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K

-FUNCTIONALS AND EXACT VALUES

OF

n

-WIDTHS IN THE BERGMAN SPACE

Mukim S. Saidusaynov

Tajik National University, Dushanbe, Tajikistan [email protected]

Abstract: In this paper, we consider the problem of mean-square approximation of complex variables functions which are regular in the unit disk of the complex plane. We obtain sharp estimates of the value of the best approximation by algebraic polynomials in terms ofK-functionals. Exact values of some widths of the specified class of functions are calculated.

Key words: Bergman space, Best mean-square approximation,K-functional,n-width.

Introduction and preliminary facts

We consider the problem of mean-square approximation by Fourier sums of complex functions f which are regular in a simply connected domain D ⊂ C and belong to the space L2 := L2(D)

with the finite norm

kfk:=kfkL2(D)= 1 π

Z Z

(D)|

f(z)|2dσ !1/2

,

where the integral is understood in the Lebesgue sense anddσ is an element of area.

The study of the mean-square approximation of functions in the domainD ⊂Cis closely related

to the theory of orthogonal functions. A sequence of complex functions {ϕk(z)} (k= 0,1,2, ...) is called an orthogonal system on the domainD if

1 π

Z Z

(D)

ϕk(z)ϕl(z)dσ= 0, k6=l.

Such a sequence of functions is called orthonormal system if 1

π Z Z

(D)

ϕk(z)ϕl(z)dσ=δk,l,

whereδk,l= 0, k6=l,and δk,k = 1, k ∈N. Iff ∈L2, then the numbers

ak(f) = 1 π

Z Z

(D)

f(z)ϕk(z)dσ (1)

are called the Fourier coefficients of the functionf with respect to the orthonormal system{ϕk(z)} (k= 0,1,2, ...). We associate with a given functionf its Fourier series with respect to the specified orthogonal system:

f(z) ∞ X

k=0

ak(f)ϕk(z). (2)

Let

Sn−1(f, z) = n−1 X

k=0

(2)

be the partial sum of ordernof the series (2). We form a linear combination of the firstnfunctions of the system{ϕk(z)}:

pn−1(z) = n−1 X

k=0

dkϕk(z),

where dk ∈ C are arbitrary complex coefficients. We call this linear combination a generalized polynomial. It is well known (see, for example, [1], p.263) that

En−1(f) = inf{kf−pn−1k: dk∈C}

=kf Sn−1(f)k= ( ∞

X

k=n

|ak(f)|2 )1/2

, (3)

whereak(f) are the Fourier coefficients of the functionf defined by (1).

In the case of the mean approximation of complex functions in a simply connected domain

D ⊂ C by Fourier series with respect to an orthogonal system of functions {ϕk(z)}

k=0 on D, the problem of finding the exact constant in the Jackson-Stechkin inequality was studied in [2]. Recall that Jackson-Stechkin inequalities are inequalities in which the value of the best approximation of a function by a finite dimensional subspace of a given normed space is estimated by the modulus of smoothness of the function itself or some its derivative. In this paper, we use the same methods as in [2, 3, 5, 15].

We study in more detail the case whereD is the unit diskU :={zC:|z|<1}. In this case,

it is clear that the system of functionsϕk(z) =zk(k= 0,1,2, ...) is orthogonal in the diskU: 1

π Z Z

(U)

ϕk(z)ϕl(z)dσ= 1 π

Z 1

0 Z 2π

0

rk+l+1ei(k−l)tdrdt= 0, k6=l.

However, this system is not orthonormal, since 1

π Z Z

(U)|

ϕk(z)|2dσ= 1 π

Z 1

0 Z 2π

0

r2k+1drdt= 1 k+ 1. Therefore, the system of functionsϕ∗

k(z) =

k+ 1zk (k= 0,1,2, ...) is orthonormal. We denote by

A(U) the set of all functionsf analytic inU. The Maclaurin series of such a function has the form

f(z) = ∞ X

k=0

ck(f)zk, (4)

whereck(f) are the Maclaurin coefficients of f. We note that

kfk2= ∞ X

k=0

|ck(f)|2 k+ 1 , E

2

n−1(f) =

∞ X

k=n

|ck(f)|2

k+ 1 . (5) It was proved in the monograph [1] that the Fourier series of a function f with respect to the orthonormal system ϕ∗

k(z) =

k+ 1zk, k = 0,1,2, ..., coincides with the series (4) for f ∈ A(U); i.e.,

f(z) = ∞ X

k=0

ak(f)ϕ∗k(z) = ∞ X

k=0

ck(f)zk. (6)

Therefore, the series (6) can be differentiated term by term any number of times and, according to the Weierstrass theorem [6, p.107], for anyrN, we get

f(r)(z) = ∞ X

k=r

ck(f)k(k−1)· · ·(k−r+ 1)zk−r:= ∞ X

k=r

(3)

where

αk,r :=k(k−1)· · ·(k−r+ 1), k∈N, r∈Z+, k≥r.

We denote by L(2r) := L(2r)(U) (L(0)2 := L2(U)) the class of all functions f ∈ L2 such that f(r)L2 (r ∈Z+, f(0)≡f).

1. Sharp estimates of the value of the best approximation by means of

K-functionals

In this section, we prove some sharp inequalities relating the value En−1(f) of the best approx-imation of functions in the classL(2r)and Peetre K-functionals. The definition and some properties of Peetre K-functionals are given in [7]. The direct and inverse theorems of the theory of approx-imation by means of K-functionals were proved in [8, 9]. We define the K-functional constructed by the spacesL2 and L(2m) as follows:

Km(f, tm)2 :=K

f, tm;L2;L(2m)

= infnkf gk2+tm· kg(m)k2 :g∈L(2m) o

, (8)

where mN and 0 < t1. We note that a weak equivalence of the K-functional defined by (8)

and a special generalized modulus of continuity of order mwas established in [8].

Theorem 1. Let n, m N and r Z+ be arbitrary numbers such that n r+m. Then the

following equality holds:

sup f∈L(r)

2

f /∈Pr p

(n+ 1)/(nr+ 1)·αn,rEn−1(f)

Km f(r), r

nrm+ 1 nr+ 1 ·

1 αn−r,m

! = 1. (9)

P r o o f. Using (7), we easily find that

En2−r−1(f(r)) =

∞ X

k=n

α2k,r |ck(f)| 2

kr+ 1, r ∈Z+. (10)

Taking into account equality (10), we obtain

En2−1(f) =

∞ X

k=n

|ck(f)|2 k+ 1 =

∞ X

k=n

kr+ 1 (k+ 1)α2

k,r

·α2k,r· |ck(f)| 2

kr+ 1

≤max k∈N k≥n

(

kr+ 1 (k+ 1)α2k,r

)

·

∞ X

k=n

α2k,r |ck(f)| 2

kr+ 1

= n−r+ 1 n+ 1 ·

1 α2

n,r ·

En2−r−1

f(r).

(11)

Now, for an arbitrary functionf L(2r), we write

En−1(f)≤ r

nr+ 1 n+ 1 ·

1 αn,r

En−r−1

f(r) r

nr+ 1 n+ 1 ·

1 αn,rk

(4)

where Sn−r−1(g) is the partial sum of order n−r of the Fourier series of an arbitrary function gL(2m). In view of (2) and (11), we get

kgSn−r−1(g)k=En−r−1(g)≤ r

nrm+ 1 nr+ 1 ·

1 αn−r,m

En−r−m−1

g(m)

r

nrm+ 1 nr+ 1 ·

1 αn−r,m

g

(m) .

(13)

It follows from inequalities (12) and (13) that

En−1(f)≤ r

nr+ 1 n+ 1 ·

1 αn,r

n

kf(r)gk+kgSn−r−1(g)k o

r

nr+ 1 n+ 1 ·

1 αn,r

(

kf(r)gk+ r

nrm+ 1 nr+ 1 ·

1 αn−r,m

g

(m)

) .

(14)

Now, we note that the left-hand side of inequality (14) does not depend on g L(2m). Therefore, passing to the infimum over all functions g L(2m) on the right-hand side of (14) and using the definition (8) of K, we get

En−1(f)≤ r

nr+ 1 n+ 1 ·

1

αn,rKm f (r),

r

nrm+ 1 nr+ 1 ·

1 αn−r,m

! .

This implies the following upper bound:

sup f∈L(r)

2

f /∈Pr p

(n+ 1)/(nr+ 1)·αn,rEn−1(f)

Km

f(r), r

nrm+ 1 nr+ 1 ·

1 αn−r,m

≤1, (15)

wherePr is the subspace of complex algebraic polynomials of degree at most r.

To obtain a lower bound of the extremal characteristic on the left-hand side of (15), in (8), we put f(z) :=pn(z), where pn(z) is an arbitrary complex algebraic polynomial in Pn. Since the functiong(z)0 belongs to the class L(2m), we obtain from (8) the upper bound

Km(pn;tm)2 ≤ kpnk.

Since the functiong(z) :=pn(z) also belongs to the class L(2m), we find from (8) that

Km(pn;tm)2 ≤tmkp(nm)k.

Thus, the last two relations imply that, for any element pn(z)∈ Pn,

Km(pn;tm)2 ≤min n

kpnk;tmkp(nm)k o

. (16)

We consider the function f0(z) =zn. Since

f0(r+m)=n(n1)· · ·(nr+ 1)· · ·(nrm+ 1)zn−r−m =αn,r·αn−r,mzn−r−m, according to (16), we have

K f0(r); r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!

r

nrm+ 1 nr+ 1 ·

1 αn−r,mk

f0(r+m)k

= r

nrm+ 1 nr+ 1 ·

1 αn−r,m ·

αn,r·αn−r,m

nrm+ 1 =

αn,r

(5)

Using the obtained inequality and the second equality in (5), we establish that

sup f∈L(r)

2

f∈Pr p

(n+ 1)/(nr+ 1)·αn,rEn−1(f)

Km f(r), r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!

p

(n+ 1)/(nr+ 1)·αn,rEn−1(f0)

Km f0(r), r

nrm+ 1 nr+ 1 ·

1 αn−r,m

! ≥1.

(17)

We obtain equality (9) by comparing the upper bound (15) with the lower bound (17). The theorem is proved.

2. Exact values of n-widths of a class of functions

We assume that S is the unit ball in the space L2, Λn ⊂ L2 is an n-dimensional subspace, and Λn L

2 is a subspace of codimension n. Let L : L2 → Λn be a continuous linear operator, let L⊥ : L2 → Λn be a continuous linear projection operator, and let M be a convex centrally symmetric subset ofL2. The quantities

bn(M, L2) = sup{sup{ε >0; εSΛn+1 M}: Λn+1L2},

dn(M, L2) = inf{sup{inf{kf −gk:g∈Λn}:f ∈M}: Λn⊂L2}, δn(M, L2) = inf{inf{sup{kf − Lfk:f M}:LL2 Λn}: ΛnL2},

dn(M, L2) = inf{sup{kfk2 :f MΛn}: ΛnL2}, Πn(M, L2) = inf

n

infnsupnkf− L⊥fk:f Mo:LL2 Λno: ΛnL2o

are called, respectively, theBernstein,Kolmogorov,linear,Gelfand, andprojection n-widths of the subsetMin the spaceL2. These widths are monotone with respect ton, and the following relation holds (see, for example, [10, 11]):

bn(M, L2)≤dn(M, L2)≤dn(M, L2) =δn(M, L2) = Πn(M, L2). (18) We recall (see, for example, [12, p. 25]) that a nondecreasing function Ψ on R+ is called a

k-majorant if the function t−kΨ(t) is nonincreasing inR

+, Ψ(0) = 0, and Ψ(t)→ 0 as t→0. For k= 1, the function Ψ is simply called a majorant.

Let W2(r)(Km,Ψ), r ∈Z+, m∈ N, be the class of all functions f ∈L(2r) whose derivatives f(r) satisfy the condition

Km(f(r), tm)≤Ψ(tm), 0< t <1.

In this definition, Ψ is a majorant, L(0)2 L2, and W2(0)(Km,Ψ) = W2(Km,Ψ). For any subset ML2, we define

En−1(M)L2 := sup{En−1(f) : f ∈M}.

(6)

Theorem 2. Let Ψ be the majorant defining the class W2(r)(Km,Ψ), m N, and r R+.

Then, for any natural number nm+r, we have

λn

W2(r)(Km,Ψ), L2

=En−1

W2(r)(Km,Ψ)

= r

nr+ 1 n+ 1 ·

1 αn,rΨ

r

nrm+ 1 nr+ 1 ·

1 αn−r,m

! ,

(19)

where λn(·) is any of the n-widths bn(·),dn(·), dn(·), δn(·), andΠn(·).

P r o o f. Letnbe a natural number such thatnm+r. In view of the definition of the class W2(r)(Km,Ψ), relations (15) and (18) imply that

λn

W2(r)(Km,Ψ), L2

≤dn

W2(r)(Km,Ψ), L2

≤En−1

W2(r)(Km,Ψ)

r

nr+ 1 n+ 1 ·

1 αn,rΨ

r

nrm+ 1 nr+ 1 ·

1 αn−r,m

! .

(20)

To find the corresponding lower bound, in view of (18), it suffices to estimate the Bernstein n-width of the class W2(r)(Km,Ψ). On the set Pn∩L2, we define the ball

Mn+1:= (

pn∈ Pn:kpnk ≤ r

nr+ 1 n+ 1 ·

1 αn,rΨ

r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!) .

Now, we note that, in view of formula (7) and the identity αk,r+m =αk,rαk−r,m, for an arbitrary pn(z) =Pnk=0ak(pn)zk ∈ Pn, the following equality holds:

p(nr+m)(z) = n X

k=r+m

ak(pn)αk,r+mzk−r−m := n X

k=r+m

ak(pn)αk,r·αk−r,mzk−r−m.

Hence, using the Parseval equality and the inequality αk,r ≤αn,r, k≤n, we obtain the Bernstein type inequality

kp(nr+m)k= ( n

X

k=r+m

|ak(pn)|2α2k,r·α2k−r,m )1/2

≤αn,r·αn−r,mkpnk. (21)

By definition, for the majorant Ψ and for any 0< τ1 ≤τ2 ≤1, we have the inequality τ1Ψ(τ2) ≤ τ2Ψ(τ1). Therefore, for any 0< t1 ≤t2 ≤1, setting τ1 =tm1 and τ2=tm2 , we obtain

t−1mΨ(tm1 )t−2mΨ(tm2 ). (22) We now show that Mn+1 ⊂ W2(r)(Km,Ψ). Thus, we need to prove that, for any polynomial pn⊂ Mn+1,

Km(p(nr), tm)≤Ψ(tm), 0< t≤1.

Since, by assumption,m, nN, rZ+, andnm+r, we consider two cases:

0< t r

nrm+ 1 nr+ 1 ·

1 αn−r,m

(7)

and

r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!1/m

≤t1. First, assume that

0< t r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!1/m .

In this case, using inequality (22) with

t1=t, t2= r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!1/m

and applying (12) and (21), for anypn∈ Mn+1, we obtain

Km(p(nr), tm)2 ≤tm· kpn(r+m)k ≤tm·αn,r·αn−r,mkpnk

≤tm·αn,r·αn−r,m· r

nr+ 1 n+ 1 ·

1 αn,r

Ψ r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!

≤tm·αn−r,m· r

nr+ 1 nrm+ 1·Ψ

r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!

≤Ψ(tm).

(23)

Now, let

r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!1/m

≤t1.

Then using (16) and the Bernstein type inequality

kp(nr)k ≤αn,r· kpnk

and taking into account that the majorant Ψ is nondecreasing, we find that

Km(p(nr), tm)2≤ kpn(r)k2 ≤αn,rkpnk2

≤αn,r r

nr+ 1 n+ 1 ·

1 αn,r

Ψ r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!

r

nr+ 1 n+ 1 ·Ψ

r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!

≤Ψ r

nrm+ 1 nr+ 1 ·

1 αn−r,m

!

≤Ψ(tm).

(24)

The definition of the classW2(r)(Km,Ψ) along with (23) and (24) implies thatMn+1⊂W2(r)(Km,Ψ). Then, taking into account the definition of the Bernstein n-width and (18), we obtain

λn

W2(r)(Km,Ψ), L2

≥bn

W2(r)(Km,Ψ), L2

≥bn(Mn+1;L2)≥ r

nr+ 1 n+ 1 ·

1 αn,r

Ψ r

nrm+ 1 nr+ 1 ·

1 αn−r,m

! .

(25)

(8)

REFERENCES

1. Smirnov V.I., Lebedev N.A. Constructive theory of functions of complex variables. Moscow-Leningrad: Nauka, 1964 [in Russian].

2. Abilov V.A., Abilova F.V., Kerimov M.K.Sharp estimates for the rate of convergence of Fourier series of functions of a complex variable in the spaceL2(D, p(z)) // J. Comp. Math. and Math. Physics,

2010. Vol. 50, no 6. P. 999–1004. [in Russian]

3. Tukhliev K.Mean-square approximation of functions by Fourier–Bessel series and the values of widths for some functional classes // Chebyshevskii Sb., 2016. Vol. 17, no. 4. P. 141–156. [in Russian]

4. Vakarchuk S.B. Mean approximation of functions on the real axis by algebraic polynomials with Chebyshev–Hermite weight and widths of function class // Math. zametki, 2014. Vol. 95, no. 5. P. 666– 684. [in Russian]

5. Shabozov M.Sh., Tukhliev K.Jackson–Stechkin type inequalities with generalized moduli of conti-nuity and widths of some classes of functions // Proceedings of Instit. of Math. and Mech. Ural Branch of RAS, 2015. Vol. 21, no. 4. P. 292–308.

6. Bitsadze A.V. Fundamentals of the theory of analytic functions of a complex variables. Moscow: Nauka, 1984. [in Russian]

7. Berg J., Lofstrom J.Interpolation spaces. An introduction. Moscow: Mir, 1980. [in Russian] 8. Ditzian Z., Totik V. K-functionals and best polynomial approximation in weighted Lp(R) // J.

Approx. Theory, 1986. Vol. 46, no. 1. P. 38–41.

9. Ditzian Z., Totik V. Moduli of smoothness. Berlin: Springer-Verlag. Heidelberg. New York. Tokyo, 1987.

10. Pinkus A.n-widths in approximation theory. Berlin: Springer-Verlag. Heidelberg. New York. Tokyo, 1985.

11. Tikhomirov V.M.Some questions of approximation theory. Moscow: MSU, 1976. [in Russian] 12. Shevchuk I.A.Approximation of polynomials and traces of continuous functions on a closed interval.

Kiev: Naukova Dumka, 1992. [Russian]

13. Farkov Yu.A.Widths of Hardy classes and Bergman classes on the ball inCn// Uspekhi Mat. Nauki,

1990. Vol. 45, no. 5. P. 229–231. [in Russian]

14. Farkov Yu.A.Then-widths of Hardy-Sobolev spaces of several complex variables // J. Approx. Theory, 1993. Vol.75, no. 2. P. 183–197.

15. Vakarchuk S.B.Best linear methods of approximation and widths of classes of analytic functions in a disk // Math. zametki, 1995. Vol. 57, no. 1. P. 30–39. [in Russian]

16. Vakarchuk S.B., Shabozov M.Sh.The widths of classes of analytic functions in a disc // Mat. Sb., 2010. Vol. 201, no. 8. P. 3–22 [in Russian].

17. Shabozov M.Sh., Langarshoev M.R.The best linear methods and values of widths for some classes of analytic functions in the Bergman weight space // Dokl. Akad. Nauk, 2013. Vol. 450, no. 5. P. 518–521. [in Russian]

18. Shabozov M.Sh., Saidusaynov M.S.The values ofn-widths and the best linear method of approxi-mation of some classes of functions in the weighted Bergman space // Izv. TSU. Natural Science, 2014. No. 3. P. 40–57.

References

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