metric entropy of subsets of absolutely convergent fourier series

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Journal of Approximation Theory 110, 229235 (2001) Metric Entropy of Subsets of Absolutely Convergent Fourier Series E. S. Belinsky Department of Computer Science, Mathematics and Physics, University of the West Indies, Cave Hill Campus, St. Michael, Barbados E-mail: ebelinskyuwichill.edu.bb Communicated by Allan Pinkus Received June 1, 2000; accepted in revised form January 5, 2001; published online April 27, 2001 We estimate the metric entropy of compact subsets of the algebra A of absolutely convergent Fourier series 2001 Academic Press Key Words: =-entropy; absolutely convergent Fourier series. In 1967, G. G. Lorentz wrote in his paper [Lor, p. 922] ``An interesting problem is to derive, from the behaviour of H = ( K), properties of the Fourier coefficients of some, or of most functions f # K, K/L p or K/C. To give only one example: Is it true, for a subset K of C, that H = ( K) Const(1= ) 2 implies the existence of a function f # K whose Fourier series is not absolutely convergent?'' The easy answer to this particular question is ``No''. Indeed, take K con- sisting of functions : m e imx , m=1, 2, ... where : m is a sequence of numbers which decreases slowly enough to zero. This class is obviously compact, and all functions are well separated, hence its entropy could be very big. Nevertheless it seems interesting to estimate the entropy of compact sub- sets of the set A of continuous functions with absolutely convergent Fourier series. Let us recall the definitions. The class H : is the set of real or complex- valued, 2?-periodic functions f such that f (0)=0 and &2 l h f & | h | : where the difference of integer order l >: is taken with the step h. We denote by A p , 0<p <2 the class of functions f ( x) such that the sequence of the Fourier coefficients belongs to the space l p , and such that & f & A p = { : & | f ( & )| p = 1p 1. For the notion of =-entropy see for example [Ti, p. 274] or [Pis, Ch. 5]. Let K be a compact set in a Banach space X. The =-entropy H = ( K; X) (or doi:10.1006jath.2000.3567, available online at http:www.idealibrary.com on 229 0021-904501 35.00 Copyright 2001 by Academic Press All rights of reproduction in any form reserved.

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Page 1: Metric Entropy of Subsets of Absolutely Convergent Fourier Series

Journal of Approximation Theory 110, 229�235 (2001)

Metric Entropy of Subsets of AbsolutelyConvergent Fourier Series

E. S. Belinsky

Department of Computer Science, Mathematics and Physics, University of the West Indies,Cave Hill Campus, St. Michael, Barbados

E-mail: ebelinsky�uwichill.edu.bb

Communicated by Allan Pinkus

Received June 1, 2000; accepted in revised form January 5, 2001;published online April 27, 2001

We estimate the metric entropy of compact subsets of the algebra A of absolutelyconvergent Fourier series � 2001 Academic Press

Key Words: =-entropy; absolutely convergent Fourier series.

In 1967, G. G. Lorentz wrote in his paper [Lor, p. 922] ``An interestingproblem is to derive, from the behaviour of H= (K), properties of theFourier coefficients of some, or of most functions f # K, K/L p or K/C.To give only one example: Is it true, for a subset K of C, that H= (K)�Const(1�=)2 implies the existence of a function f # K whose Fourier series isnot absolutely convergent?''

The easy answer to this particular question is ``No''. Indeed, take K con-sisting of functions :m eimx, m=1, 2, ... where :m is a sequence of numberswhich decreases slowly enough to zero. This class is obviously compact,and all functions are well separated, hence its entropy could be very big.

Nevertheless it seems interesting to estimate the entropy of compact sub-sets of the set A of continuous functions with absolutely convergentFourier series.

Let us recall the definitions. The class H: is the set of real or complex-valued, 2?-periodic functions f such that f� (0)=0 and &2 l

h f &��|h|: wherethe difference of integer order l>: is taken with the step h.

We denote by Ap , 0<p<2 the class of functions f (x) such that thesequence of the Fourier coefficients belongs to the space lp, and such that

& f &Ap={:

&

| f� (&)| p=1�p

�1.

For the notion of =-entropy see for example [Ti, p. 274] or [Pis, Ch. 5].Let K be a compact set in a Banach space X. The =-entropy H= (K; X) (or

doi:10.1006�jath.2000.3567, available online at http:��www.idealibrary.com on

2290021-9045�01 �35.00

Copyright � 2001 by Academic PressAll rights of reproduction in any form reserved.

Page 2: Metric Entropy of Subsets of Absolutely Convergent Fourier Series

simply H(K, =)) is the logarithm to the base two of the number of pointsin the minimal =-net for K. We use also the inverse characteristic, so-calledentropy numbers given by

em (K; X)=inf {=: _x1 , ..., x2m : K/ .2m

j=0

(xj+=BX)= ,

where the infimum is taken over all = such that K can be covered by 2m

open balls =BX of radius = (we denote by BX the open unit ball of theBanach space X).

We write an<<bn if there exists constant C, independent of n such thatan�Cbn .

We start with the result for the classical Wiener algebra of absolutelyconvergent Fourier series A=A1 .

Theorem 1. The following estimates hold

H= (A & H: ; L�)&1=2 , :=1�2

log(1�=)=2 <<H= (A & H: ; L�)<<

log2 (1�=)=2 , 0<:<1�2.

Remark. The case :>1�2 is not interesting because by the classicalBernstein theorem (see, for example [Zy, Ch. 6, Th. 3.1]) we have theembedding H: /A and the order of the entropy of this class H= (H: ; L�)&=&1�: is well known [KoT], (see also [Lor. p. 920]).

Remark. If H: & AI denotes the class H: functions which coincide witha function from A on an interval I, |I |<2? then

H= (H: & AI ; L�)&=&1�:, 0<:<1�2.

Indeed, the above estimate follows from the embedding H: & AI /H: .In order to construct the set of =-separated functions for the estimate frombelow, we can take each function from the corresponding set on [0, 2?]"I,and extend each function by zero onto I. K

Proof of the theorem. Let :=1�2. The estimate from above followsdirectly from the obvious embedding A & H1�2 /H1�2 and the classicalresult (see the reference above). We prove the estimate from below. For this

230 E. S. BELINSKY

Page 3: Metric Entropy of Subsets of Absolutely Convergent Fourier Series

we construct a big enough set of =-separated functions. Let ==- ?�n, andconsider the function

0, |x|>h

*h (x)={1, x=0

linear, 0<|x|<h

extended periodically outside of [&?, ?]. Take h=?�n. Then the function- h *h (x) belongs to H1�2 . We consider the functions

Ft (x)=- h :n

k=0

rk (t) *h (x&(2k+1) h),

where rk (t)=sgn sin 2k?t are the Rademacher functions. For each t, thefunction Ft (x) # H1�2 , and if |t1&t2 |> ?

2n then

&Ft1&Ft2

&�>>- h.

Therefore, we have a set of 2n =-separated functions. We have to check onlythat each one is in the space A.

The Fourier series of Ft (x) is

Ft (x)= :n

k=0

h3�2 _12

+ :�

&=1\sin &h

&h +2

rk (t) cos &(x+(2k+1) h)&=h3�2 _1

2+ :

&=1\sin &h

&h +2

\ :n

k=0

rk (t) cos &(x+(2k+1) h)+& .

Hence

&Ft&A�h3�2 :�

&=0\sin &h

&h +2

} :n

k=0

rk (t) cos &(x+(2k+1) h) }.Therefore by the Chebyshev inequality

m[t: &Ft&A> y]�1y |

1

0h3�2 :

&=0 \sin &h

&h +2

_} :n

k=0

rk (t) cos &(x+(2k+1) h) } dt.

231METRIC ENTROPY ESTIMATES

Page 4: Metric Entropy of Subsets of Absolutely Convergent Fourier Series

The orthogonality of the Rademacher functions, and two simple inequalitiessin x�x and |sin x|�1 give us the estimate

m[t: &Ft&A> y]�Const

y.

If we choose y such that the right-hand part �1�2 then for at least half ofthe constructed functions we have

&Ft&A< y.

The estimate is proved.

Remark. The same estimate from below can be obtained from thefollowing simple observation. The set A & H1�2 contains the set of all tri-gonometric polynomials Tn (x)=� |k|�n ckeikx such that &Tn&��n&1�2.Hence, considering the (2n+1)-dimensional subspace of L� with the coef-ficients ck as coordinates, covering this subset of it with the balls bystandard way, comparing the Euclidean volumes in this subspace, andchoosing the optimal n we obtain the estimate.

Let us consider the case 0<:<1�2. Take ==n&1�2. The estimate fromabove is an easy consequence of the following three facts.

(a) Classical approximation by Fejer means of the Fourier series(see, for example [Zy, Ch. 3, Th. 3.15])

& f (x)&Fn ( f; x)&�<<n&:.

We take Fejer means of order m=n1�2:, reducing the problem to theestimate of the entropy of the trigonometric polynomials of order �2m.

(b) The best approximation by trigonometric polynomials with aprescribed number of harmonics:

Lemma [DvT]. For every trigonometric polynomial Tm=�mk=&m ck eikx

there exists a trigonometric polynomial tn with n harmonics such that

&Tm&tn&��{n1�2&1�p- lg (m�n) &Tm&Ap

m1&1�pn&1�2- lg (m�n) &Tm&Ap

0<p�11<p�2.

This reduces the problem to the estimate of the entropy of the unit ballin the space of trigonometric polynomials with n harmonics.

(c) Estimate of =-entropy of the unit ball of finite dimensional space.

232 E. S. BELINSKY

Page 5: Metric Entropy of Subsets of Absolutely Convergent Fourier Series

Lemma [KoT]. See also [Pi, p. 63] If X is an n-dimensional space, then

n log1=

�H= (BX ; X)�n log \1+2=+ .

Finally we apply this estimate to the unit ball of each subspace andcount the possible number of subspaces, which is at most ( m

n ).Let us prove the estimate from below. With the same ==n&1�2 we con-

struct the =-distinguished set of functions by a linear combination of shiftsof the *h (x). Take h=?�n1�2:. Divide [0, 2?] into n1�2:+1 equal intervalsby n1�2: points xj . Then the function h:*h (x) # H: . Let

Ft= :n

j=1

h:rj (t) *h (x&xnj),

where n points xnjare chosen randomly among all n1�2: knots. Then

&Ft&A<<2?n1�2 _h+h :

&=1\sin &h

&h +2

} :n

j=0

rj (t) cos &xj }& .

We choose signs (value t) such that &Ft&A�Const. It is obvious that fortwo different functions

&Ft&F $t &��n&1�2.

The total number of functions is ( n1�2:

n ), which can be estimated from belowby n(1�2:&1) n. This gives the estimate from below.

Let us denote by H q: the class of functions f such that f� (0)=0 and

&2 lh f &q�|h|:, where the difference of integer order l>: is taken with the

step h.

Corollary. Suppose 2<q<�. Then

log(1�=)=2 <<H= (A & H q

: ; L�)<<log2 (1�=)

=2 ,1q

<:�12

.

Proof. Indeed, the result follows directly from the embeddings H: /H q

: /H:&1�q (the left-hand part is obvious, for the right-hand part see, forexample [Nik, Ch. 6]) and Theorem 1.

The order of the entropy of the subsets of Ap , 0<p<1 is also inde-pendent of :. We formulate the result in terms of the entropy numbers.

233METRIC ENTROPY ESTIMATES

Page 6: Metric Entropy of Subsets of Absolutely Convergent Fourier Series

Theorem 2. The following estimates hold

em (Ap & H: ; L�)&1

m: , :=1p

&12

\log mm +

1�p&1�2

<<em (Ap & H: ; L�)

<<\log mm +

1�p&1�2

- log m, 0<:<1p

&12

.

The proof of the above estimate is the same as in Theorem 1. To provethe estimate from below, the modified function *� h=*h V } } } V *h is needed.The convolution is taken a number of times sufficient for the necessarysmoothness of the function *� h .

Another fact which has to be taken into account is that

&*h&Ap&h1&(1�p).

This can be checked by simple calculation.But the case of Ap when 1<p<2 is completely different, here the order

of entropy depends on the smoothness of the functions.

Theorem 3. The following estimates hold

em (Ap & H: ; L�) &1

m: , :=1p

&12

\log mm +

(:�2)�(:+1�p$)

<<em (Ap & H: ; L�)

<<\log mm +

(:�2)�(:+1�p$)

- log m,

0<:<1p

&12

,

where as usual 1�p+1�p$=1.

The proof of this statement follows the same scheme, but the second lineof the [DvT] Lemma has to be applied for the above estimates.

The same proof can be used for the classes of functions of small smooth-ness. Let H :

| be the class of functions f such that & f (x)& f (x+h)&��(log 1�h)&: for fixed 0<:<� and arbitrary 0<h<2?.

234 E. S. BELINSKY

Page 7: Metric Entropy of Subsets of Absolutely Convergent Fourier Series

Theorem 4. The following estimates hold

m&:�2:+1<<em (H :| & A; L�)<<m&:�2:+2.

ACKNOWLEDGMENTS

I am grateful to H. Millington and the referee for their careful reading of the manuscript.Their critique undoubtedly made the presentation better.

REFERENCES

[DvT] R. DeVore and V. Temlyakov, Nonlinear approximation by trigonometric sums,Fourier Anal. Appl. 2 (1995), 29�48.

[Lor] G. Lorentz, Metric theory and approximation, Bull. Amer. Math. Soc. 72 (1966),903�937.

[KoT] A. N. Kolmogorov and V. M. Tikhomirov, =-entropy and =-capacity of sets in func-tional spaces, Uspekhi Mat. Nauk 14 (1959), 3�86 [In Russian]; English translationin Amer. Math. Soc. Transl. 17 (1961), 277�364.

[Mk] Y. Makovoz, On trigonometric n-widths and their generalizations, J. Approx. Theory41 (1984), 361�366.

[Nik] S. Nikolskii, ``Approximation of Functions of Several Variables and EmbeddingTheorems,'' Springer-Verlag, New York, 1969.

[Pis] G. Pisier, ``The Volume of Convex Bodies and Banach Space Geometry,'' CambridgeUniv. Press, Cambridge, UK, 1989.

[Ti] V. Tikhomirov, ``Some Questions of Approximation Theory,'' Moscow University,Moscow, 1976. [In Russian]

[Zy] A. Zygmund, ``Trigonometric Series,'' 2nd ed., Cambridge Univ. Press, Cambridge,UK, 1959.

235METRIC ENTROPY ESTIMATES