U.S.S.R. Comput. MathsMath. Phys. Vol. 18, pp, 236-242 0 Pergamon Press Ltd. 1979. Printed in Great Britain.
0041-5553/78/0601-0236$07.50/O
THE OPTIMAL APPROXIMATION OF NON-LINEAR OPERATORS* A. I. GREBENNIKOV
Moscow (Received 24 December 1976; revised 13 April 1977)
THE OPTIMALITYin respect of order of the methods of interpolating for the approximation
of the values of an arbitrary non-linear
and regularized splines
operator is proved for discrete
initial data. 1. Many applied problems may be formulated the values of some (possibly unbounded
mathematically
as a problem of calculating
operator B, acting from the Hilbert
and non-linear)
space H into the linear normed space I’. The initial data about the elements B is calculated
are as a rule specified as a collection
linear functionals
2, . . . , m,
Zi, i=l,
the approximate
fi=li(U)
We introduce
values
of values
f;, i=l,
UEH,
2, . . . , m,
on which of some
on these elements. Here instead of the exact values f[=l, (u)+gi,
where the ti are errors, are often given.
the operator Au=(Z,(o),...,1,(u)),
acting from H into the m-dimensional
Euclidean space F.
UEM~={UED:IILUII~~R},
We will assume that
O
< +m,
where L is a linear operator acting from H into the Hilbert space G and
D&D=D,IlD,.
We write f= (fir . . 1 fm),
f= VI, .--1 t),
E=(E1, ..-,
Em).
We define the set of exact initial data as the set Nw={f=Au,
and the set of approximate
initial data, as Na, R=(f~F:
Here the number
6>0
UEMR),
r=Au+g,
ucM,,
Ilgk6).
describes the accuracy of definition
The problem of calculating
of the elements
f=NR.
the values of the operator B on these assumptions
is ill-posed [ 1] .
There is considerable interest in methods of solving ill-posed problems which are in some sense optimal. For linear problems the questions of the construction of optimal methods have been fairly fully studied (see, for example, [2,3] ), but non-linear problems have been investigated to a lesser extent. Here we must mention the paper of V. P. Tanana [4] , where for the case of the solution of a non-linear equation of the first kind with an approximate right side the optimality in respect of order of the method of discrepancy and the method of quasi-solutions of V. K. Ivanov [S] was proved. *Zh_ @hid.
Mat. mat. Fiz., 18, 3, 762-766, 1978.
236
237
Short communicdons
The problem considered below differs in the fact that the operator B calculated is regarded as non-linear,
and the initial information
is specified by a linear operator A. This leads to a
position where the element on which the calculation
of the value of the operator B gives the least
error (in respect of order), belongs to a linear space of interpolating and regularizing (in the case of approximate data) splines. In the case of approximate
data this paper investigates the optimal properties of Tikhonov’s
therefore as in [3] , a relative error of approximation
method of regularization, regularization
parameter is chosen. The introduction
enabled us, when considering prior information,
optimization
criteria
problems, not to require the existence of quantitative etc, and to manage with only qualitative
prior
that is, knowledge of the operators A and L. This made it possible to reduce the
problem of optimization
for different initial data to the choice of the regularization
On the other hand the introduction due to the fairly complex structure definition
depending on the
of a parameter in the optimality
such as, for example, the level of error of the input data or the constant
occurring in the method of quasi-solutions information,
(in the case of exact data)
of the traditionally
parameter.
of this relative error enabled us to avoid dif~culties
of the sets of admissible elements, which participate
in the
used error [2] , since in the proposed approach the admissible
elements vary in a linear set D, which facilitates the investigation. Efficient ~go~thms
for the numerical
realization
of the optimal order methods indicated
in this paper are given, for example, in [6]. 2. Let
6=0,
that is, the input information
is specified exactly.
U,(j) ={u=.UR:
We introduce
the set
Au=/)
for some fixed vector f= NR, and let T be an arbitrary operator defined on A [D] , acting in V. The error in calculating the value of the operator B for the data vector fby means of the operator T is described by the quantity
and on the whole set NR by the quantity
Problems of finding optimal operators from the condition all-possible admissible operators constructed
T were formulated
of the minimum
of these errors for
in [3] and such optimal operators were
for a linear B.
For an arbitrary non-linear
operator B the construction
of optimal operators is difficult.
However, operators optimal in respect of order can be indicated,
that is, operators for which the
error differs from the optimal by some constant. Let U(f)={u4: Au=f}, element USED such that
fEA[D].
IlLufllci =
We consider an auxiliary problem:
inf IILuIIc. UGU(i)
find the
238
A. I. tirebennikov
It is assumed that problem (1) has a unique solution (conditions on A [D] , and also on
for example, in [2] ). Consequently, operator
S : Sf=u,,
sufficient
Y,rA[D]
for this are indicated, the linear bounded
is defined.
Theorem I
made the operator To = BS is of optimal order, the following estimates
With the assumptions being valid:
2oonT(B) a 0s CR,To) 2 wm (B) = sup OonT(B, f).
(3)
f=NR Proof:
For any
u=U,(f)
T the following inequalities
and arbitrary
T, f))
a(& ) -
1 2
max{llBu-Tfllv,
{IPJJ-Tfllv
hold:
Wf-Tfllv) (4)
1
+II~f-~urIIv)~
- 2 IIBU-%fllv,
from which the left side of (2) follows. The right side of (2) is obvious. If in the series of inequalities and then with respect to fEivR, (4) we take the exact upper bound first with respect to u=UR(f), we obtain (3). The theorem is proved. 3. For a rather different choice of the error and the supplementary operator to be approximated
conditions
on the
it is possible to indicate an optimal algorithm of approximation
of
the values of the operator B. Let P be an arbitrary operator defined on the space F, acting in D. The error in calculating the value of the operator B for the data vector fis described by the quantity sup IlB(u-Pf)
P, f) =
aB(&
IIT’,
U-=UB(f)
and on the whole set NR by the quantity &, (R, P) = sup GE @, p, f)
.
fENR We
say that the operator
&
isf-optimal if GB(R, PO,f) = inf i;iS @, P, f) = h CRY f),
P
and we say that the operator PO is NR -optimal if
where inf is taken over all-possible operators P. We introduce
the set UB={u=MR:
Au=O}.
(5)
239
Short communications
We write WE(B) = sup IlBullv. UECJR Theorem 2 If the operator B is antisymmetric,
that is,
B(-u)
then the operator
PO=S,
=-Bu
BED,,
is NB -optimal, where &%z)
If, in addition,
(7)
03)
=aB@).
the relation
$
G
holds, then the same operator S is f-optimal,
vui, UZEDB,
IIBui+Buzllv
(9)
where
GJB (R, f) =
sup
IIB(a-@)
(10)
IV-
u=.un(f)
Proof:
element
The properties of interpolating (2uf-U)
splines imply that for any element
also belongs to the set &y).
Also, for any
ud,(f)
u=U,(f) and arbitrary
the f=NR
we have the obvious inequality &(R,
P, f)>max
By relations (7) and (9) for any
{IIB(2ur--u--Pf)IIv,
IIB(u---Pf)Ilv}.
(11)
and any permissible operator P we have the
u~lJ,(f)
inequalities Ilv+liB(u-Pf)
2IIB(u,-U) Il6llB(2r~~-~-Pf)
llv, IIB(u-W)
~2 max {llB(2u,-zz-Pf) From these inequalities
and (11) by the arbitrariness
~B(R,
p,
f) 3
sup
of
IIv
IV).
u= U,(f)
IIB(u-Sf) Ilv.
we obtain the inequality
02)
u=Un(f)
Here equality in (12) is attained for P = S, and this implies that the solution of problem (5) is the operator PO = S, and Eq. (10) follows. For any u=Uv,(f) and arbitrary j=NR by the properties of interpolating splines the element (uf-u) =UR. From this and Theorem 1 of [3] there follow relations valid for operators B satisfying only condition (7):
A. I. Grebennikov
240
liJ,(I?,P)~
sup IIB(u-Uj)IlV. ~ENRUEURU)
WB(R)~ sup
The extreme terms in (13) are identical for P = S,and accordingly, from (13). The theorem is proved.
&=S.
(13) Equation (8) follows
We give an example of non-linear operators satisfying the relations (7) and (9). Let H=Wik) then conditions (7) and (9) are satisfied by the operators la, bl, V=LIa, bl, B*(z)= (J.C$) onlyfor
where (2~I)<0
2”-‘,
u(~)(I)+O
n=O, *i,
and
*2,. . . ,
k=O, 1,. . . ,
~=[a, b].
4. In the case of approximate data, for DO, we consider an approach to the problem of optimizing the calculation of the values of the operator B, based on A. N. Tikhonov’s method of regularization [ 1 ] . For any
UEF, h>O
we define the functional @Au, vl=~IIAu--vll~~+IILullc~,
and consider the auxiliary problem: find an element
U&ED
u=D,
such that
(14)
It is assumed that this problem has a unique solution uh for any hr0 &: &v=u~ED is defined. Thereby for all v=F the linear operator
and
u=F.
We specify the non-empty set NcF. We defme the measure of approximation of the operator B at the point v=N by the quantity OS&; T, 0) = sup {IIBU-T4lv/uAu, UED
VI),
and on the whole set N by the quantity os(h; T) =
sup OB(h; T, 0). USN
Here and below we regard as admissible the operator T defined on the whole set N and acting in K We write OF (h; u)= inf os(h; T, v), T
WF (h) = inf oB(li; T), T
where inf is taken over all admissible operators. l%eorem 3 The operator
TL=BS1.
is of optimal order, and the following relations are satisfied:
241
Short communications
ProoJ: For any u=D, u=N and arbitrary T the following inequalities are satisfied:
which imply the left sides of inequalities (15). The right sides of these inequalities are trivial. The theorem is proved. The chosen errors of approximation of the operator B depend on the parameter A, whose introductjon permitted us to reduce the problem of constructing the optimal appro~mating operator for various initial data to the choice of a suitable value of the parameter X depending on the initial data of the specific problem. 5. As the set N let the set be specified. We denote by i?j, the solution of Na. R. problem (14) corresponding to the parameter il=h (6, r), chosen from the conditions of the discrepancy jMn,--fib,=6 (see [2] )_We write
CO:’ (6, R, f) = inf COB (6, R, T, f), T Theorem
wyT (6, R) = inf og(6, R, T). P
4
The operator
TAta,y)=Ti
is of optimal order, the following relations holding:
2@;==(8, R, f) 2 eM6, R, TA,f) 3 O? (6, R, f,, 2m”B”’(S,fR)>
sup
on (6, R, FL, f) ,, OF (8, R).
f-EN&. R
The proof of this theorem essentially repeats the proof of Theorem 3. 6. We note that the operators To and 7j constructed have the structure To=BS, T1=BSI., where the operators S and fi are independent of the approximate operator B, and are completely determined by the operators A and L. Thereby the optimal properties of these operators are preserved for the class of problems, that is, for ah-possible permissible operators B. When the condition of B-complementarity is satisfied the convergence of the optimal order methods presented can be investigated as in [2]. Translated by J. Berry.
242
Yu. L. Gaponenko REFERENCES
1.
TIKHONOV, A. N. The solution of ill-posed problems and a method of regularization. Dokl. Akad. Nauk SSSR, 151,3,501-504,1963.
2.
MOROZOV, V. A. Regular methods of solving ill-posedproblems (Regulyamye metody resheniya nekorrektno postavlennykh zadach), Izd-vo MGU, Moscow, 1974.
3.
MOROZOV, V. A. and GREBENNIKOV, A. I. The optimal approximation Nauk SSSR, 223,6,1307-1310,1975.
4.
TANANA, V. P. Optimal methods of solving non-linear unstable problems. Dokl. Akad. Nauk SSSR, 200, 5,1035-1037,1975.
5.
IVANOV, V. K. and KOROLYUK, T. I. Error estimates for solutions of i&posed problems. Zh. vj@hisl. Mat. mat. Fiz., 9,1,30-40,1969.
6.
LORAN, P. Zh. Approximation and optimization (Approksimatsiya
US.S.R. Comput. Maths Math. Phys. Vol. 18, pp. 242-245 0 Pergamon Press Ltd. 1979. Printed in Great Britain.
of operators. Dokl. Akad.
i optimizatsiya),
“Mir”, Moscow, 1975.
0041-5553/78/0601-0242$07.50/O
THE METHOD OF CONSISTENT APPROXIMATION FOR SOLVING NON-LINEAR OPERATOR EQUATIONS* Yu . L. GAPONENKO
Moscow (Received 16 July 1976) A NEW REGULARIZATION method is proposed for the approximate solution of non-linear equations. The method is based on the well-known idea of the construction of a compact set. As regularization parameter a mesh step compulsorily consistent with the error of the initial data is used. The method guarantees uniform convergence to the exact solution of the class in the one-dimensional and two-dimensional cases. Operator equations of the first kind constitute an important class of ill-posed problems. The problem of constructing an approximate solution of an ill-posed equation for approximate initial data can be solved by the methods of the theory of regularization (see, for example, [l-7]). In this paper a regularization method for the approximate solution of non-linear equations is presented. 1. Statement of the problem
We consider the operator equation Av=f,
(1)
where A is a continuous operator acting from the space C[O, I] into the space L2 [0, I] . We will assume that Eq. (1) has a unique solution u(z) 43 ‘10, 11 and that for the operator A the prior estimate lIAv-Awll~6l(llv-wl~o,
max(llvllo,
Il~llo));
(2)
is known, here Il.li and ll.lk-~denote the norms in the metrics of L2 [0,l] and C[O, l] respectively, satisfying and Q(t, R) denotes a non-negative continuous function, O