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Research article

Approximation of functions in a certain Banach space by some generalized singular integrals

  • Received: 27 September 2023 Revised: 26 November 2023 Accepted: 28 November 2023 Published: 05 January 2024
  • MSC : 26A16, 41A25, 42A50

  • We introduced the q-Picard, the q-Picard-Cauchy, the q-Gauss-Weierstrass, and the q-truncated Picard singular integrals. Using the last three mentioned integrals, the orders of approximation for functions from a generalized Hölder space were determined, both in the Lp-norm and in the generalized Hölder-norm.

    Citation: Xhevat Z. Krasniqi. Approximation of functions in a certain Banach space by some generalized singular integrals[J]. AIMS Mathematics, 2024, 9(2): 3386-3398. doi: 10.3934/math.2024166

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  • We introduced the q-Picard, the q-Picard-Cauchy, the q-Gauss-Weierstrass, and the q-truncated Picard singular integrals. Using the last three mentioned integrals, the orders of approximation for functions from a generalized Hölder space were determined, both in the Lp-norm and in the generalized Hölder-norm.



    Already we know well that the approximation theory is concerned with how functions can best be approximated with simpler functions and with quantitatively characterizing the errors introduced. A closely related topic is the approximation of functions by Fourier series. Staying in this particular topic, the approximation of 2π-periodic and integrable functions by their Fourier series in the Hölder metric has been studied regularly by lots of researchers. Das et al. studied the degree of approximation of functions by matrix means of their Fourier series in the generalized Hölder metric [6], generalizing some well-known previous results. Again, Das et al. [7] studied the rate of the convergence problem of the Fourier series in a new Banach space of functions conceived as a generalization of the spaces introduced by Prössdorf [26] and Leindler [20]. Later on, Nayak et al. [24,25] studied the rate of the convergence problem of the Fourier series by delayed arithmetic mean in the generalized Hölder metric space, which was earlier introduced in [7]. This obtained a sharper estimate of Jackson's order and was the main objective of their results. In [18], Kim treated the degree of approximation of functions in the same generalized Hölder metric by using the so-called even-type delayed arithmetic mean of Fourier series. Intentionally, we do not want to mention all published results here because they are somehow beyond the topic treated here. However, for the sake of the interested reader, recent results on that topic can be found in references [14,15,16,17,18,24,25] and the references therein.

    We return back again to the paper of Prössdorf, referenced by [26], who studied the degree of approximation problems of Fourier series of functions from Hα (0<α1) space in the Hölder metric. Let C2π be the Banach space of 2π-periodic continuous functions defined in [π,π] under the sup-norm. For 0<α1 and some positive constant K, the function space Hα is given by

    Hα={fC2π:|f(x)f(y)|K|xy|α}.

    The space Hα is a Banach space with the norm fα defined by

    fα=fC+supx,y{Δαf(x,y)},

    where

    fC=supπxπ|f(x)|

    and

    Δαf(x,y):=|f(x)f(y)||xy|α,xy.

    At this stage, we agree to write (by convention) Δ0f(x,y):=0.

    Now, let us recall the well-known Picard, Picard-Cauchy and Gauss-Weierstrass singular integrals given by

    Pξ(f;x)=12ξf(x+t)e|t|ξdt, (1.1)
    Qξ(f;x)=ξπππf(x+t)t2+ξ2dt (1.2)

    and

    Wξ(f;x)=1πξππf(x+t)et2ξdt, (1.3)

    respectively, where ξ is a positive parameter that tends to zero.

    Everywhere in this paper, we write

    φx(t):=12[f(x+t)+f(xt)2f(x)]

    and u=O(v), whenever there exists a positive constant K, not necessarily the same at each occurrence, such that uKv.

    Let f be a bounded real valued function defined on the real line R or (π,π). By B we denote the Banach space of such functions under the sup-norm.

    Mohapatra and Rodrigez [23] yielded the error bound of fHα in the norm β for (0β<α1). Among others, they proved the following theorems.

    Theorem 1.1. Let fB and

    ω(δ)=sup|t|δ|f(x+t)f(x)|,(δ>0),

    such that ω(t)/t is a nonincreasing function of t, then as ξ0+, the following hold:

    fPξ(f;)C=O(ω(ξ)), (1.4)
    fQξ(f;)C=O(ω(ξ)|ln(1/ξ)|), (1.5)
    fWξ(f;)C=O(ω(ξ)ξ12). (1.6)

    Theorem 1.2. Let 0β<α1 and fHα, then as ξ0+,

    fPξ(f;)β=O(ξαβ),fQξ(f;)β=O(ξαβ|ln(1/ξ)|),fWξ(f;)β=O(ξαβ12).

    Seemingly wishing to generalize the Hölder metric (see [20]), Leindler introduced the function space Hω (a truly generalization) given by

    Hω:={fC[π,π]:|f(x+t)f(x)|=O(ω(|t|))},

    where ω(δ,f) is the modulus of continuity of f and ω is a modulus of continuity; that is, ω is a positive nondecreasing continuous function on [0,2π] having the properties ω(0)=0 and ω(δ1+δ2)ω(δ1)+ω(δ2) for 0δ1δ22π.

    He also introduced the norm ω on the space Hω by

    fω=fC+supt0|f(x+t)f(x)|ω(|t|).

    In the case when ω(δ)=δα, 0<α1 the space Hω reduces to Hα space and the norm ω clearly becomes α–norm, which, as we mentioned above, was introduced by Prössdorf. It is known (see [26]) that

    HαHβC2π,0β<α1.

    Das, Nath and Ray [7] generalized further the space Hω by

    H(ω)p:={fLp[0,2π]:supt0f(+t)f()pω(|t|)<}

    and

    f(ω)p:=fp+supt0f(+t)f()pω(|t|),

    where

    fp:=(12π2π0|f(x)|pdx)1p

    for 1p<, while for p=,

    f:=esssupx(0,2π){|f(x)|}.

    Choosing ω(t) and v(t) so that ω(t)/v(t) is nondecreasing, then

    f(v)pmax(1,ω(2π)/v(2π))f(ω)p,

    which shows the relations

    H(ω)pH(v)pLp,p1.

    The singular integrals Pξ(f;x), Qξ(f;x), Wξ(f;x), as well as their generalizations, are widely used in the problems of approximation of certain class functions. The approximation of functions, belonging to a certain class of functions, have been studied by Khan and Umar [12], Gal [9,10], Deeba et al. [5], Mezei [22], Anastassiou and Mezei [1], Anastassiou and Gal [2], Anastassiou and Aral [3], Rempulska and Tomczak [27], Firlejy and Rempulska [8], Bogalska et al. [4], Leśniewicz et al. [19], Khan and Ram [13] and, of course, there are many other results established by numerous researchers.

    Following from [3], for q>0 and for all nonnegative real ξ, the q-ξ real number [ξ]q is defined by

    [ξ]q:=1qξ1qforq1and[ξ]q:=ξforq=1.

    Now, we are in able to introduce the following generalizations of the integrals (1.1)–(1.3):

    Pξ;q(f;x):=12[ξ]qf(x+t)e|t|[ξ]qdt,
    Qξ;q(f;x):=[ξ]qπππf(x+t)t2+[ξ]2qdt

    and

    Wξ;q(f;x):=1π[ξ]qππf(x+t)et2[ξ]qdt.

    Since, for q=1, these integrals reduce to the singular integrals Pξ(f;x), Qξ(f;x) and Wξ(f;x), respectively, it make sense to name the integrals Pξ;q(f;x), Qξ;q(f;x) and Wξ;q(f;x) the q-Picard singular integrals, the q-Picard-Cauchy singular integrals and q-Gauss-Weierstrass singular integrals, respectively.

    Before we pass to the aim of this paper, we introduce the integral

    ¯Pξ;q(f;x):=12(1eπ[ξ]q)[ξ]qππf(x+t)e|t|[ξ]qdt,

    which we name it "the q-truncated Picard singular integral". The idea of introducing such an integral is that it enables Lemma 1 (see section two) to be applied in the proof of the main results, and in this way it might enlarge its applicability and usefulness in approximations problems. As we will see, the application of the q-truncated Picard singular integral, in approximation of a function f, provides the same degree of approximation, which we are going to show in section three.

    The purpose of this paper is to prove the homologous of Theorems 1.1 and 1.2 in the metric ()p of the space H()p. To my best knowledge and the accessible literature, such results are not reported so far. For the proofs of the main results, we use the same lines of the arguments of [23,26].

    The generalized Minkowski's inequality for integrals states that the norm of an integral is less or equal to the integral of the corresponding norm. For the Lp spaces, it can be formulated as follows.

    Lemma 2.1. (Generalized Minkowski inequality [11]) If z(x,t) is a function in two variables defined for ctd, axb, then

    {ba|dcz(x,t)dt|pdx}1pdc{ba|z(x,t)|pdx}1pdt,p1.

    Lemma 2.2. Let fH(ω)p (p1) and ω and v be two moduli of continuity, such that ω/v is a nondecreasing function of t, then

    (i) φ(t)p=O(ω(t));

    (ii) φ+h(t)φ(t)p=O(ω(t));

    (iii) φ+h(t)φ(t)p=v(|h|)O(ω(t)/v(t)).

    Proof. The proof can be done in the same way as Lemma 1 in [7].

    First we report the following first main result.

    Theorem 3.1. Let qξ(0,1) such that qξ1 as ξ0+. Let fH(ω)p with p1 and ω(t)/t be a nonincreasing function of t, then

    ¯Pξ;qξ(f;)fp=O(ω([ξ]qξ)), (3.1)
    Qξ;qξ(f;)fp=O(ω([ξ]qξ)|ln(1/[ξ]qξ)|), (3.2)
    Wξ;qξ(f;)fp=O(ω([ξ]qξ)[ξ]12qξ). (3.3)

    Proof. Throughout the proof (for simplicity of notation) we simply write q instead of qξ. Taking into account the equality

    ππe|t|[ξ]qdt=2(1eπ[ξ]q)[ξ]q

    and the truncated Picard singular integral ¯Pξ;q(f;x) we can write

    ¯Pξ;q(f;x)f(x)=1(1eπ[ξ]q)ξπ0φx(t)e|t|[ξ]qdt.

    Therefore, using Lemma 2.1, we have

    ¯Pξ;q(f;)fp={12π2π0|1(1eπ[ξ]q)[ξ]qπ0φx(t)e|t|[ξ]qdt|pdx}1p1(1eπ[ξ]q)[ξ]qπ0{12π2π0|φx(t)|pdx}1pe|t|[ξ]qdt=1(1eπ[ξ]q)[ξ]q[ξ]q0φ(t)pe|t|[ξ]qdt:=P1+1(1eπ[ξ]q)[ξ]qπ[ξ]qφ(t)pe|t|[ξ]qdt:=P2, (3.4)

    where 0<[ξ]q<π.

    Since ω(t) is monotonically increasing, Lemma 2.1 (ⅰ) implies

    P1=O(1)1(1eπ[ξ]q)[ξ]q[ξ]q0ω(t)e|t|[ξ]qdt=O(1)ω([ξ]q)(1eπ[ξ]q)[ξ]qξ0e|t|[ξ]qdt=O(1)ω([ξ]q)(1eπ[ξ]q)[ξ]qe1e[ξ]q=O(ω([ξ]q)). (3.5)

    Moreover, using the condition that ω(t)/t is nonincreasing and integrated by parts, we also obtain

    P2=O(1)1[ξ]qπ[ξ]qω(t)e|t|[ξ]qdt=O(1)1[ξ]qπ[ξ]qω(t)tte|t|[ξ]qdt=O(1)ω([ξ]q)[ξ]2qπ[ξ]qte|t|[ξ]qdt=O(1)ω([ξ]q)[ξ]2q[ξ]q(2ξe1eπ[ξ]q([ξ]q+π))=O(ω([ξ]q)). (3.6)

    Consequently, (3.4) along with (3.5) and (3.6) imply (3.1).

    By (1.2) and some appropriate operations, we arrive at

    Qξ;q(f;x)f(x)=2[ξ]qππ0φx(t)t2+[ξ]2qdtf(x)L([ξ]q), (3.7)

    where

    L([ξ]q):=2[ξ]qππ0dtt2+[ξ]2q+1.

    The L'hospital's rule gives us

    lim[ξ]q0+L([ξ]q)[ξ]q=lim[ξ]q0+(1[ξ]q2π1[ξ]qarctan(π[ξ]q))=2π2

    and therefore (0<[ξ]qπ)

    L([ξ]q)=O([ξ]q)=O([ξ]qω([ξ]q)ω([ξ]q))=O(πω(π)ω([ξ]q))=O(ω([ξ]q)), (3.8)

    since t/ω(t) is an increasing function of t.

    Now, we need to estimate from upper the integral appearing in (3.7). Indeed, first we write

    q:=2[ξ]qππ0φx(t)t2+[ξ]2qdt=2[ξ]qπ([ξ]q0φx(t)t2+[ξ]2qdt:=Q1+π[ξ]qφx(t)t2+[ξ]2qdt:=Q2),

    then, using Lemma 2.1 and fH(ω)p, we obtain

    Q1p=O(1)[ξ]q0φ(t)pt2+[ξ]2qdt=O(1)[ξ]q0ω(t)t2+[ξ]2qdt=O(ω([ξ]q))[ξ]q0dtt2+[ξ]2q=O(ω([ξ]q)/[ξ]q).

    Once more, using Lemma 2.1, fH(ω)p and the assumption, we get

    Q2p=O(1)π[ξ]qφ(t)pt2+[ξ]2qdt=O(1)π[ξ]qω(t)tt(t2+[ξ]2q)dt=O(ω([ξ]q)/[ξ]q)π[ξ]qtdtt2+[ξ]2q=O(ω([ξ]q)/[ξ]q)lnπ2+[ξ]2q2[ξ]2q.

    Besides that, the limit

    lim[ξ]q0+lnπ2+[ξ]2q2[ξ]2qln(1[ξ]q)=lim[ξ]q0+2π2π2+[ξ]2q=2

    implies

    Q2p=O((ω([ξ]q)/[ξ]q)|ln(1/[ξ]q)|).

    Thus,

    qp=O([ξ]q)(Q1p+Q2p)=O(ω([ξ]q)|ln(1/[ξ]q)|). (3.9)

    Consequently, (3.7)–(3.9) imply

    Qξ;q(f;)fpqp+fp|L([ξ]q)|=O(ω([ξ]q)ln|1/[ξ]q|),

    which is (3.2).

    When all was said and done, we can write

    Wξ;q(f;x)=2π[ξ]qπ0φx(t)et2[ξ]qdt+2f(x)π[ξ]qπ0et2[ξ]qdt,

    and taking into account that

    et2[ξ]qdt=π[ξ]q([ξ]q>0), (3.10)

    we get

    Wξ;q(f;x)f(x)=2π[ξ]qπ0φx(t)et2[ξ]qdt:=W11π[ξ]q(ππ)f(x)et2[ξ]qdt:=W2. (3.11)

    Using Lemma 2.1 and fH(ω)p, we have

    W1p=O(1[ξ]q)π0φ(t)pet2[ξ]qdt=O(1[ξ]q)([ξ]q0ω(t)et2[ξ]qdt:=W11+π[ξ]qω(t)et2[ξ]qdt:=W12). (3.12)

    For W11 (using (3.10)), we have

    W11ω([ξ]q)[ξ]q0et2[ξ]qdtω([ξ]q)0et2[ξ]qdt=π2[ξ]12qω([ξ]q)π2ω([ξ]q), (3.13)

    while for W12, we obtain

    W12ω([ξ]q)π[ξ]qt[ξ]qet2[ξ]qdtω([ξ]q)[ξ]qt[ξ]qet2[ξ]qdt=12e[ξ]qω([ξ]q)12ω([ξ]q). (3.14)

    Thus, from (3.12)–(3.14), we get

    W1p=O(1[ξ]q)(W11+W12)=O(ω([ξ]q)[ξ]q). (3.15)

    For W2, we can write

    W2=2f(x)π[ξ]qπet2[ξ]qdt

    and, therefore, using the assumption that t/ω(t) is increasing with respect to t, we find that

    W2p2fpππ[ξ]qπtet2[ξ]qdt=fpππ[ξ]q[ξ]qeπ2[ξ]qω([ξ]q)[ξ]q[ξ]qω([ξ]q)fpω(π)πeπ2[ξ]qω([ξ]q)[ξ]q=O(ω([ξ]q)[ξ]q)for0<[ξ]q<π. (3.16)

    Combining (3.11), (3.15) and (3.16), we obtain

    Wξ;q(f;)fpW1p+W2p=O(ω([ξ]q)[ξ]q),

    which is (3.3).

    The proof is completed.

    Remark 3.1. The assumption in Theorem 3.1, qξ(0,1) such that qξ1 as ξ0+ is significant to the rate of convergence in the metric p. Otherwise, if q(0,1), then

    limξ0[ξ]q=11q0.

    To overcome this inconvenience, for example, let us choose qξ so that

    121ξqξ<1

    for some ξ>0, then

    [ξ]qξ=1qξξ1qξ2(1qξ)2ξ,

    which shows that [ξ]qξ0 as ξ0.

    If we replace the function ω(t) by tα (0<α1) in definition of the H(ω)p space, then it reduces to the Banach space H(α,p) equipped with the norm (α,p) (for more details, see [6], p. 140). In this case, the condition that ω(t)/t has to be a nonincreasing function of t is satisfied automatically. For this reason, Theorem 3.1 implies the following corollary.

    Corollary 3.1. Let qξ(0,1) such that qξ1 as ξ0+. Moreover, let fH(α,p) with p1 and 0<α1, then

    ¯Pξ;qξ(f;)f(α,p)=O([ξ]αqξ),Qξ;qξ(f;)f(α,p)=O([ξ]αqξ|ln(1/[ξ]qξ)|),Wξ;qξ(f;)f(α,p)=O([ξ]α12qξ).

    Note here that H(α,) is the familiar Hα space introduced earlier by Prössdorf [26]. Therefore, from Theorem 3.1 (q=1), we also derive the following.

    Corollary 3.2. [23] Let fHα with 0<α1, then as ξ0+,

    Qξ(f;)fC=O(ξα|ln(1/ξ)|),Wξ(f;)fC=O(ξα12).

    Remark 3.2. Note that Theorem 1.1 (recalled in the introduction of this article) can be implied from Theorem 3.1 as a special case (except relation (3.14)).

    Now, we prove the homologous statement of Theorem 1.2.

    Theorem 3.2. Let qξ(0,1) such that qξ1 as ξ0+. Moreover, let fH(ω)p with p1, ω(t)v(t) be a nondecreasing function, ω(t)/t be a nonincreasing function and h[[ξ]qξ,π], then

    f¯Pξ;qξ(f;)(v)p=O(ω([ξ]qξ)v([ξ]qξ)), (3.17)
    fQξ;qξ(f;)(v)p=O(ω([ξ]qξ)v([ξ]qξ)|ln(1/[ξ]qξ)|), (3.18)
    fWξ;qξ(f;)(v)p=O(ω([ξ]qξ)v([ξ]qξ)[ξ]qξ). (3.19)

    Proof. For simplicity (only in the proof), we write q instead of qξ. If we put

    Dξ;q(f;x):=¯Pξ;q(f;x)f(x),

    then we can write

    Dξ;q(f;x+h)Dξ;q(f;x)=1(1eπ[ξ]q)[ξ]qπ0[φx+h(t)φx(t)]e|t|[ξ]qdt=1(1eπ[ξ]q)[ξ]q([ξ]q0[φx+h(t)φx(t)]e|t|[ξ]qdt:=D1+π[ξ]q[φx+h(t)φx(t)]e|t|[ξ]qdt:=D2), (3.20)

    where 0<[ξ]qhπ.

    Using Lemma 2.1 and Lemma 2.2 (ⅲ), we find that

    D1p=O(1)[ξ]q0φ+h(t)φ(t)pe|t|[ξ]qdt=O(v(|h|))[ξ]q0ω(t)v(t)e|t|[ξ]qdt=O(v(|h|))ω([ξ]q)v([ξ]q)π0e|t|[ξ]qdt=O((1eπ[ξ]q)[ξ]qv(|h|)ω([ξ]q)v([ξ]q)). (3.21)

    Analogously, using Lemma 2.1, Lemma 2.2 (ⅱ), and the assumption that ω(t)/t is a nonincreasing function of t, we have

    D2p=O(1)π[ξ]qφ+h(t)φ(t)pe|t|[ξ]qdt=O(1)π[ξ]qω(t)tte|t|[ξ]qdt=O(ω([ξ]q)[ξ]q)π[ξ]qte|t|[ξ]qdt=O(ω([ξ]q)[ξ]q)ππ0e|t|[ξ]qdt=O((1eπ[ξ]q)[ξ]qω([ξ]q)v([ξ]q)v([ξ]q))=O((1eπ[ξ]q)[ξ]qv(|h|)ω([ξ]q)v([ξ]q)) (3.22)

    for 0<[ξ]qhπ.

    Using Minkowski's inequality in (3.20), and keeping in mind (3.21) and (3.22), we obtain

    Dξ;q(f;+h)Dξ;q(f;)pv(|h|)=O(1(1eπ[ξ]q)[ξ]q)(D1p+D2p)=O(ω([ξ]q)v([ξ]q)). (3.23)

    Based on relation (3.1) of Theorem 3.1, we can write

    ¯Pξ;q(f;)fp=O(ω([ξ]q))=O(ω([ξ]q)v([ξ]q)v([ξ]q))=O(ω([ξ]q)v([ξ]q)) (3.24)

    because of v([ξ]q)v(π).

    Thus, using (3.23) and (3.24), we have

    f¯Pξ;q(f;)(v)p=O(ω([ξ]q)v([ξ]q)),

    which is (3.17) as requested.

    The proofs of (3.18) and (3.19) can be done in a similar way as (3.17). Therefore, we have intentionally skipped them.

    The proof is completed.

    Let ω(t)=tα, v(t)=tβ, 0β<α1. These conditions enable us (from Theorem 1.2) to extract the following.

    Corollary 3.3. Let qξ(0,1) such that qξ1 as ξ0+. Moreover, let fH(α,p) with p1, 0β<α1 and h[[ξ]qξ,π], then

    f¯Pξ;qξ(f;)(β,p)=O([ξ]αβqξ),fQξ;qξ(f;)(β,p)=O([ξ]αβqξ|ln(1/[ξ]qξ)|),fWξ;qξ(f;)(β,p)=O([ξ]αβ1/2qξ).

    Remark 3.3. Let ω(t)=tα, v(t)=tβ, 0β<α1 and fHα, then Theorem 1.2 can be implied by Theorem 3.2 (except relation (3.17)).

    Remark 3.4. We note that, even the singular integrals Pξ(f;x) and ¯Pξ;1(f;x) differ in their limits of integration and they give the same order of approximation in various metrics.

    In this paper we have introduced the q-Picard, the q-Picard-Cauchy, the q-Gauss-Weierstrass, and the q-truncated Picard singular integrals in a simple form. The deviations, in the Lp-norm and in the generalized Hölder-norm, between these integrals and the functions from a generalized Hölder space has been obtained. We have demonstrated that the obtained degrees of approximation are of Jackson's order, with exception in the case when the q-Picard-Cauchy singular integral has been used. To achieve these degrees of approximation, we have shown that the values of the number q>0 have to be restricted. These results, in the point of view for future research, open new perspectives for further generalizations.

    The author declares he has not used Artificial Intelligence (AI) tools in the creation of this article.

    We would like to thank the reviewers for their comments which improved the submitted version of this paper.

    The author has no conflict of interest to declare.



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