Let L2 := L2[0, 2π] denote the space of Lebesgue measurable 2π-periodic real functions f with norm

formula1

Let 311—1 be the subspace of all trigonometric polynomials of degree n — 1. It is well known that, for any function f E- L2 with Fourier expansion

formula2

the value of its best approximation in L2 by elements of the subspace ℑn−1 is

formula3

where,

formula4

is the partial sum of order n − 1 of the Fourier series for the function f and formula5

Let formula6 denote the norm of the mth.order difference of a function f e L2: with step h, that is,

formula7

Then

formula8

defines the mth-order modulus of continuity of a function f e L2

By (r E N; L(0)2 = L2) we denote the set of functions f E L2, whose (r — l)st derivatives are absolutely continuous and fr E L2, In Section 3, in defining classes of functions, we characterize the structural properties of a function f E Lr2 by the rate of convergence to zero of the modulus of continuity of its rth derivative f(r), defining this rate in terms of the majorant of some averaged quantity ωm(f(r); t).

Related Extremal Problems

Extremal problems in the theory of approximation of differentiable periodic functions by trigonometric polynomials in the L2 space involve the determination of sharp constants in inequalities of Jackson-Stechkin type

formula9

is smaller than the Jackson functional ωm(f, π/n) and, is apparently more natural for characterizing best approximations En−1(f) of periodic functions in L2.

Given these considerations Ligun [2] studied extremal characteristics of the form (in what follows the ratio 0/0 is set equal to zero):

formula10

where m, n e N; r Z+; O < h 6 rt/n; 9(t)> 0 is integrable on the segment [0, h]. He showed that

formula11

In order to generalize the results of [2], using the scheme of reasoning in Pinkus [3, pp.104-107], Shabozov and Yusupov [4] introduced the extremal characteristic

formula12

where formula13 is integrable on the segment [O, h], and for O < p 6 2 proved the inequality

formula14

In the calculation of the exact values of the n-widths of classes of functions directly from (2.1), and in connection with the accuracy of (2.2) there is a need to establish the equality

formula15

for any positive integrable functions φ on the segment [0, h]. In general, the verification of (2.3) is not always possible. For some specific weight functions φ, condition (2.3) is proved in [5]. Obviously, equation (2.3) depends on the structural properties of the weight function φ. A natural question arises: what structural and differential properties must a function φ have in order to satisfy (2.3)? The answer to the question is contained in the following statement.

Theorem 2.1:Suppose that the weight function φ (t) defined on [0, h] is non-negative and continuously differentiable thereon. If, for formula16 and every t E [0, h] we have

(rp − 1)φ(t) − tφ'(t) ≥ 0, (2.4)

then, for any m, n e N and formula17 Wn we have the equality

formula18

There is a function formula19 const, realizing the upper bound in (2.1) equal to (2.5).

Proof:We use the following simplified version of Minkowski’s inequality [3, p.104]

formula20

Indeed, bearing in mind that for any function f E L(r)2 we have the relation [10]

formula21

is a strictly increasing function in the domain Q = { x : x ≥ 0 } and, hence,

formula22

Indeed, differentiating (2.7) and using the elementary identity

formula23

Integrating by parts in the last integral of (2.9), the inequality (2.4), we finally obtain

formula24

which implies the relation (2.8)

Therefore continuing inequality (2.6), we have

formula25

Since the last inequality holds for any f L (r) 2 we have an upper bound for (2.5):

formula26

The lower bound in (2.5), valid for all 0 < h ≤ π/n, is obtained by using the function fo(x) cos nx e L(r)2 . We have

formula27

Thus

formula28

Equation (2.5) is a consequence of (2.11) and (2.12). This completes the proof of Theorem 2.1.

As a particular case of Theorem 2.1 we have:

formula29

Proof:The parameter values p, r, β, γ, h as in the statement of Corollary 2.1 suffice to verify (2.4). We have

formula30

because for the values of the above parameters

formula31

This proves Corollary 2.1.

Corollary 2.1 contains, in particular, the results of [4-8] for different parameters p, γ, β and h.

The Statement of the Main Results

We recall the necessary concepts and definitions which will be used later. Suppose that S = {v: ||V|| ≤ 1} is the unit ball in L; is a convex centrally symmetric subset from It; L2; ΛNCL2 is an N.dimensional subspace; ΛN CL2 is a subspace of codimension N; L : L2 + ΛN is a continuous linear operator taking elements of the space L2 to ΛN; and L : L2 + ΛN is a continuous linear projection operator from L2: onto ΛN, The quantities

formula32

formula33

are called, respectively, the Bernstein, Gelfand, Kolmogorov, linear, and projection N-widths in the space L2 . Since L2 is a Hilbert space, the N-widths listed above are related by (see, e.g., [3]):

formula34

We shall denote by Wm(f(r); φ)p,h, m E N u {0},0 < p ≤ 2, O ≤ π the pth mean value of the modulus of continuity of mth order of functions f(r) with weight φ(t) :

formula35

and, by L(r)2 (m, p, h; φ) we designate the set of functions f E L(r)2 for which Wm(f(r); φ)p,h ≤ ω(f(r); h),

where C(m, r, p, h) is a positive constant that depends on the values of the parameters in parentheses. With this notation, the search for the smallest constant in the Jackson-Stechkin inequality is equivalent to the problem of computing the exact upper bound

formula36

Here we will look for the lowest constant relative to the entire

set of the spaces ℑN CL2 of fixed dimension N. This will show that the result can not be improved upon by switching to another subspace of the same dimension

formula37

We also put

formula38

Proposition 3.1:Suppose that h, p > 0, r ℤ+,.. m, n ∈ N. Then the following inequality holds

formula39

Proof. If f ∈ L(r)2, φ(t)≥0 is integrable on the segment [O. h] and, Wm(f(r), φ)p,h = α > 0 then for f1(x) = α−1 f(x), we have Wm(f(r)1 , φ)p,h = 1. Given the positive homogeneous functional E(f, ℑ N )2 and Wm(f(r) , φ)p,h, for any 0 < p ≤ 2 and a fixed h> 0 we have

formula40

Through (3.4) the lower bound over all subspaces ℑN ⊂ L2 dimension N we obtain

formula41

On the other hand, for any function L(r)2 ∈ (m, p, h; φ) bydefinition of the class L(r)2 (m, p, h; φ) have an inequality of the form

formula42

and as this is true for every subspace ℑN ⊂ L2 then

formula43

Proposition 3.1 follows from (3.5) and (3.6).

Theorem 3.1. Suppose that the weight function φ (t) defined on the segment [0, h] is non-negative and continuously differentiable thereon. If for some r ∈ ℕ, 1/r < p ≤ 2, and any t ∈ [0, h], we have

formula44

then, for any m, n ∈ ℕ and 0 < h ≤ π/n

formula45

where δk(·) are any of the k-widths: Bernstein bk(·), Kolmogorov dk (·), linear λk (·), Gelfand dk (·) or projection πk (·). All k–widths are attained by taking the partial sums of the Fourier series Sk−1(f;t).

Proof:From (2.10) and since (3.7) holds, it follows that

formula46

Hence, for the width of the projection of class L(r)2 (m, p, h; φ), we obtain an upper bound

formula47

In order to obtain a lower bound for the Bernstein n-width of L(r)2 (m, p, h; φ) we consider the ball

formula48

in the (2n+1)–dimensional subspace ℑ2n+1 of trigonometric polynomials and show that 𝔹2n+1 ⊂ L(r)2 (m, p, h; φ). In [7] it is proved that for an arbitrary polynomial Tn ∈ ℑ2n+1 for 0 < h ≤ π/n, the inequalit

formula49

Elevate both sides of (3.9) to the to the power p, multiply by φ and integrate the result over t in the range from 0 to h. Whence we obtain directly

formula50

from which 𝔹2n+1 ⊂ L(r)2 (m, p, h; φ). By the definition of the Bernstein n-width we obtain the lower bound

formula51

This completes the proof of Theorem 3.1.

As a particular case of Theorem 3.1 we have a result found in [5]. Namely,

Corollary 3.1:Let formula52

Then the following inequality holds

formula53

where δk(·) are any of the above-listed k-widths


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  3. Pinkus A (1985) n-Widths in Approximation Theory, SpringerVerlag, Berlin, Heidelberg, New York, Tokyo.
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