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FOR A CLASS OF REGULARIZATION METHODS USING A MODIFIED PROJECTION SCHEME

M. T. NAIR AND M. P. RAJAN Received 22 June 2001

Solodki˘ı (1998) applied the modified projection scheme of Pereverzev (1995) for obtaining error estimates for a class of regularization methods for solving ill-posed operator equations. But, no a posteriori procedure for choosing the regularization parameter is discussed. In this paper, we consider Arcangeli’s type discrepancy principles for such a general class of regularization methods with modified projection scheme.

1. Introduction

Regularization methods are often employed for obtaining stable approximate solutions for ill-posed operator equations of the form

T x=y, (1.1)

whereT :XXis a compact linear operator on a Hilbert spaceX. It is well known that if R(T ) is infinite dimensional, then the problem of solving the above equation is ill-posed, in the sense that the generalized solutionxˆ:=Ty does not depend continuously on the datay. Here,Tis the generalized Moore- Penrose inverse ofT defined on the dense subspaceD(T):=R(T )+R(T ) ofX, andR(T )denotes the range of the operatorT. A typical example of such an ill-posed equation is the Fredholm integral equation of the first kind

b a

k(s, t )x(t )=y(s), asb, (1.2) withX=L2[a, b], andk(·,·)a nondegenerate kernel belonging toL2([a, b

[a, b]).

Copyright © 2001 Hindawi Publishing Corporation Abstract and Applied Analysis 6:6 (2001) 339–355

2000 Mathematics Subject Classification: 65J10, 65J20, 47L10 URL:http://aaa.hindawi.com/volume-6/S1085337501000653.html

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In a regularization method, corresponding to an inexact data y, one looks˜ for a stable approximation x˜ ofxˆ such that ˆx− ˜xis “small” whenever the data errory− ˜yis “small.” A well-studied class of regularization methods for such a purpose is characterized by a class of Borel functionsgα,α >0, defined on an interval(0, b]wherebT2. Corresponding to such functionsgα, the regularized solutions are defined by

xα:=gα

TT

Ty, x˜α:=gα

TT

Ty.˜ (1.3) (Cf. [1].) In order to perform error analysis, we impose certain conditions on the functionsgα,α >0. Two primary assumptions are the following.

Assumption 1. There existsν0>0 such that for everyν(0, ν0], there exists cν>0 such that

0≤λ≤bsup λν1−λgα(λ)cνανα >0. (1.4) Assumption 2. There existsd >0 such that

0≤supλb

λ1/2gα(λ)−1/2α >0. (1.5) These assumptions are general enough to include many regularization meth- ods such as the ones given below.

For applying our discrepancy principle, we would like to impose two addi- tional conditions.

Assumption 3. There existα0>0 andκ0>0 such that

1−λgα(λ)κ0αν0λ∈ [0, b],αα0. (1.6) Assumption 4. The functionf (α)=αq[1−λgα(λ)],q >0, as a function ofα, is continuous and differentiable andf (α)is an increasing function.

Now we list a few regularization methods which are special cases of the above procedure.

Tikhonov regularization

TT+αI

xα=Ty. (1.7)

Here

gα(λ)= 1

λ+α. (1.8)

Assumptions1,2,3, and4hold withν0=1, andκ0 inAssumption 3can be taken as greater than or equal to 1/(α0+T2).

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Generalized Tikhonov regularization TTq+1

+αq+1I xα=

TTq

Ty. (1.9)

Here

gα(λ)= λq

λq+αq+1. (1.10)

Assumptions 1, 2, 3, and 4 hold with ν0 = q+1, q ≥ −1/2, and κ0 in Assumption 3can be taken greater than or equal to 1/(αq0+1+T2(q+1)).

Iterated Tikhonov regularization.In this method, thekth iterated approximation xα(k)is calculated from

TT+αI

xα(i)=αxα(i−1)+Ty, i=1, . . . , k, (1.11) withxα(0)=0. Here, with

gα(λ)=1 λ

1− α

α+λ k

. (1.12)

Assumptions1,2,3, and4hold withν0=kand the constantκ0inAssumption 3 can be taken as any number greater than or equal to 1/(α0+T2)k.

In order to obtain numerical approximations ofx˜α=gα(TT )Ty, one may˜ have to replaceT by an approximation of it, say byTn, where(Tn)is a sequence of finite rank bounded operators which converges to T in some sense, and consider

˜

xα,n:=gα

TnTn

Tny˜ (1.13)

in place of x˜α. One of the well-considered finite rank approximations in the literature for the case of Tikhonov regularization is the projection method in whichTnis taken as eitherT PnorPT Pm, where for eachn∈N,Pn:XX is an orthogonal projection onto a finite-dimensional subspaceXn ofX.

In [4], Periverzev considered Tikhonov regularization, with Tn=P1T P22n+

n

k=1

P2kP2k1

T P22nk (1.14)

withR(P2k+1)R(P2k+1)and showed that the computational complexity for obtaining the solution

˜ xα,n:=

TnTn+αI−1

Tny˜ (1.15)

is far less than that for ordinary projection method whenT andTare having certainsmoothness propertiesand(Pn)is having certainapproximation prop- erties.

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Recently, Solodki˘ı [6] applied the above modified projection approxima- tion to the general regularization method, and obtained error estimate for the approximation

˜

xα,n=gα

TnTn

Tny˜ (1.16)

under an a priori choice of the regularization parameterα.

In this paper we not only consider the above class of regularization meth- ods defined byx˜α,n=gα(TnTn)Tny˜ withTn as in (1.14), but also consider a modified form of the generalized Arcangeli’s discrepancy principle

Tnx˜α,n− ˜f= δ+an

p

αq , p >0, q >0, (1.17) for choosing the regularization parameterα. Here(an)is a sequence of positive real numbers such thatan→0 asn→ ∞. It is to be mentioned that, in [3], the authors considered the above discrepancy principle for Tikhonov regularization withTnas in (1.14). The advantage of having a general sequence(an)instead of the traditional(n), whereTTn =O(n), is that the order of convergence of the approximation is in terms of powers ofδ+an, in place of powers ofδ+n

with an smaller thann. By properly choosing (an), it can happen that, for a smallδ, the values ofn for which an =O(δ), can be much smaller than that required forn=O(δ). In this paper we are going to use the estimateTTn = O(n),n =2nr, proved in [3], wherer >0 is a quantity depending on the smoothness property of T, and take (an) such that 2nr =O(anλ) for some λ >0. For instance one may takean=2nr/λ for anyλ(0,1].

In order to specify thesmoothness propertiesof the operatorT andapprox- imation propertyof(Pn), we adopt the following setting as in [3,4].

Forr >0, letXrbe a dense subspace of the Hilbert spaceXandLr:XrX a closed linear operator. OnXr consider the inner product

f, gr:= f, g+

Lrf, Lrg

, f, gXr, (1.18) and the corresponding norm

fr:= f+Lrf, fXr. (1.19) It can be seen that, with respect to the above inner product·,·r,Xris a Hilbert space.

IfA:XX,B :XrX,C:XXr are bounded operators, then we will denote their norms by

A, Br,0, C0,r, (1.20)

respectively.

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We assume thatT :XX is a compact operator having thesmoothness properties

R(T )Xr, R T

Xr, R LrT

Xr, (1.21) with

T :X−→Xr, T:X−→Xr, LrT

:X−→Xr (1.22) being bounded operators, so that there exist positive real numbersγ1, γ2, γ3such that

T0,rγ1, T

0,rγ2, LrT

0,rγ3. (1.23) Further, we assume that(Pn)is a sequence of orthogonal projections having theapproximation property

IPn

r,0crnr, (1.24)

wherecr>0 is independent ofn.

2. Error estimate and discrepancy principle

2.1. Error estimate. LetT :XXbe a compact operator having the smooth- ness properties specified by (1.21) and (1.23) and(Pn)a sequence of orthogonal projections having the approximation property (1.24). For eachn∈N, letTnbe defined by (1.14).

LetyR(T )andy˜∈Xbe such that

y− ˜yδ. (2.1)

Let{gα:α >0}be a set of Borel measurable functions defined on(0, b], where b≥max

T2,Tn2

n∈N, (2.2)

and satisfying Assumptions1,2,3, and4. Let ˆ

x:=Ty, xα:=gα

TT Ty, xα,n:=gα

TnTn

Tny, x˜α,n:=gα

TnTn

Tny.˜ (2.3) Further we assume thatxˆ∈R((TT )ν)for someν(0, ν0], and

ˆ x=

TTν

ˆ

u, uˆ∈X. (2.4)

In order to find an estimate for the error ˆx− ˜xα,n, first we observe that xˆ− ˜xα,nxˆ−xα,n+xα,n− ˜xα,n. (2.5)

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By the definition ofxα,n,x˜α,n, and using spectral results, we have xα,n− ˜xα,n=gα

TnTn

Tn y− ˜y

=Tngα

TnTn y− ˜y

. (2.6)

Therefore, usingAssumption 2ongα, we get xα,n− ˜xα,n=Tngα

TnTn y− ˜y

=TnTn1/2

gα

TnTn y− ˜y

≤ sup

0≤λb

λ1/2gα(λ)y− ˜yd δ

α.

(2.7)

Thus, we have

xˆ− ˜xα,nxˆ−xα,n+d δ

α. (2.8)

The following theorem supplies an estimate for ˆxxα,n. For its proof we will make use of the result

AAnaAAnmin{1,}, >0, (2.9) proved in [7] for positive, selfadjoint, bounded operatorsAandAn onX, with (An)uniformly bounded, wherea>0 is independent ofn.

Proposition2.1. Letxˆ andxα,nbe as in (2.3). Then xˆ−xα,nc

αν+TTTnTnmin{1,ν}+α−1/2TnP2nT

TTν. (2.10) Proof. We observe that

ˆ

xxα,n= ˆxgα

TnTn

TnTxˆ

= Igα

TnTn

TnTn

xˆ+gα

TnTn

Tn TTn

x,ˆ (2.11) so that

xˆ−xα,nIgα

TnTn

TnTn

xˆ+gα

TnTn

Tn TTn

xˆ. (2.12) Sincexˆ=(TT )νu,ˆ

Igα

TnTn

TnTn

xˆ=ITnTngα

TnTn

TTν

ˆ u

ITnTngα

TnTn

TTν

TnTn

ν ˆ u +ITnTngα

TnTn

TnTn

ν

ˆ u.

(2.13)

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Now, usingAssumption 1ongα, ITnTngα

TnTn

TnTn

ν

ˆ

u≤ sup

0<≤λ≤bλν1−λgα(λ)uˆ≤cνuˆαν, (2.14) and byAssumption 1ongαand the result (2.9) withA=TT,An=TnTnand =ν,

rα

TnTn

TTν

TnTn

ν ˆ urα

TnTnTTν

TnTn

νuˆ

c0uˆTTν

TnTn

ν

c0aνuˆTTTnTnmin{1,ν}.

(2.15) SinceTnP2n=Tn,xˆ=(TT )νuˆ and usingAssumption 2ongα, we have

gα

TnTn

Tn TnT

ˆ

x=gα

TnTn

Tn

TnP2nT ˆ x

=TnTn1/2

gα

TnTn

TnP2nT ˆ x

TnTn1/2

gα

TnTnTnP2nT TTν

ˆ u

duˆα−1/2TnP2nT

TTν.

(2.16) Using the above estimates for[Igα(TnTn)TnTn] ˆxandgα(TnTn)Tn(TTn)xˆin relation (2.12) we get the required result.

In view of relation (2.8) andProposition 2.1, we have to find estimates for the quantities

TT−TnTn, Tn−P2nT

TTν. (2.17) It is proved in [4] (also see [6]) that

TTTnTn=O 2−2nr

(2.18) so that

TTTnTnmin{1,ν}=O

2−2nrν1

, ν1=min{ν,1}. (2.19) Also, the estimate for(TnP2nT )(TT )νgiven in the following lemma can be deduced from a result of Solodki˘ı [6]. Here we will give an independent and detailed proof for the same. We will use the estimates

T

IPm=O mr

, T

IPm

0,r=O mr

(2.20) obtained by Pereverzev [4] (cf. also [3]) and the estimate

IPm

|T|=OT

IPmmin{,1}

, >0, (2.21) given in [5].

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Lemma2.2. Forν >0, TnP2nT

TTν=O

2nr(2+ν2)

, ν2=min{2ν,1}. (2.22) Proof. It can be seen that

P2nTTn=P1T

IP22n +

n

k=1

P2kP2k−1

T

IP22n−k

. (2.23) Therefore,

P2nTTn

TTν

T IP22n

TTν+

n

k=1

IP2k−1 T

IP22n−k

TTν

T

IP22nIP22n TTν +

n

k=1

I−P2k1

T

IP22nkIP22nk

TTν

T

IP22nIP22n

TTν +

n

k=1

IP2k−1

r,0T

IP22n−k

0,rIP22n−k

TTν. (2.24) Now using (1.24), (2.20), and (2.21), it follows that

P2nTTn

TTν

κ12−2nr

2−2nrmin{2ν,1}

+κ2

n k=1

2(k−1)r2(2nk)r

2(2nk)rmin{2ν,1}

κ22nr22nrν2

n

k=0

2krν2, ν2=min{2ν,1},

=O

2nr(2+ν2) .

(2.25)

Thus the lemma is proved.

Now, the estimates in (2.19) and (2.22) together with Proposition 2.1 and relation (2.8) gives the following result.

Theorem2.3. Suppose thatxˆ∈R((TT )ν)andyR(T ). Then xˆ− ˜xα,nc

αν+2−2nrν1+2nr(2+ν2)

α + δ

α

, (2.26)

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where

ν1=min{ν,1}, ν2=min{2ν,1}. (2.27) 2.2. Discrepancy principle. We consider the discrepancy principle

Tnx˜α,n− ˜y= δ+an

p

αq , p >0, q >0, (2.28) where(an)is a sequence of positive reals such thatan→0 asn→0.

Let

fn

α,y˜

=αqTnx˜α,n− ˜y. (2.29) We observe that

Tnx˜α,n− ˜y= TnTngα

TnTn

I

˜

y. (2.30)

Hence, by Assumptions1and3ongα,α >0, and using spectral theory, we have Tnx˜α,n− ˜y=TnTngα

TnTn

I

˜

y≤ sup

0<λb

1−λgα(λ)y˜≤c0, Tnx˜α,n− ˜y2=TnTngα

TnTn

I

˜ y2=

b 0

1−λgα(λ)2

dEλy˜2

b 0

κ0αν02

dEλy˜2

κ0αν0y˜2.

(2.31) Therefore, it follows that

αlim→0fn

α,y˜

=0, lim

α→∞fn

α,y˜

= ∞. (2.32)

Hence by the intermediate value theorem andAssumption 4on{gα}, there exists a uniqueαsatisfying the discrepancy principle (2.28). It also follows that

δ+an

p

αq =Tnx˜α,n− ˜yκ0αν0y˜ (2.33) so that

α=O δ+an

p/(q+ν0)

. (2.34)

For the next result we make use of the estimate TTn=O

2−nr

(2.35) proved in [3].

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Proposition2.4. Suppose thatxˆ∈R(TT )ν for someν with0< νν0,(an) is such that2nr =O(anλ)for someλ >0andα is chosen according to the discrepancy principle (2.28). Then

δ+an

p

αq =O δ+an

s

, (2.36)

where

s=min

1, λ,

q+ν0, p 2

q+ν0+2λν2

, ν2=min{v,1}, ω=min

v+1

2, ν0

.

(2.37)

Proof. From the discrepancy principle (2.28) we have δ+an

p

αq =Tnx˜α,n− ˜y=Igα

TnTn TnTn

˜ y

=Igα

TnTn TnTn

y+Igα

TnTn TnTn

˜ yy.

(2.38) We observe that

Igα

TnTn TnTn

y=Igα

TnTn TnTn

TTn

xˆ +Igα

TnTn TnTn

Tnxˆ

=ITnTngα

TnTn TTn

xˆ +ITnTngα

TnTn Tnxˆ.

(2.39)

Now, using the fact thatxˆ=(TT )νu,ˆ Assumption 1ongα,α >0, and spectral results, we have

ITnTngα

TnTn

Tnxˆ=TnTn

1/2

ITnTngα

TnTn

TTν

ˆ u

=TnTn

1/2

ITnTngα

TnTn

TnTn

ν

ˆ u +TnTn

1/2

ITnTngα

TnTn

× TTν

TnTn

ν ˆ u

≤ ˆcναωuˆ+c1/2α1/2uˆTTν

TnTn

ν, (2.40) where cˆν = cν+1/2 if ν+1/2≤ν0 and cˆν =cν0 if ν+1/2≥ν0, and ω = min{ν+1/2, ν0}. Hence

Igα

TnTn TnTn

yc0TTn

xˆ+cναωuˆ +c1/2α1/2uˆTTν

TnTn

ν. (2.41)

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Also, we have

Igα

TnTn TnTn

˜

yyc0δ. (2.42)

Thus

δ+an

p

αqc0TTn

xˆ+cναωuˆ+c1/2α1/2uˆ

×TTν

TnTn

ν+c0δ.

(2.43)

Now by the results (2.9), (2.34), (2.35), and the assumption that 2nr=O(aλn), we have

δ+an

p

αqc

anλ+αω+α1/2an2λν2+δ

c δ+an

λ

+αω+α1/2 δ+an

2λν2+ δ+an

c δ+an

λ

+ δ+an

pω/(q+νo)

+ δ+an

(p/2(q+ν0))+2λν2+ δ+an

,

(2.44)

whereν2=min{ν,1},ω=min{ν+1/2, νo}. Thus δ+an

p

αq =O δ+an

s , s=min

1, λ, p 2

q+ν0+2λν2, q+ν0

.

(2.45) Theorem2.5. In addition to the assumptions inProposition 2.4, suppose that

p < s+2qmin 1, λ

2+ν2

, (2.46)

where

s=min

1, λ, q+ν0

, p

2

q+ν0+2λν2

, ω=min

v+1

2, ν0

, ν1=min{ν,1}, ν2=min{2ν,1}.

(2.47)

Then

µ:=min

q+ν0

,1p 2q+ s

2q, λ 2+ν2

p 2q+ s

2q

>0, xˆ− ˜xα,n=O

δ+an

µ .

(2.48)

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Proof. Clearly,ps+2qmin{1, λ(2+ν2)}impliesµ >0. Now to obtain the estimate for ˆx− ˜xα,n, first we recall fromTheorem 2.3that

xˆ− ˜xα,nc

αν+2−2nrν1+2nr(2+ν2)

α + δ

α

. (2.49)

Now, using the assumption that 2nr =O(anλ)for some λ >0, and relation (2.34), we have

xˆ− ˜xα,nc δ+an

pν/(q+ν0)

+an2λν1+anλ(2+ν2)

α + δ

α

c δ+an

pν/(q+ν0)

+ δ+an

2λν1+ δ+an

λ(2+ν2)

α +δ+an

α

. (2.50) Since

δ+an

α = δ+an

p/2q δ+an

p

αq

1/2q

(2.51) for any >0, byProposition 2.4,

δ+an

α =O δ+an

1−(p/2q)+(s/2q) , δ+an

λ(2+ν2)

α =O δ+an

λ(2+ν2)(p/2q)+(s/2q) .

(2.52)

Thus xˆ− ˜xα,n=O

δ+an

µ

. (2.53)

The following corollary whose proof is immediate from the above theorem, specifies a condition required to be satisfied by λ, and there by the sequence (an), so as to yield a somewhat realistic error estimate.

Corollary2.6. In addition to the assumption inTheorem 2.5, supposeλ, p, q are such that

p q+ν0max

ν0,1

2

λ≤1. (2.54)

ThensandµinTheorem 2.5are given by s=

q+ν0, µ=min

q+ν0,1− p 2

q+ν0

1+ν0ω q

. (2.55)

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In particular, withλas above, we have the following:

µ=

q+ν0 whenever p

q+ν0 ≤ 2

2ν+1+0ω)/q, (2.56) µ= 2ν

2ν+1 whenever p

q+ν0 = 2

2ν+1, ν0−1

2≤νν0, (2.57) µ= 2ν

0+1 whenever p

q+ν0 = 2

0+1, q≥1

2. (2.58)

We may observe that the result in (2.58) ofCorollary 2.6shows that the choice ofp,q in the discrepancy principle (2.28) does not depend on the smoothness of the unknown solutionx. Also, from the above corollary we can infer that forˆ the Arcangeli’s discrepancy principle

Tnx˜α,n− ˜y= δ+an

α , (2.59)

one obtains the error estimate xˆ− ˜xα,n=O

δ+an

µ

, µ= 2ν

0+1, (2.60) provided(an)satisfies

2nr=O aλn

, max

00+1,1

2

λ≤1. (2.61) In particular, for Tikhonov regularization, where ν0 =1, we have the order O((δ+an)2ν/3)whenever 2/3≤λ≤1.

3. Numerical example

In this section, we carry out some numerical experiments using JAVA program- ming for Tikhonov regularization, and implement our discrepancy principle. We also implement the a priori parameter choice strategy numerically.

Consider the Hilbert spaceX =Y =L2[0,1] with the Haar orthonormal basis {e1, e2, . . . ,}, of piecewise constant functions, where e1(t ) =1 for all t∈ [0,1], and form=2k−1+j,k=1,2, . . .,j=1,2, . . . ,2k−1,

em(t )=



















2(k−1)/2 iftj−1

2k1,j−1/2 2k1

,

−2(k−1)/2 ift

j−1/2 2k−1 , j

2k−1

,

0 ift

j−1 2k−1, j

2k−1

.

(3.1)

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LetT :XXbe the integral operator, (T x)(s)=

1

0

k(s, t )x(t ) dt, s∈ [0,1], (3.2) with the kernel

k(s, t )=

t (1s), ts,

s(1t ), t > s. (3.3) We take Xr with r =1 as the Sobolev space of functionsf with derivative fL2[0,1]. In all the following examples, we have xˆ ∈R((TT )ν) with 2ν≤1. In this case the error estimate inTheorem 2.3takes the form

xˆ− ˜xα,nc

αν+2−2nν+2−2n(1+ν)

α + δ

α

. (3.4)

Taking the a priori choice of the parameterαas

α∼2−2n, αδ2/(2ν+1), (3.5)

we get the optimal order

xˆ− ˜xα,n=O

δ2ν/(2ν+1)

. (3.6)

In a posteriori case, we findαusing Newton-Raphson method, namely αk+1=αkg

αk

g

αk

, k=0,1, . . . , (3.7) where

g(α)=α2q

¯

xTMCx¯−2x¯TCB+

˜ y,y˜

δ+an

2p

, g(α)=2qα2q−1

¯

xTMCx¯−2x¯TCB+

˜ y,y˜

α2q

¯

xTMC(α+M)−1x¯− ¯xT+M)−1MCx¯−2x¯T+M)−1CB , (3.8) with

¯ x=

x1, x2, . . . , xm

, [B]i=

ei,y˜

, i=1,2, . . . , m, [M]ij =

2nν

r=1

ei, Aer

ej, Aer

, i, j=1,2, . . . ,2n, [C]ij =

φi, φj

, φ1=P22nTe1, φi=P22nTei, i

2−1,2

, =1,2, . . . , n.

(3.9)

(15)

Here we used the notation[A]ij for theijth entry of ann×nmatrixAand[B]i

for theith entry of ann×1 (column) matrixB.

In the following examples, we take the perturbed datay˜ as

˜

y(s)=y(s)+δ, 0≤s≤1. (3.10)

For the a posteriori case, we takepandqsuch thatp/(q+1)=2/3, andan= (2n)1/λ withλ=2/3. As per Corollary 2.6, the rate is O((δ+an)pν/(q+1)).

We will use the notatione˜α,nfor the computed value of ˆx− ˜xα,n.

Example 3.1. Lety(s)=(1/6)(ss3). In this case, it can be seen thatx(t )ˆ =t, t∈ [0,1]. It is known (cf. [2]) thatxˆ∈R(TT )νfor allν <1/8. In the following two cases we takeν=1/9.

A priori case

δ n m e˜α,n δ+1 e˜α,n+1

2 4 0.9059731 0.7371346 1.229047

21.22n 3 8 0.7722685 0.6328782 1.220248

4 16 0.4068352 0.5433674 0.7487295

A posteriori case

p,q δ n m e˜α,n +an)

q+1 e˜α,n.(δ+an)

q+1

p=1 q=1/2

2 4 0.5102194 0.89450734 0.5703915 21.22n 3 8 0.4890685 0.8196771 0.5966605 4 16 0.3504178 0.7517244 0.4661520

p=2 q=2

2 4 0.4000930 0.89450734 0.4482135 21.22n 3 8 0.3664487 0.8196771 0.4470647 4 16 0.3294871 0.7517244 0.43830837

p=1 q=1/2

2 4 0.5754841 0.8414794 0.6838956 1010 3 8 0.5430453 0.7719075 0.7035708 4 16 0.2975858 0.7187710 0.4202669

p=2 q=2

2 4 0.5395960 0.8414794 0.6412471 1010 3 8 0.4648603 0.7719075 0.6022228 4 16 0.28503888 0.7187710 0.3965642

Example 3.2. Lety(s)=(1/24)(s2s3+s4). In this case,x(t )ˆ =(1/2)(tt3),t∈ [0,1] andxˆR(TT )ν for allν <5/8 (cf. [2]).

参照

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