Return to Article Details Generalized growth and approximation errors of entire harmonic functions in Rn, n3

Generalized Growth and Approximation Errors of Entire Harmonic Functions in Rn, n3

Devendra Kumar

October 20, 2018. Accepted: December 17, 2018. Published online: February 17, 2019.

Department of Mathematics, Faculty of Sciences, Al-Baha University, P.O.Box-1988, Alaqiq, Al-Baha-65431, Saudi Arabia, K.S.A.
Department of Mathematics, [Research and Post Graduate Studies], M.M.H.College, Model Town, Ghaziabad-201001, U.P., India e-mail: d_kumar001@rediffmail.com.

In this paper we study the continuation of harmonic functions in the ball to the entire harmonic functions in space Rn,n3. The generalized order introduced by M.N. Seremeta has been used to characterize the growth of such functions. Moreover, the generalized order, generalized lower order and generalized type have been characterized in terms of harmonic polynomial approximation errors. Our results apply satisfactorily for slow growth.

MSC. 30E10, 41A15.

Keywords. Approximation errors, entire harmonic functions, generalized order, generalized type and ball of radius R

1 Introduction

Since the entire functions form a simplest class of analytic functions which includes all polynomials several researchers like Varga [ 14 ] , Batyrev [ 1 ] , Reddy [ 7 ] , Ibraginov and Shikhaliev [ 3 ] , Vakarchuk [ 13 ] , Kasana and Kumar [ 6 ] and others had obtained the characterization of growth parameters of an entire function f(z) in terms of the sequences of polynomial approximation and interpolation errors taken over different domains in the complex plane. Similar characterizations had been investigated for entire harmonic functions in Rn,n3 in terms of harmonic polynomial approximation errors. When we discuss time dependent problems in R3 it leads to study the entire harmonic functions in R4. Therefore, it is significant to mention here that the harmonic functions play an important role in theoretical mathematical research, physics and mechanics to describe different stationary processes. Hence, sometime it is reasonable to study generalized growth characteristics of harmonic functions in an n-dimensional space.

Let xRn(n3) be an arbitrary point where x=(x1,x2,,xn) and put |x|=(x12+x22++xn2)12. The set of all non-constant entire harmonic functions on Rn is denoted by H. For each uH,r>0 we have an expansion into a Fourier-Laplace series [ 11 ]

u(rx)=k=0Y(k)(x;u)rk,
1

where xSn={xRn:|x|=1} a unit sphere in Rn centered at the origin and

Y(k)(x;u)=a1(k)Y1(k)(x)+a2(k)Y2(k)(x)++aγk(k)Yγk(k)(x),aj(k)=(u,Yj(k))=Γ(n2)2(π)n2Snu(x)Yj(k)(x)dS,j=1,γk,γk=(2k+n2)(k+n3)!k!(n2)!.

Here dS is the element of the surface area on the sphere Sn,(u,Yj(k)) is the scalar product in L2(Sn) and Y(k) is a spherical harmonic of degree k,kZ+={0,1,2,,} on the unit sphere Sn(n2) [ 10 ] .

Let BR={yRn:|y|R} be the ball of radius R in space Rn,n3 centered at the origin, and BR be the closure of BR. We denote HR, the class of harmonic functions in BR and continuous on BR,0<R<.

An approximation error of function uHR by harmonic polynomials PΠk is defined as

ERk(u)=infPΠk{maxyBR|u(y)P(y)|},
2

where Πk be a set of harmonic polynomials of degree not exceeding k.

We state some results which will be useful in the sequel.

Lemma 1

[ 15 ] If uHR, then for all kN inequality

maxxSn|Y(k)(x;u)|Rk4(k+2ν)2ν(2ν)!ERk1(u)

holds, where ν=n22.

Lemma 2

[ 15 ] For an entire harmonic function uRn,n3 which is assigned by the series 1, the following inequality hold

(2ν)!21(k+2ν)νmaxxSn|Y(k)(x;u)|M(r;u)rk,kZ+,r>0,

where M(r;u)=maxxSn|u(rx)|.

Lemma 3

[ 15 ] For an entire harmonic function uRn,n3, the following estimation holds

ERk(u)2(2ν)!(2ν+1)(k+2ν)2νM(r;u)(Rr)k,kZ+,r>eR.

2 Generalized Growth Parameters

Let ϕ be a real valued function defined and differentiable on [a,+) at some a0 such that ϕ(x) is positive, strictly monotonically increasing and tends to . Then ϕ is said to belong to the class Lo if for every real valued function φ(x) such that φ(x)0 as x,ϕ satisfies

limxϕ[(1+φ(x))x]ϕ(x)=1
3

and belongs to the class Δ if for all c,0<c<, we have the stronger condition

limxϕ(cx)ϕ(x)=1.
4

Using the functions from the classes Lo,Δ Seremeta [ 8 ] obtained the following characterizations for entire function f(z)=k=0akzk:

Theorem A

Let α(x)Δ,β(x)Lo. Set G(x,c)=β1[cα(x)]. If dG(x,c)dlogx=O(1), as x for all c,0<c<, then the generalized order

ρ(α,β,f)=lim suprα(logM(r;f))β(logr)=lim suprα(k)β(log|ak|1k),
where M(r;f)=max|z|=r|f(z)|.

Theorem B

Let α(x)Lo,β1(x)Lo,φ(x)Lo. Let ρ,0<ρ<, be a fixed number. Set G(x,σ,ρ)=φ1{[β1(σα(x))]1ρ}. Suppose that for all σ, 0<σ<,

  1. If φ(x)Δ and α(x)Δ, then dG(x,σ,ρ)dlogx=O(1), as x.

  2. If φ(x)LoΔ or α(x)LoΔ, then limxdG(x,σ,ρ)dlogx=1ρ.

Then we have

lim suprα(logM(r;f))β[(φ(r))ρ]=lim supkα(kρ)β{[φ(e1ρ|ak|1k)]ρ}.

S.M. Shah [ 9 ] introduced the generalized lower order λ(α,β,f) as

λ(α,β,f)=lim infrα(logM(r;f))β(logr)

and proved the following theorem:

Theorem C

Let f(z)=Σk=0akzk be an entire function. Set G(x)=β1(α(x)). For some function ξ(x) β(xξ(x))β(ex)0,dG(x)d(logx)=O(1), as x,

|akak+1| is ultimately a non decreasing function of k. Then

λ(α,β,f)=lim infkα(k)β(log|ak|1k).

It has been observed that the functions G(x,c) and G(x) of Theorem A and Theorem C respectively, do not satisfy the conditions when α(x)=β(x) i.e., when the entire function f(z) is of slow growth. To include these functions, Kapoor and Nautiyal [ 5 ] introduced a new class of functions and defined generalized order and generalized type as follows:

Let Ω be the class of functions ϕ(x) satisfying the following conditions:

(H,i) ϕ(x) is defined on [a,) such that ϕ is positive, strictly increasing, differentiable and tends to as x.

(H,ii)

limxd(ϕ(x))d(logx)=K, 0<K<.

The generalized order ρ(α,α,f), generalized lower order λ(α,α,f) and generalized type of the entire function f(z) were defined as

ρ(α,α,f)=lim suprα(logM(r;f))α(logr),λ(α,α,f)=lim infrα(logM(r;f))α(logr),1λ(α,α,f)ρ(α,α,f),T(α,α,f)=lim suprα(logM(r;f))[α(logr)]ρ.

where α(x)Ω.

N. Juhong and C. Qing [ 4 ] extended the range of α(x) by defining a new class Ω as the extension of Ω and obtained some results concerning above generalized growth parameters of entire function f(z).

Let Ω be the class of functions ϕ(x) satisfying the condition (H,i) and (H,iii),

(H,iii)

limxd(ϕ(x))d(log[p]x)=K,0<K<,p1,pN+,

where log[0]x=x,log[1]x=logx,log[p]x=log[p1]logx. Also ϕ(x) satisfies 3 and 4.

It is clear that α(x)Ω is a particular case of α(x)Ω for p=1.

Theorem D

[ 4 ] Let α(x)Ω, then some necessary and sufficient conditions of the entire function f(z) with generalized order ρ is

lim suprα(logM(r;f))α(logr)1=lim supkα(k)α(log|ak|1k),p=1,lim supkα(k)α(log|ak|1k)lim suprα(logM(r;f))α(logr)lim supkα(k)α(log|ak|1k)+1, p=2,3,

Theorem E

[ 4 ] . Let α(x)Ω, then the entire function f(z) of generalized order ρ,1<ρ<, is of generalized type T if, and only if

lim suprα(logM(r;f))[α(logr)]ρ=lim supkα(k)[α(log|ak|1k)]ρ1,p=1,lim suprα(logM(r;f))[α(logr)]ρ=lim supkα(k)[α(log|ak|1k)]ρ,p=2,3,

3 Main Results

In this section we shall characterize the generalized growth parameters of entire harmonic functions in space Rn,n3 in terms of harmonic polynomial approximation error defined by 2.

Let uHR. Then the generalized order ρR(α,β,u) and generalized lower order λR(α,β,u) of u is defined as

ρR(α,β,u)=lim suprα(logM(r;u))α(logr),λR(α,β,u)=lim infrα(logM(r;u))α(logr),1λR(α,β,u)ρR(α,β,u).
5

Further, for 0<ρR<, we define the generalized type TR(α,β,u) of u as

T(α,β,u)=lim suprα(logM(r;u))β((φ(r))ρR).
8

The functions α,β and φ satisfy the conditions stated in Theorem B.

Now we prove our main results.

Theorem 4

α(x)Δ,β(x)Lo. Set G(x,c)=β1(cα(x)). If dG(x,c)d(logx)=O(1), as x for all c,c(0,), then for uHR can be continued to the entire harmonic function in space Rn,n3, for which generalized order

ρR(α,β,u)=lim supkα(k)β(logR[ERk(u)]1k).
9

Proof â–¼
Consider the complex valued functions
f1(z)=k=0(2ν)!2(2ν+1)!(k+2ν)2νERk(u)(zR)k=k=0bkzk(say),g(z)=k=14(2ν)!(k+2ν)2νERk(u)(zR)k=k=1ckzk(say).

From Lemma 3 we have

limk(bk)1k=  and limk(ck)1k=,
10

therefore, f1(z) and g(z) represents entire functions of complex variable z. Further, we have

log(bk)1logRk[ERk(u)]1  as  k.

Using Theorem A, we get

lim suprα(logM(r;f1))β(logr)=lim supkα(k)β(logR[ERk(u)]1k).
11

If μ(r;f1) denotes the maximum term of f1(z) then by a result of Valiron [ 12 , p. 34 ] , we get logM(r;f1)logμ(r;f1) as r. From Lemma 1 we have

M(r;u)|Yo(ξ;u)|+4(2ν)!k=1(k+2ν)2νERk1(u)(rR)k

or

M(r;u)|Yo(ξ;u)|+M(r;g).
12

Now from Lemma 3 and 12 we have

μ(r;f1)M(r;u)|Yo(ξ;u)|+M(r;g).
13

Thus 12 gives

lim suprα(logM(r;f1))β(logr)lim suprα(logM(r;u))β(logr)lim suprα(logM(r;g))β(logr).
14

Now using 7, 11 and 14 we get 9.

Theorem 5

Let uHR be of generalized order ρR(α,β,u),0<ρR(α,β,u)<. Let the functions α,β and φ satisfy the conditions of Theorem B, then the function u can be continued to the entire harmonic function in space Rn,n3, for which generalized type

T(α,β,u)=lim suprα(logM(r;u))β((φ(r))ρR)=lim supkα(kρR)β[{φ(e1ρRR[ERk(u)]1k)}ρR].
15

Proof â–¼
Since αLo, we have from Theorem 4

α(logM(r;u))α(logM(r;f1))
16

and f1(z) is also an entire function of generalized order ρR(α,β,f1), now using Theorem B, we have

lim suprα(logM(r;f1))β((φ(r))ρR)=lim supkα(kρR)β[{φ(e1ρR|bk|1k)}ρR].
17

Since φ(x)Lo, we have

lim supkα(kρR)β[{φ(e1ρR|bk|1k)}ρR]=lim supkα(kρR)β[{φ(e1ρRR[ERk(u)]1k)}ρR].
18

The above relations 16, 17 and 18 with 8 together gives 15.

Theorem 6

Let uHR. Set G(x)=β1(α(x)). Then the function u can be continued to the entire harmonic function in space Rn,n3, for which generalized lower order

λR(α,β,u)=lim infrα(logM(r;u))β(logr)lim infkα(k)β(logR[ERk(u)]1k).
19

if the following condition satisfied:

For some function ξ(x) as x,β(xξ(x))β(ex)0,dG(x)d(logx)=O(1), as x,

If, in addition, ratio |ERk(u)ERk+1(u)| is a non decreasing function of k then inequality in the right hand side of 19 transforms into the equality.

Proof â–¼
We see that f1(z) is also of generalized lower order λR(α,β,f1) and
bkbk+1=[(k+1+2ν)(k+2ν)]2νERk(u)ERk+1(u)(Rz),r>eR

is a non decreasing function of k. Now using 10 and applying Theorem C to the function f1(z), we obtain

λR(α,β,f1)=lim infkα(k)β(log|bk|1k)=lim infkα(k)β(logR[ERk(u)]1k).

Remark 7

If α(x)=logx,β(x)=x in Theorem 4 and α(x)=β(x)=φ(x)=x in Theorem 5, we get the coefficient characterizations for the classical order and type of entire harmonic function u in space Rn,n3, in terms of harmonic polynomial approximation errors.

Remark 8

If α(x)=x,β(x)=x1ρR,φ(x)=xρR(x) in Theorem 5, where ρR(x) is the proximate order of harmonic function u such that x=θ(τ) is the function inverse to τ=xρR(x), we obtain the formula for the generalized type with respect to proximate order ρR(x).

Theorem 9

Let α(x)Ω, then necessary and sufficient conditions for uHR to be continued to the entire harmonic function in space Rn,n3 with generalized order ρR(α,α,u) is

lim suprα(logM(r;u))α(logr)1=lim supkα(k)α(logR[ERk(u)]1k),for  p=1,lim supkα(k)α(logR[ERk(u)]1k)lim suprα(logM(r;u))α(logr)lim supkα(k)α(logR[ERk(u)]1k)+1,for  p=2,3,.
Proof follows on the lines of Theorem 4 and using Theorem D.

Theorem 10

Let α(x)Ω, then the function uHR can be continued to the entire harmonic function in space Rn,n3, with generalized order ρR(α,α,u),1<ρR(α,α,u)<, is of generalized type TR(α,α,u) if, and only if

lim suprα(logM(r;u))[α(logr)]ρR=lim supkα(k)[α(logR[ERk(u)]1k)]ρR1,p=1,lim suprα(logM(r;u))[α(logr)]ρR=lim supkα(k)[α(logR[ERk(u)]1k)]ρR,p=2,3,

Proof follows on the lines of Theorem 5 and using Theorem E.

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