SOME ESTIMATESOF THE RATE OF CONVERGENCE OF REGULARIZED APPROXIMATIONSFOR EQUATIONS OF THE CONVOLUTION TYPE* A.V.
GONCHARSKII,
A, S. LEONOV and A, G. YAGOLA Moscow
(Received 21 May 1971; revised
A NEW mathod of obtaining
estimates
version
27 July 1971)
of the rate of convergence
of regularized
approximations to the exact solution for one-dimensional Fredholm integral equations of the first kind of the convolution type is proposed. The method is based
on a study
transform
of the behaviour
of the kernel
hood of its zeros We consider
of the square
of an integral
equation
of the modulus at infinity
of the Fourier
and in the neighbour-
on the real axis. the Fredholm
integral
equation
of the first kind of the convolu-
tion type +*
K(s-@z(s)& = a(s), -cQ
44[x9g(s)1 =
(1)
which is often encountered Let the functions
occurring
K(v) &Li(&f7 Also, to some function
equation
(I), the function
information
in applications. in the equation
u (5) =
L2 (Ed
2 (s)
Usually
u (x) itself,
u6 (3~)such that
Mat. mat. Fiz., 12, 3. 762-770, 1972.
243
the requirements
W2’
(Ed).
a unique
in the treatment
llu(t) - Q(s) I/tz =C 6.
+ Zh. vychisl.
E
u (x) let there correspond z (s).
we know not the function
it, a function
9
satisfy
solution
of
of experimental
but some &approximation
of
V. Goncharskii,
A.
244
We
consider
the Tikhonov
A. S. Leonov
functional
and A. G. Yagola
[l]
In [2] it is shown that for any a > 0 there exists realizing the minimum of the functional
a unique
way that 6’ /a (6) + 0, the sequence
z6* (6) (s) converges
solution
and it follows
of (l), in the norm W,‘(E,),
[3] that the convergence
element
zsa (s)
(4), and if C-I (8) -, 0 as S + 0 in such a
of the approximate
to z (s), the exact
from the imbedding
to the exact
solution
theorem
is uniform.
Moreover, if we consider the functional Ma [z, u], we can find a unique function za (s) on which the minimum of Ma [z, u] is realized for a fixed a > 0, where za (s) -+ z (s) as a + 0 [l, 21. After using the convolution theorem, Plancherel’s equation 141 and varying the functionals Ma [a, u,], Ma [z, U] on a set of functions of Wll, we obtain that the minimum of the functional Ma [z, u,] is attained on the function E.51
(3)
i +-.r(O)E*(W)et@* do ZIP(0) = zft s L(o)+ a(d + 1) ’ -LI1
and the minimum of the functional i
(4)
z”(s)
=
-
(0) fj (a)
2% f_,Lfti)+
where K’(o) = X(-u,)), f(w) are the Fourier We also notice
+-r
Ma [z,
ul on
the function
eisr do
No2 + 4) ’
L(W) = ]ff(a) 1’ -Ill(w)I transforms of the functions
and K(O), aa(
g(w),
K(Y), r&(z), u(z), Z(t).
that (1) implies
(5) We consider the question of the rate of convergence of the regularized approximation to the exact solution of (I). As will be shown below, the estimates of the rate of convergence depend essentially on the behaviour of the square of the modulus of the Fourier transform of the kernel at infinity and in the neighbourhoods of its zeros on the real o-axis. Very interesting estimates of the rate of convergence, based on a study of the behaviour of the Fourier
transform of the kernel at infinity, and also on the behaviour of the function in the denominator of (3) in the neighbourhoods of its zeros in the complex o-plane, were obtained in [5-71. The method of obtaining the rate of convergence
of the rate of convergence
Some estimates
presented
below is simpler
15-71 and enables
than the method of obtaining
estimates
of this type to he obtained
estimates
245
explained
for more complex
in
classes
of kernels. Usually z$‘)
(s)
particular,
the interest to the exact
is in estimating solution
such estimates
the accuracy
of the approximation
.z (s) in the norm of some Banach
will be obtained
below for the spaces
space
B.
of In
C and t,.
It is easy to see that the inequality
s.slb(s) -z=ts)IIrJ + W(S) - ZP(S)Ils.
llz(s) -zaa(s)Ils
(6) holds.
It follows
from (S), (6) that-
J L(o)+ a(02 +1)’ -m ~a(~)~ef~n~~ 1*Y?rfo)[s(W)(s) - Z&U (s) =--g (8) za J L(o)+a(w2+~) * +OD(02 + l)P(o)ei”* do
(7)
za (s) = ;
z(s)-
It remains to estimate (7) and;;) as functions of a and 6. We show that for the assumptions formulated above the following estimates hold (see 18, 91) (9)
8 lfZ=(s) - za=(s) ilL*< -3 l’a
(f0)
112&(s)-
6
1
ZP(S)Ilc f --.
ya
1’2
We use Plancherel’s
theorem: 1
(11)
llP(s)-
-
z8ys)llt,2= (24’
+II
H”(w)[E@)-
J _m
L(o)+
1 +~~(o)K(~)]~(~)-~a(~)I'~
2x 5 -0D
[L(o)+
a(02 + ill”
=G
u”g(@l)]e*‘b* do a(02 + 1)
a =
II L2
A. V. Goncharskii,
A. S. Leonov
and A. G. Yagola
Here we have used the fact that
estimate
(9) follows
from (11).
Also,
Using
(12) and Plancherel’s
We notice independent
We estimate 14(w) I
that the estimates
of the exact
solution
theorem,
we obtain
obtained
depend
(7) in the metric of the space
C.
from (7) we obtain OD(CO2 + 1) ff(w) [do
Ilz(s)-- z”(s)/lc f
”3x s
0
We partition
the last integral
It is easy to obtain (15)
We now obtain
L(o) +c@+11’ into two:
a lower bound for T(a>:
I(a) 3 const a.
an upper bound:
only on 8 and a but are
z (s). Because
of the evenness
of
of the rate of convergence
Some estimates
247
where
‘la
dp(o)
since
< +ofh
12do
z(t) E W2i. We obtain
an estimate
about the Fourier
for I,.
transform
(1) Uo) = IRW I” there are no zeros
Here we will make the following
assumptions
of the kernel: has a countable
or a finite
number
number of zeros
of them the estimate
on the real w-axis obtained
remains
8(if
all
the more valid); (2) there exists of the function L(0)
where
of non-intersecting
3
fZi(CO~-W)2P,
OE
(3) outside
of the i-th c-neighbourhood
the +neighbourhoods
L(O) >,
(4) points exception,
Azc.+,
of condensation
perhaps,
k > 0,
~-neighbourho~s
Ei, Oi + Ei],
are the zeros
of L (w), i = 1, 2,. . . ;
(the point w = 0 is considered
indicated AZ > 0;
of the zeros
of L (0) do not exist
(with the
of w = + -), and if N (MM> is the number of zeros
Ml,
(the case
of the zeros
w 2 0 such that
[a-
ai > a = const > 0, p > ‘14, WI> 0
ci is the radius separately);
(0,
a system
L (0) on the real semiaxis
y = 0 corresponds
to a finite
number
of zeros).
of L (w) on
248
A. V. Goncharskii,
These
constraints
of kernels
A. S. Leonou
are not too stringent,
encountered
in applications
and A. G. Yagola
and there exist
which satisfy
fairly wide classes
the requirements
formulated,
for example, sin29 mo
L(0) =
u2r
We now estimate
m = cone_
’
12(o) Ido =a2-t6oL(o)+a(u2+1)
>
1
etc.
o’-e’(~2+1) II(o) Ido
1)
{J
J
+
e, L(o)+a(a’+l)
0
N(M)
r
I,: (d+
Ii
(17)
CI >
ol+at
L(o)+ a(02 +1) (o2
+
1)
If(&))
Ido
J
N(M)-’
“i+‘-‘i+‘(02
+
CJ t=I Cli-ei
Z
i=i
Oifei
+
1)
+
If(o)
I&l
L(o)+a.(d+1)
+
M
to2 + 1) I:(o) Ido
I:” + I:” + I:“’ + I:“’ + I:“‘.
G
J L(o)+ ~(N)P(N)M For I(:)
a(o2 + 1) >
we obtain ai+i-et+r
“l+,-cl+r
(02 + 1) 12(o) Ido
(18)
a
GJ oi+L1 L(o)+ a(a2 + 1) 2%
+
J
(02 + i) I?(O) I&l -< A20-k
@l+=l
Ido = J ok+2lz’(o)
al+b-ei+l
2
3
1
I+ min(wi + ( i ui+l-Fitl UA3
-J3t
ok+*li(o)
6)’
)
Of+81
AS = convt > 0,
Ido,
mitEi
since
(1%
69 + 1 < (I+
min(oi +
Ei)-2)W2
i
(here we have used the property It follows
from (18) that
(3)).
=
P02,
!2 =
const > 0
Some estimates
from which,
Similarly,
using
the Cauchy
249
of the rate of convergence
inequality,
we obtain
for 1i2) (or {,‘I’ + f:‘)n if L (0) f 0) we obtain
where
It is also obvious fi3).
that the estimate
For convenience
we write n = l/a*
and (19), we obtain
We use the Cauchy
(20) is also valid for 1:).
inequality
Then taking
We will estimate
into account
property
(2)
250
A.
From (21)-(23)
Similarly,
it follows
A. S. Leonov and A. G. Yagola
that
if L (0) = 0,
I:” g Finally,
V. Goncharskii,
A,allQ
A, = const > 0.
,
for I, we obtain
(24)
Hence from (14), (16) and (24) we have
$ +A,abW%
l(a)< As =
Using
const > 0.
(4) and introducing
-!k ‘)‘M + (A
‘(u)<
Minimizing smallness, (25)
+ Da ll*hltN (M) + Bia + AIaLlhp,
4 +
with respect
r = max{k + *lzlv),
Bai14P)Mr+i + AIa’/‘P + Bia,
to M and discarding
we arrive at an estimate lIza(s) -
where 0 depends
2
(s) IIc &
I (a) =
A,B=const>O.
terms of a higher order of
of the rate of convergence 0{a114~~~2r+3)),
on z, K, CU,~1, 01, a, r, k, P.
It is thereby proved that when conditions estimate (25) holds for (7). We estimate integral
we obtain
(7) in the metric of the space
I(a) =llz(s)-
za(s)llLa2
=
S
(l)-(4)
L,.
are satisfied
the uniform
We now denote
by I (a) the
(02 + i)Zjf(o)
J 0
[L(o)+
ato’+
I’&0 1)12’
*
251
of convergence
Some estimates of the fate
As for (15) we find (Z(i)
f(a) 3 con& u2. For an upper bound of I(a) we will suppose
(4) are satisfied.
We also require
We partition
(l)-
that
F=const>O.
Iz”(o)/ <:,
(27)
as before that conditions
the integral
Z(a) = Ii + I2 = %
f(a) into two:
y J o
I” do
(d + q’p(0)
[L(o)+
aw +
=
U12 +$J
~
(02 + i)*fz(o)]a
do
IQo)+a(~‘+~)P
.
It is easy to see that
f2
CI =
In order to estimate same ranges
the integral
of integration
The integrals (2)
I, we partition
it into 5 integrals
as in (17):
I:” + p+ I:“‘+
I, =
Z:“, II
const > 0.
zp+I:“‘.
are estimated
I&Q, I,(5)
in the same way as (20):
g B3a2M2k+2 9
where BJ = Bs(k, 51, z, Kl. For I,(z) (or I&Q + Z$*l, if L (0) 4 0) we obtain Z1@)=g BIa2, We estimate
f 1t3). Introducing NW
(281
B, = &(eo,
a(+‘1
CJ id
Also,
taking
n = l/a,
(o”+f)‘lz(o) [nL(63)+
q-q
into account
et, w,
2,
K).
we have
N(w
1” do 02 + 112
“’
c cm. i-1
(2), (25) and (41), we obtain
over the
A. V. Goncharskii,
252
Using
A. S. Leonov
and A. G. Yagola
of + et < M, we obtain
w
P=COIlSt>O*
[(Oi+&)2+i]z
Hence
from (28)-(30)
I:” <
taking
at/aPD @)
(23) it follows
that
FpM’N(M). 3-P
I,“’ similarly
We estimate
into account
(if L (0) = 0):
Adding the estimates for I, and I,, taking the minimum with respect neglecting terms of a higher order of smallness in a, we obtain
II2(8) -z=(s)
(31)
to M and
11~~ = l([Z(a)] = 0(a1/2P(~+r)},
where q = max 1~ + 2, 2k].
Here 0 depends
on the same quantities
as in (25),
and also on F. It is thereby
proved that if conditions
(l)-(4)
are satisfied
for (7) in the
metric L,, then (31) is satisfied. We have obtained estimate
estimates
for the integrals
We show that if conditions (l)-(4) are satisfied holds for the rate of convergence of the regularized solution
(7), (8).
We now obtain
an
for (6).
of equation
(1):
(32)
l/z(s)-
Q??(S) llC = 0
(3%
b(r)
2’(s)
Indeed,
-
II 4
x
0
{~M~+~P(~+~)l},
{~m+P(~+4)1}.
(6), (13) and (25) imply that
the following approximations
estimate to the exact
Some estimates
I/z(s)-
z=“(s)
Minimizing
manner,
;
ai/bP(37+3)
’ ,
to a, that is, selecting we obtain
from the estimates
approximations
=
defining
in (25), (32) determines
essentially
parameter
the rate of convergence on the behaviour
Thus,
the maximum order of the zeros
of its zeros
the regularization
max {2k, y + 2).
and at infinity.
increases,
const.
=
(33), if
obtained,
depends
of its zeros
D,
253
(32) if
Q
r occurring behaviour
+
0{fy-2/r~+P(P+4,1},
As is obvious neighbourhoods
Di
from (6), (9) and (31) we obtain
#-J(6) =
regularized
<
with respect
in some “optimal”
Similarly,
IIc
of the rate of convergence
the estimates of L (w).
the rate of decrease
as o + DO. The slower
of the
of L (0) in the worsen
Also,
as p
the quantity
of L (w) and also the
L (0) decreases
at infinity
and the
more its zeros cluster at the point at infinity, the worse, in general, is the estimate of the rate of convergence of the regularized approximations to the exact solution. The estimates (15), (26) give constraints on the rate of convergence
as a + 0 downwards.
We notice
that by using
a similar
type (25), (32) for other classes is changed
method we can obtain
of kernels.
For example,
to the following: L (0) > A2e-mm;
m > 0,
Az = const > 0,
the estimates
b(s)-
z”(s)IIc = 0
1
1
ln(W
>
hold, and as for (32),
llw-z;(a)(s)I,c =
0
. 1,.___!_l W/Q
estimates
of the
if the requirement
(3)
A. V. Goncharskii,
254
In conclusion
the authors
and also V. Ya. Arsenin
A. 5”. Leonov
and A. G. Yagola
thank A. N. Tikhonov
and V. B. Glasko
for supervising
for many discussions
the work,
and for reading
the manuscript. Translated
by J. Berry
1.
TIKHONOV, A. N. On the solution of incorrectly formulated problems and a method of regularization. Dokl. Akad. Nauk SSSR, 151, 3, 501-504, 1963.
2.
BAKUSHINSKII, A. B. Some problems of the theory of regularizing (RA). In: Comp~~~~g methods and Pro~amm~g Wychiel. vanie). 56-79, 12, Izd-vo MGU, Moscow, 1969.
3.
SOBOLEV, S. L. Some Applications Physics fizike).
4.
(Nekotorye primeneniya Izd-vo LGU, Leningrad,
BOCHNER, S. Lectures Fizmatgiz,
Moscow,
of Functional funktsial’nogo 1950.
on Fourier ~~te~aZs 1962.
algorithms metody i programmiro-
Analysis in Mathematical analiza v matematicheskoi
tL_ektsii ob integralakh
Fur’e),
5.
ARSENIN, V. YA. and IVANOV, V. V. The solution of certain convolution type integral equations of the first kind by the regularization method. Zh. uychisl. Mat. mat. Fiz., 8, 2, 310-321, 1968.
6.
ARSENW, V. YA. and IVANOV, V. V. The effect of polarization Zh. vychisl. Mat. mat. Fiz., 8, 3, 661-662, 1968.
7.
ARSENIN, V. YA. and SAVELOVA, F. I. The application of the regularization method to convolution type integral equations of the first kind. Zh. uychisl. Mat. mat. Fiz., 9, 6, 1392-1395, 1969.
8.
IVANOV, V. V. and KUDR~SKII, V. YU. Approximate solution of l&ear operator equations in Hilbert space by the method of least squares. Zh. vychisl. Mat. mat. Fiz., 6, 5, 831-841, 1966.
9.
MOROZOV, V. A. The error principle in the solution of operational equations by the regularization method. Zh. vychiei. Mat. mat. Fiz., 8, 2, 295-309, 1968.
of order p.