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TRANSFORM OF FUNCTIONS OF BOUNDED VARIATION

N.S. BARNETT, S.S. DRAGOMIR, AND G. HANNA

Abstract. In this paper we point out an approximation for the Fourier trans-form for functions of bounded variation and study the approximation error of certain associated quadrature rules.

1. Introduction

TheFourier Transform has applications in a wide variety of fields in science and engineering [1, p. xi].

In this paper, by use of some integral identities and inequalities developed in [4](see also [5]), we point out some approximations of the Fourier transform in terms of the complex exponential meanE(z, w) (see Section 2) and study the error of approximation for different classes of mappings of bounded variation defined on finite intervals.

Letg: [a, b]→Rbe a Lebesgue integrable mapping defined on the finite interval [a, b] andF(g) its Fourier transform, i.e.,

F(g) (t) :=

Z b

a

g(s)e−2πitsds.

The inverse Fourier transform ofgwill also be considered, and will be defined by

F−1(g) (t) :=

Z b

a

g(s)e2πitsds.

The following inequality was obtained in [2]:

Theorem 1. Letg: [a, b]→Rbe an absolutely continuous mapping on[a, b].Then

we have the inequality

F(g) (x)−E(−2πixa,−2πixb)

Z b

a

g(t)dt

≤               

1 3kg

0k

∞(b−a)

2

, ifg0∈L∞[a, b],

2 1

q

[(q+1)(q+2)]1q

(b−a)1+1q kg0k

p, ifg

0L

p[a, b] ;1p +1q = 1, p >1,

(b−a)kg0k1

;

Date: May 21, 2003.

1991Mathematics Subject Classification. Primary 42Xxx; 26D15; Secondary , 41A55.

Key words and phrases. Fourier Transform, Analytic Inequalities, Adaptive Quadrature Formulae.

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for all x∈[a, b], x6= 0, whereE is the exponential mean of two complex numbers, that is,

E(z, w) :=

  

ezew

z−w if z6=w exp (w) if z=w

, z, w∈C.

The following inequality for a more general class of functions was pointed out in [3].

Theorem 2. Let g : [a, b] → R be a measurable mapping on [a, b], then we have

the inequality:

F(g) (x)−E(−2πixa,−2πixb)

Z b

a

g(s)ds

≤               

3 |x|(b−a) 2

kgk if g∈L∞[a, b] ;

21+ 1qπ(ba)1+ 1q

[(q+1)(q+2)]1q

|x| kgkp if g∈Lp[a, b], p >1, p1+1q = 1;

2π|x|(b−a)kgk1 if g∈L1[a, b] ; for allx∈[a, b],x6= 0.

It is the main aim of this paper to point out some new inequalities for the Fourier transform of functions of bounded variation. Error bounds for some associated quadrature formulae are also mentioned.

2. Some Inequalities

The following inequality holds:

Theorem 3. Let g : [a, b]→R be a mapping of bounded variation on[a, b], then

we have the inequality

(2.1)

F(g) (x)−E(−2πixa,−2πixb)

Z b

a

g(s)ds

≤3

4(b−a) b

_

a (g)

for allx∈[a, b], x6= 0, whereWb

a(g)is the total variation of g on[a, b].

Proof. Using the integration by parts formula for the Riemann-Stieltjes integral, we have (see also [4]) that

(2.2)

Z t

a

(s−a)dg(s) = (t−a)g(t)− Z t

a

g(s)ds

and

(2.3)

Z b

t

(s−b)dg(s) = (b−t)g(t)− Z b

t

g(s)ds,

for allt∈[a, b].

Adding (2.2) and (2.3) and dividing by (b−a), we deduce the representation [4]: (2.4) g(t) = 1

b−a

Z b

a

g(s)ds+ 1 b−a

Z t

a

(s−a)dg(s) + 1 b−a

Z b

t

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for allt∈[a, b],which is itself of interest. Assume thatx∈[a, b], x6= 0, then,

F(g) (x) =

Z b

a

g(t)e−2πixtdt (2.5) = Z b a " 1 b−a

Z b

a

g(s)ds+ 1 b−a

Z t

a

(s−a)dg(s)

+ 1

b−a

Z b

t

(s−b)dg(s)

#

e−2πixtdt

= 1

b−a

Z b

a

g(s)ds

Z b

a

e−2πixtdt

+ 1

b−a

Z b

a

Z t

a

(s−a)dg(s)

e−2πixtdt

+ 1

b−a

Z b

a

Z b

t

(s−b)dg(s)

!

e−2πixtdt

=E(−2πixa,−2πixb)

Z b

a

g(s)ds

+ 1

b−a

Z b

a

Z t

a

(s−a)dg(s)

e−2πixtdt

+ 1

b−a

Z b

a

Z b

t

(s−b)dg(s)

!

e−2πixtdt,

as

Z b

a

e−2πixtdt= (b−a)E(−2πixa,−2πixb). Using the properties of modulus, we have, by (2.5),that

F(g) (x)−E(−2πixa,−2πixb)

Z b

a

g(s)ds

(2.6) ≤ 1

b−a

Z b a Z t a

(s−a)dg(s)

e−2πixtdt

+ 1

b−a

Z b a Z b t

(s−b)dg(s)

!

e−2πixtdt

≤ 1

b−a

Z b a Z t a

(s−a)dg(s)

e−2πixt

dt

+ 1

b−a

Z b a Z b t

(s−b)dg(s)

e−2πixt

dt

= 1

b−a

Z b a Z t a

(s−a)dg(s)

dt+ 1 b−a

Z b a Z b t

(s−b)dg(s)

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It is well known that ifp: [c, d]→Ris continuous andv: [c, d]→Ris of bounded

variation on [c, d],then the Riemann-Stieltjes integral Rd

c p(x)dv(x) exists and

(2.7) Z d c

p(x)dv(x)

≤ sup x∈[c,d]

|p(x)|

d

_

c (v).

Applying (2.7) on the intervals [a, t] and [t, b], we deduce that

Z t a

(s−a)dg(s)

≤(t−a) t

_

a (g),

Z b t

(s−b)dg(s)

≤(b−t) b

_

t (g)

and further that,

Z t a

(s−a)dg(s)

+ Z b t

(s−b)dg(s)

≤(t−a) t

_

a

(g) + (b−t) b

_

t (g)

≤ max

t∈[a,b]{t−a, b−t}

" t

_

a (g) +

b

_

t (g)

#

= b

_

a (g)

1

2(b−a) +

t−a+b

2 .

Using (2.6),

F(g) (x)−E(−2πixa,−2πixb)

Z b

a

g(s)ds

≤ 1

b−a b

_

a (g)

Z b

a

1

2(b−a) +

t−a+b

2 dt = 3 4(b−a)

b

_

a (g),

as a simple calculation shows that

Z b a

t−a+b

2

dt= (b−a) 2

4 ,

and the theorem is completely proved.

Remark 1. If we consider the inverse Fourier transform

F−1(g) (x) =

Z b

a

g(t)e2πixtdt,

then, by a similar argument, we can prove that

(2.8)

F−1(g) (x)E(2πixa,2πixb)

Z b

a

g(s)ds

≤ 3

4(b−a) b

_

a

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The following corollaries are a natural consequence.

Corollary 1. Let g: [a, b]→R be a monotonic mapping on[a, b]. Then we have

the inequality

(2.9)

F(g) (x)−E(−2πixa,−2πixb)

Z b

a

g(s)ds

≤3

4(b−a)|g(b)−g(a)|, for allx∈[a, b], x6= 0.

The proof is obvious by Theorem 3, taking into account that every monotonic mapping is of bounded variation andWb

a(g) =|g(b)−g(a)|.

Corollary 2. Letg: [a, b]→Rbe an L−Lipschitzian mapping on[a, b],i.e.,

(L) |g(t)−g(s)| ≤L|t−s| for allt, s∈[a, b]. Then we have the inequality

(2.10)

F(g) (x)−E(−2πixa,−2πixb)

Z b

a

g(s)ds

≤ 3

4L(b−a) 2

.

The proof is obvious by Theorem 3, taking into account that ifg: [a, b]→Ris L−Lipschitzian, thenLis of bounded variation on [a, b] andWb

a(g)≤L(b−a). 3. A Numerical Quadrature Formula

LetIn :a=x0 < x1< ... < xn−1 < xn =bbe a division of the interval [a, b], puthk:=xk+1−xk(k= 0, ..., n−1) andν(h) := max{hk|k= 0, ..., n−1}.Define the sum (see also [2] and [3])

(3.1) E(g, In, x) := n−1

X

k=0

E(−2πixxk,−2πixxk+1)×

Z xk+1

xk

g(t)dt,

wherex∈[a, b], x6= 0.

The following approximation theorem holds.

Theorem 4. Let g: [a, b]→Rbe a mapping of bounded variation on [a, b].Then

we have the quadrature rule

(3.2) F(g) (x) =E(g, In, x) +R(g, In, x) ;

where E(g, In, x)is as defined in (3.1) and the remainder R(g, In, x) satisfies the estimate

(3.3) |R(g, In, x)| ≤

3 4ν(h)

b

_

a (g).

Proof. Applying Theorem 3 on every subinterval [xk, xk+1],we can state that

Z xk+1

xk

g(t)e−2πixtdt−E(−2πixxk,−2πixxk+1)×

Z xk+1

xk

g(t)dt

≤ 3

4hk xk+1

_

xk

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for allk∈ {0, ..., n−1}andx∈[a, b], x6= 0.

Summing over ifrom 0 to n−1 and using the generalized triangle inequality, we can state that

|R(g, In, x)|=|F(g) (x)− E(g, In, x)|

≤3

4 n−1

X

k=0 hk

xk+1

_

xk

(g)≤3

4ν(h) n−1

X

k=0 xk+1

_

xk

(g)

=3 4ν(h)

b

_

a (g),

and the theorem is proved.

In practical applications, it is more convenient to consider the equidistant par-titioning of the interval [a, b].Thus, let

In:xj=a+j· b−a

n , j= 0, ..., n;

be an equidistant partition of [a, b], and define the sum (see also [2] and [3])

(3.4) En(g, x) := n−1

X

k=0 E

−2πix

a+k· b−a

n

,−2πix

a+ (k+ 1)· b−a

n

×

Z a+(k+1)·b−na

a+k·b−a n

g(t)dt.

The following corollary of Theorem 4 holds.

Corollary 3. Letg be as defined in Theorem 4. Then we have (3.5) F(g) (x) =En(g, x) +Rn(g, x),

where En(g, x)approximates the Fourier transform at any point x∈[a, b], x6= 0. The error of approximation Rn(g, x)satisfies the bound

(3.6) |Rn(g, x)| ≤

3

4n(b−a) b

_

a (g),

for allx∈[a, b], x6= 0.

Remark 2. If we know the total variation Wb

a(g) of g on [a, b] and would like to approximate the Fourier transformF(g) (x)by the adaptive quadrature formula

En(g, x)with an error less than a given ε >0,we have to divide the interval [a, b] into at leastnε∈Npoints, where

nε:=

"

3 (b−a) 4ε

b

_

a (g)

#

+ 1,

and[r] denotes the integer part of r∈R.

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Corollary 4. Letg: [a, b]→Rbe a monotonic mapping on[a, b].Then we have the

quadrature formula (3.2) where the remainder is such that it satisfies the estimate

(3.7) |R(g, In, x)| ≤ 3

4ν(h)|g(b)−g(a)|, x∈[a, b], x6= 0.

In particular, ifIn is taken to be equidistant, then we have the formula(3.5),where the remainderRn(g, x)satisfies the estimate

(3.8) |Rn(g, x)| ≤

3 (b−a)

4n |g(b)−g(a)|, x∈[a, b], x6= 0. A similar result holds for Lipschitzian mappings.

Corollary 5. Letg: [a, b]→Rbe a Lipschitzian mapping with the constantL >0.

Then we have the quadrature formula(3.2)where the remainder satisfies the bound

(3.9) |R(g, In, x)| ≤ 3 4L

n−1

X

i=0 h2i ≤ 3

4L(b−a)ν(h).

In particular, ifIn is chosen to be equidistant, then we have the formula(3.5)where the remainderRn(g, x)is such that it satisfies the inequality

(3.10) |Rn(g, x)| ≤

3L(b−a)2

4n .

4. Some Numerical Experiments

In the following we numerically illustrate the approximation for the Fourier trans-form provided by

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,

E(g, In, x) (4.1)

: =

n−1

X

k=0 E

2πix

a+k·b−a

n

,−2π i

a+ (k+ 1)b−a n

×

Z a+(k+1)b−na

a+k·b−a n

g(t)dt.

If we consider, for instance, the exponential functiong(t) = exp(t), t∈[−1,1], then the plots of the error rn(x) := |Rn(g, x)|, x∈[−1,1] for n= 1, n= 10 and n= 100,respectively, are depicted in Figure 1, 2 and 3.

References

[1] P.L. BUTZER and R.J. NESSEL,Fourier Analysis and Approximation Theory,I, Academic Press, New York and London, 1971.

[2] N.S. BARNETT and S.S. DRAGOMIR, An Approximation for the Fourier Transform of Ab-solutely Continuous Mappings,RGMIA Res. Rep. Coll.,5(2002), Supplement, Article 33.[ON LINE: http://rgmia.vu.edu.au/v5(E).html],Proc. 4th Int. Conf. on Modelling and Simula-tion, Victoria University, Melbourne, 2002, 351-355.

[3] S.S. DRAGOMIR, Y.J. CHO and S.S. KIM, An approximation for the Fourier transform of Lebesgue integrable mappings,”Inequality Theory & Applications”, Volume 2, (Eds. Y.J. Cho, J.K. Kim and S.S. Dragomir), Nova Science Publishers, New York, to appear.

[4] S.S. DRAGOMIR, On the Ostrowski’s integral inequality for mappings with bounded variation and applications,Mathematical Inequalities and Applications,4(1) (2001), 59-66.

[5] S.S. DRAGOMIR and TH. M. RASSIAS (Eds.),Ostrowski Type Inequalities and Applications in Numerical Integartion, Kluwer Academic Publishers, Dordrecht/Boston/London, 2002.

School of Computer Science and Mathematics, Victoria University of Technology, PO Box 14428, Melbourne City, MC 8001 Australia

References

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