119862 be a closed convex subset of an arbitraryBanach space 119864 and let 119879 119862 rarr 119862 be a Zamfirescu operatorLet 119910
119899 be defined by (119872
119899) and 119910
0isin 119862 with a sequence 119887
119899
in [0 1] satisfying suminfin119899=0
119887119899= infin Then 119910
119899 converges strongly
to the fixed point of 119879 and moreover the Picard iteration 119909119899
converges faster than the Mann iteration
Remark 9 In [9] Qing and Rhoades by taking a counterex-ample showed that the Mann iteration process convergesmore slowly than the Ishikawa iteration process for Zam-firescu operators
In this paper we establish a general theorem to approxi-mate fixed points of quasi-contractive operators in a Banachspace through themultistep iteration process Our result gen-eralizes and improves upon amongothers the correspondingresults of Babu and Vara Prasad [8] and Berinde [4 6 7]
We also prove that the Mann iteration process and theIshikawa iteration process converge more slowly than themultistep iteration process for Zamfirescu operators
2 Main Results
We now prove our main results
Theorem 10 Let 119862 be a nonempty closed convex subset of anarbitrary Banach space 119864 and let 119879 119862 rarr 119862 be an operatorsatisfying (4) Let 119909
119899 be defined through the iterative process
(119877119878119899) and 119909
0isin 119862 where 119887
119899 and 119887119894
119899 119894 = 1 2 119901minus2 (119901 ge
2) are sequences in [0 1] with suminfin119899=0
119887119899= infin If 119865(119879) = 0 then
119865(119879) is a singleton and the sequence 119909119899 converges strongly to
the fixed point of 119879
Proof Assume that 119865(119879) = 0 and 119908 isin 119865(119879) Then using(119877119878119899) we have
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 =
10038171003817100381710038171003817(1 minus 119887
119899) 119909119899+ 1198871198991198791199101
119899minus 119908
10038171003817100381710038171003817
=10038171003817100381710038171003817(1 minus 119887
119899) (119909119899minus 119908) + 119887
119899(1198791199101
119899minus 119908)
10038171003817100381710038171003817
le (1 minus 119887119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 119887119899
100381710038171003817100381710038171198791199101
119899minus 119908
10038171003817100381710038171003817
(5)
Now for 119909 = 119908 and 119910 = 1199101
119899 (4) gives
100381710038171003817100381710038171198791199101
119899minus 119908
10038171003817100381710038171003817le 120575
100381710038171003817100381710038171199101
119899minus 119908
10038171003817100381710038171003817 (6)
By substituting (6) in (5) we obtain
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 le (1 minus 119887
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 120575119887119899
100381710038171003817100381710038171199101
119899minus 119908
10038171003817100381710038171003817 (7)
In a similar fashion again by using (119877119878119899) we can get
10038171003817100381710038171003817119910119894
119899minus 119908
10038171003817100381710038171003817le (1 minus 119887
119894
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 120575119887119894
119899
10038171003817100381710038171003817119910119894+1
119899minus 119908
10038171003817100381710038171003817 (8)
where 119894 = 1 2 119901 minus 2 (119901 ge 2) and
10038171003817100381710038171003817119910119901minus1
119899minus 119908
10038171003817100381710038171003817le (1 minus (1 minus 120575) 119887
119901minus1
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (9)
It can be easily seen that for 119894 = 1 2 119901 minus 2 (119901 ge 2) wehave
100381710038171003817100381710038171199101
119899minus 119908
10038171003817100381710038171003817le (1 minus 119887
1
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 1205751198871
119899
100381710038171003817100381710038171199102
119899minus 119908
10038171003817100381710038171003817
10038171003817100381710038171003817119910119901minus3
119899minus 119908
10038171003817100381710038171003817le (1 minus 119887
119901minus3
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 120575119887119901minus3
119899
10038171003817100381710038171003817119910119901minus2
119899minus 119908
10038171003817100381710038171003817
10038171003817100381710038171003817119910119901minus2
119899minus 119908
10038171003817100381710038171003817le (1 minus 119887
119901minus2
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 + 120575119887119901minus2
119899
10038171003817100381710038171003817119910119901minus1
119899minus 119908
10038171003817100381710038171003817
(10)
Abstract and Applied Analysis 3
Substituting (9) in (10) gives us
10038171003817100381710038171003817119910119901minus2
119899minus 119908
10038171003817100381710038171003817le (1 minus (1 minus 120575) 119887
119901minus2
119899(1 + 120575119887
119901minus1
119899))1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (11)
It may be noted that for 120575 isin [0 1) and 120578119899 isin [0 1] the
following inequality is always true
1 le 1 + 120575120578119899le 1 + 120575 (12)
From (11) and (12) we get
10038171003817100381710038171003817119910119901minus2
119899minus 119908
10038171003817100381710038171003817le (1 minus (1 minus 120575) 119887
119901minus2
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (13)
By repeating the same procedure finally from (7) and (10) weyield
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 le [1 minus (1 minus 120575) 119887
119899]1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (14)
By (14) we inductively obtain
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 le
119899
prod
119896=0
[1 minus (1 minus 120575) 119887119896]10038171003817100381710038171199090 minus 119908
1003817100381710038171003817 119899 ge 0 (15)
Using the fact that 0 le 120575 lt 1 0 le 119887119899le 1 andsuminfin
119899=0119887119899= infin it
results that
lim119899rarrinfin
119899
prod
119896=0
[1 minus (1 minus 120575) 119887119896] = 0 (16)
which by (15) implies that
lim119899rarrinfin
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 = 0 (17)
Consequently 119909119899rarr 119908 isin 119865 and this completes the proof
Now by a counterexample we prove that the multistepiteration process is faster than the Mann and Ishikawaiteration processes for Zamfirescu operators
Example 11 Suppose that 119879 [0 1] rarr [0 1] is defined by119879119909 = (12)119909 119887
119899= 0 = 119887
119901minus1
119899= 119887119894
119899 119894 = 1 2 119901 minus 1 (119901 ge
2) and 119899 = 1 2 15 119887119899= 4radic119899 = 119887
119901minus1
119899= 119887119894
119899 119894 =
1 2 119901 minus 1 (119901 ge 2) and 119899 ge 16 It is clear that 119879 is aZamfirescu operator with a unique fixed point 0 and that allof the conditions ofTheorem 10 are satisfied Also119872
119899= 1199090=
119868119899= 119877119878119899 119899 = 1 2 15 Suppose that 119909
0= 0 For the Mann
and Ishikawa iteration processes we have
119872119899= (1 minus 119887
119899) 119909119899+ 119887119899119879119909119899
= (1 minus4
radic119899)119909119899+
4
radic119899
1
2119909119899
= (1 minus2
radic119899)119909119899
= sdot sdot sdot =
119899
prod
119894=16
(1 minus2
radic119894) 1199090
119868119899= (1 minus 119887
119899) 119909119899+ 119887119899119879 ((1 minus 119887
1015840
119899) 119909119899+ 1198871015840
119899119879119909119899)
= (1 minus4
radic119899)119909119899+
4
radic119899
1
2(1 minus
2
radic119899)119909119899
= (1 minus2
radic119899minus4
119899)119909119899
= sdot sdot sdot =
119899
prod
119894=16
(1 minus2
radic119894minus4
119894) 1199090
119877119878119899= (1 minus 119887
119899) 119909119899+ 1198871198991198791199101
119899
119910119894
119899= (1 minus 119887
119894
119899) 119909119899+ 119887119894
119899119879119910119894+1
119899
119910119901minus1
119899= (1 minus 119887
119901minus1
119899) 119909119899+ 119887119901minus1
119899119879119909119899 119899 ge 0
(18)where 119894 = 1 2 119901 minus 2 (119901 ge 2) implies that
119877119878119899= (1 minus
119901
sum
119895=1
(2
radic119899)
119895
)119909119899
= sdot sdot sdot =
119899
prod
119894=16
(1 minus
119901
sum
119895=1
(2
radic119894)
119895
)1199090
(19)
Now consider
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119872119899minus 0
10038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
) 1199090
prod119899
119894=16(1 minus (2radic119894)) 119909
0
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
)
prod119899
119894=16(1 minus (2radic119894))
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=2(2radic119894)
119896
1 minus (2radic119894)
)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=2(2radic119894)
119896
radic119894
radic119894 minus 2)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
(20)
It is easy to see that
0 le lim119899rarrinfin
119899
prod
119894=16
(1 minus
sum119901
119896=2(2radic119894)
119896
radic119894
radic119894 minus 2)
le lim119899rarrinfin
119899
prod
119894=16
(1 minus1
119894)
= lim119899rarrinfin
15
119899
= 0
(21)
Hence
lim119899rarrinfin
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119872119899minus 0
10038161003816100381610038161003816100381610038161003816
= 0 (22)
4 Abstract and Applied Analysis
Thus theMann iteration process converges more slowly thanthe multistep iteration process to the fixed point 0 of 119879
Similarly
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119868119899minus 0
10038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
) 1199090
prod119899
119894=16(1 minus (2radic119894) minus (4119894)) 119909
0
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
)
prod119899
119894=16(1 minus (2radic119894) minus (4119894))
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
1 minus (2radic119894) minus (4119894)
)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
119894radic119894
119894radic119894 minus 2119894 minus 4radic119894)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
(23)
with
0 le lim119899rarrinfin
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
119894radic119894
119894radic119894 minus 2119894 minus 4radic119894)
le lim119899rarrinfin
119899
prod
119894=16
(1 minus1
119894)
= lim119899rarrinfin
15
119899
= 0
(24)
implies that
lim119899rarrinfin
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119868119899minus 0
10038161003816100381610038161003816100381610038161003816
= 0 (25)
Thus the Ishikawa iteration process converges more slowlythan the multistep iteration process to the fixed point 0 of 119879
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors would like to thank the editor and the refereesfor their useful comments and suggestions This study wassupported by research funds from Dong-A University
References
[1] W R Mann ldquoMean value methods in iterationrdquo Proceedings ofthe American Mathematical Society vol 4 pp 506ndash510 1953
[2] S Ishikawa ldquoFixed points by a new iteration methodrdquo Proceed-ings of the American Mathematical Society vol 44 pp 147ndash1501974
[3] B E Rhoades and S M Soltuz ldquoThe equivalence betweenMann-Ishikawa iterations and multistep iterationrdquo NonlinearAnalysis Theory Methods amp Applications vol 58 no 1-2 pp219ndash228 2004
[4] V Berinde ldquoPicard iteration converges faster than Mann iter-ation for a class of quasi-contractive operatorsrdquo Fixed PointTheory and Applications no 2 pp 97ndash105 2004
[5] T Zamfirescu ldquoFix point theorems inmetric spacesrdquoArchiv derMathematik vol 23 pp 292ndash298 1972
[6] V Berinde ldquoOn the convergence of the Ishikawa iteration inthe class of quasi contractive operatorsrdquoActaMathematica Uni-versitatis Comenianae vol 73 no 1 pp 119ndash126 2004
[7] V Berinde ldquoA convergence theorem for some mean value fixedpoint iteration proceduresrdquoDemonstratio Mathematica vol 38no 1 pp 177ndash184 2005
[8] G V R Babu and K N V V Vara Prasad ldquoMann iteration con-verges faster than Ishikawa iteration for the class of Zamfirescuoperatorsrdquo Fixed Point Theory and Applications vol 2006Article ID 49615 6 pages 2006
[9] Y Qing and B E Rhoades ldquoComments on the rate of con-vergence between Mann and Ishikawa iterations applied toZamfirescu operatorsrdquo Fixed PointTheory and Applications vol2008 Article ID 387504 3 pages 2008
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
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Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
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Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
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Mathematical PhysicsAdvances in
Complex AnalysisJournal of
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OptimizationJournal of
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CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
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Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
Abstract and Applied Analysis 3
Substituting (9) in (10) gives us
10038171003817100381710038171003817119910119901minus2
119899minus 119908
10038171003817100381710038171003817le (1 minus (1 minus 120575) 119887
119901minus2
119899(1 + 120575119887
119901minus1
119899))1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (11)
It may be noted that for 120575 isin [0 1) and 120578119899 isin [0 1] the
following inequality is always true
1 le 1 + 120575120578119899le 1 + 120575 (12)
From (11) and (12) we get
10038171003817100381710038171003817119910119901minus2
119899minus 119908
10038171003817100381710038171003817le (1 minus (1 minus 120575) 119887
119901minus2
119899)1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (13)
By repeating the same procedure finally from (7) and (10) weyield
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 le [1 minus (1 minus 120575) 119887
119899]1003817100381710038171003817119909119899 minus 119908
1003817100381710038171003817 (14)
By (14) we inductively obtain
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 le
119899
prod
119896=0
[1 minus (1 minus 120575) 119887119896]10038171003817100381710038171199090 minus 119908
1003817100381710038171003817 119899 ge 0 (15)
Using the fact that 0 le 120575 lt 1 0 le 119887119899le 1 andsuminfin
119899=0119887119899= infin it
results that
lim119899rarrinfin
119899
prod
119896=0
[1 minus (1 minus 120575) 119887119896] = 0 (16)
which by (15) implies that
lim119899rarrinfin
1003817100381710038171003817119909119899+1 minus 1199081003817100381710038171003817 = 0 (17)
Consequently 119909119899rarr 119908 isin 119865 and this completes the proof
Now by a counterexample we prove that the multistepiteration process is faster than the Mann and Ishikawaiteration processes for Zamfirescu operators
Example 11 Suppose that 119879 [0 1] rarr [0 1] is defined by119879119909 = (12)119909 119887
119899= 0 = 119887
119901minus1
119899= 119887119894
119899 119894 = 1 2 119901 minus 1 (119901 ge
2) and 119899 = 1 2 15 119887119899= 4radic119899 = 119887
119901minus1
119899= 119887119894
119899 119894 =
1 2 119901 minus 1 (119901 ge 2) and 119899 ge 16 It is clear that 119879 is aZamfirescu operator with a unique fixed point 0 and that allof the conditions ofTheorem 10 are satisfied Also119872
119899= 1199090=
119868119899= 119877119878119899 119899 = 1 2 15 Suppose that 119909
0= 0 For the Mann
and Ishikawa iteration processes we have
119872119899= (1 minus 119887
119899) 119909119899+ 119887119899119879119909119899
= (1 minus4
radic119899)119909119899+
4
radic119899
1
2119909119899
= (1 minus2
radic119899)119909119899
= sdot sdot sdot =
119899
prod
119894=16
(1 minus2
radic119894) 1199090
119868119899= (1 minus 119887
119899) 119909119899+ 119887119899119879 ((1 minus 119887
1015840
119899) 119909119899+ 1198871015840
119899119879119909119899)
= (1 minus4
radic119899)119909119899+
4
radic119899
1
2(1 minus
2
radic119899)119909119899
= (1 minus2
radic119899minus4
119899)119909119899
= sdot sdot sdot =
119899
prod
119894=16
(1 minus2
radic119894minus4
119894) 1199090
119877119878119899= (1 minus 119887
119899) 119909119899+ 1198871198991198791199101
119899
119910119894
119899= (1 minus 119887
119894
119899) 119909119899+ 119887119894
119899119879119910119894+1
119899
119910119901minus1
119899= (1 minus 119887
119901minus1
119899) 119909119899+ 119887119901minus1
119899119879119909119899 119899 ge 0
(18)where 119894 = 1 2 119901 minus 2 (119901 ge 2) implies that
119877119878119899= (1 minus
119901
sum
119895=1
(2
radic119899)
119895
)119909119899
= sdot sdot sdot =
119899
prod
119894=16
(1 minus
119901
sum
119895=1
(2
radic119894)
119895
)1199090
(19)
Now consider
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119872119899minus 0
10038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
) 1199090
prod119899
119894=16(1 minus (2radic119894)) 119909
0
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
)
prod119899
119894=16(1 minus (2radic119894))
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=2(2radic119894)
119896
1 minus (2radic119894)
)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=2(2radic119894)
119896
radic119894
radic119894 minus 2)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
(20)
It is easy to see that
0 le lim119899rarrinfin
119899
prod
119894=16
(1 minus
sum119901
119896=2(2radic119894)
119896
radic119894
radic119894 minus 2)
le lim119899rarrinfin
119899
prod
119894=16
(1 minus1
119894)
= lim119899rarrinfin
15
119899
= 0
(21)
Hence
lim119899rarrinfin
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119872119899minus 0
10038161003816100381610038161003816100381610038161003816
= 0 (22)
4 Abstract and Applied Analysis
Thus theMann iteration process converges more slowly thanthe multistep iteration process to the fixed point 0 of 119879
Similarly
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119868119899minus 0
10038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
) 1199090
prod119899
119894=16(1 minus (2radic119894) minus (4119894)) 119909
0
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
)
prod119899
119894=16(1 minus (2radic119894) minus (4119894))
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
1 minus (2radic119894) minus (4119894)
)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
119894radic119894
119894radic119894 minus 2119894 minus 4radic119894)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
(23)
with
0 le lim119899rarrinfin
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
119894radic119894
119894radic119894 minus 2119894 minus 4radic119894)
le lim119899rarrinfin
119899
prod
119894=16
(1 minus1
119894)
= lim119899rarrinfin
15
119899
= 0
(24)
implies that
lim119899rarrinfin
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119868119899minus 0
10038161003816100381610038161003816100381610038161003816
= 0 (25)
Thus the Ishikawa iteration process converges more slowlythan the multistep iteration process to the fixed point 0 of 119879
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors would like to thank the editor and the refereesfor their useful comments and suggestions This study wassupported by research funds from Dong-A University
References
[1] W R Mann ldquoMean value methods in iterationrdquo Proceedings ofthe American Mathematical Society vol 4 pp 506ndash510 1953
[2] S Ishikawa ldquoFixed points by a new iteration methodrdquo Proceed-ings of the American Mathematical Society vol 44 pp 147ndash1501974
[3] B E Rhoades and S M Soltuz ldquoThe equivalence betweenMann-Ishikawa iterations and multistep iterationrdquo NonlinearAnalysis Theory Methods amp Applications vol 58 no 1-2 pp219ndash228 2004
[4] V Berinde ldquoPicard iteration converges faster than Mann iter-ation for a class of quasi-contractive operatorsrdquo Fixed PointTheory and Applications no 2 pp 97ndash105 2004
[5] T Zamfirescu ldquoFix point theorems inmetric spacesrdquoArchiv derMathematik vol 23 pp 292ndash298 1972
[6] V Berinde ldquoOn the convergence of the Ishikawa iteration inthe class of quasi contractive operatorsrdquoActaMathematica Uni-versitatis Comenianae vol 73 no 1 pp 119ndash126 2004
[7] V Berinde ldquoA convergence theorem for some mean value fixedpoint iteration proceduresrdquoDemonstratio Mathematica vol 38no 1 pp 177ndash184 2005
[8] G V R Babu and K N V V Vara Prasad ldquoMann iteration con-verges faster than Ishikawa iteration for the class of Zamfirescuoperatorsrdquo Fixed Point Theory and Applications vol 2006Article ID 49615 6 pages 2006
[9] Y Qing and B E Rhoades ldquoComments on the rate of con-vergence between Mann and Ishikawa iterations applied toZamfirescu operatorsrdquo Fixed PointTheory and Applications vol2008 Article ID 387504 3 pages 2008
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
4 Abstract and Applied Analysis
Thus theMann iteration process converges more slowly thanthe multistep iteration process to the fixed point 0 of 119879
Similarly
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119868119899minus 0
10038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
) 1199090
prod119899
119894=16(1 minus (2radic119894) minus (4119894)) 119909
0
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
prod119899
119894=16(1 minus sum
119901
119895=1(2radic119894)
119895
)
prod119899
119894=16(1 minus (2radic119894) minus (4119894))
1003816100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
1 minus (2radic119894) minus (4119894)
)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
=
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
119894radic119894
119894radic119894 minus 2119894 minus 4radic119894)
100381610038161003816100381610038161003816100381610038161003816100381610038161003816
(23)
with
0 le lim119899rarrinfin
119899
prod
119894=16
(1 minus
sum119901
119896=3(2radic119894)
119896
119894radic119894
119894radic119894 minus 2119894 minus 4radic119894)
le lim119899rarrinfin
119899
prod
119894=16
(1 minus1
119894)
= lim119899rarrinfin
15
119899
= 0
(24)
implies that
lim119899rarrinfin
10038161003816100381610038161003816100381610038161003816
119877119878119899minus 0
119868119899minus 0
10038161003816100381610038161003816100381610038161003816
= 0 (25)
Thus the Ishikawa iteration process converges more slowlythan the multistep iteration process to the fixed point 0 of 119879
Conflict of Interests
The authors declare that there is no conflict of interestsregarding the publication of this paper
Acknowledgments
The authors would like to thank the editor and the refereesfor their useful comments and suggestions This study wassupported by research funds from Dong-A University
References
[1] W R Mann ldquoMean value methods in iterationrdquo Proceedings ofthe American Mathematical Society vol 4 pp 506ndash510 1953
[2] S Ishikawa ldquoFixed points by a new iteration methodrdquo Proceed-ings of the American Mathematical Society vol 44 pp 147ndash1501974
[3] B E Rhoades and S M Soltuz ldquoThe equivalence betweenMann-Ishikawa iterations and multistep iterationrdquo NonlinearAnalysis Theory Methods amp Applications vol 58 no 1-2 pp219ndash228 2004
[4] V Berinde ldquoPicard iteration converges faster than Mann iter-ation for a class of quasi-contractive operatorsrdquo Fixed PointTheory and Applications no 2 pp 97ndash105 2004
[5] T Zamfirescu ldquoFix point theorems inmetric spacesrdquoArchiv derMathematik vol 23 pp 292ndash298 1972
[6] V Berinde ldquoOn the convergence of the Ishikawa iteration inthe class of quasi contractive operatorsrdquoActaMathematica Uni-versitatis Comenianae vol 73 no 1 pp 119ndash126 2004
[7] V Berinde ldquoA convergence theorem for some mean value fixedpoint iteration proceduresrdquoDemonstratio Mathematica vol 38no 1 pp 177ndash184 2005
[8] G V R Babu and K N V V Vara Prasad ldquoMann iteration con-verges faster than Ishikawa iteration for the class of Zamfirescuoperatorsrdquo Fixed Point Theory and Applications vol 2006Article ID 49615 6 pages 2006
[9] Y Qing and B E Rhoades ldquoComments on the rate of con-vergence between Mann and Ishikawa iterations applied toZamfirescu operatorsrdquo Fixed PointTheory and Applications vol2008 Article ID 387504 3 pages 2008
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of
Submit your manuscripts athttpwwwhindawicom
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical Problems in Engineering
Hindawi Publishing Corporationhttpwwwhindawicom
Differential EquationsInternational Journal of
Volume 2014
Applied MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Probability and StatisticsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Mathematical PhysicsAdvances in
Complex AnalysisJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
OptimizationJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
CombinatoricsHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Operations ResearchAdvances in
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Function Spaces
Abstract and Applied AnalysisHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of Mathematics and Mathematical Sciences
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Algebra
Discrete Dynamics in Nature and Society
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Decision SciencesAdvances in
Discrete MathematicsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom
Volume 2014 Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Stochastic AnalysisInternational Journal of