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Volume 2010, Article ID 287647,5pages doi:10.1155/2010/287647

Research Article

A Version of Hilbert’s 13th Problem for

Infinitely Differentiable Functions

Shigeo Akashi and Satoshi Kodama

Department of Information Sciences, Faculty of Science and Technology, Tokyo University of Science, 2641 Yamazaki, Noda City, Chiba Prefecture 278-8510, Japan

Correspondence should be addressed to Shigeo Akashi,[email protected]

Received 29 December 2009; Accepted 4 March 2010

Academic Editor: Anthony To Ming Lau

Copyrightq2010 S. Akashi and S. Kodama. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

In 1957, Kolmogorov and Arnold gave a solution to the 13th problem which had been formulated by Hilbert in 1900. Actually, it is known that there exist many open problems which can be derived from the original problem. From the function-theoretic point of view, Hilbert’s 13th problem can be exactly characterized as the superposition representability problem for continuous functions of several variables. In this paper, the solution to the superposition representability problem for infinitely differentiable functions of several variables is given.

1. Superposition Representability and

Superposition Irrepresentability

In 1957, Kolmogorov and Arnold1solved Hilbert’s 13th problem asking if all continuous real-valued functions of several real variables can be represented as superpositions of continuous functions of fewer variables. Moreover, in 1964, Vitushkin2solved the problem, which had been derived from Hilbert’s 13th problem, asking if all finitely differentiable real-valued functions of several real variables can be represented as superpositions of finitely differentiable functions of fewer variables. In this paper, the solution to the superposition representability problem for infinitely differentiable functions of several variables is given.

LetFP3resp.,FP2be a set of functions of three variablesresp., two variables satisfying the condition P such as continuity or differentiability. Then, the superposition representability can be classified into the following two concepts.

Strong representabity: there exists a positive integerksatisfying that, for any function

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Weak representability: for any functionf ofFP3, there exists a positive integerkf such thatf can be represented as akf-time nested superposition constructed from several functions ofFP2.

Here, for a certain conditionP,Pis said to be stronglyresp., weaklyrepresentable, if strongresp., weakrepresentability under the conditionPholds. It is clear thatPis weakly representable, ifP is strongly representable. By the same way as above, the superposition irrepresentability can be also classified into the following two concepts.

Strong irrepresentability: there exists a function f of FP3 which cannot be represented as any finite-time nested superposition constructed from several functions of FP2.

Weak irrepresentability: for any positive integerk, there exists a functionfkofFP3 which cannot be represented as anyk-time nested superposition constructed from several functions ofFP2.

Here, for a certain conditionP,Pis said to be stronglyresp., weaklyirrepresentable, if strong resp., weak irrepresentability under the condition P holds. It is clear that P is weakly irrepresentable, if P is strongly irrepresentable. Moreover, it is also clear that P is weakly irrepresentable resp., representable, if P is not strongly representable resp., irrepresentable. Therefore, we can classify a condition such as continuity or differentiability into three cases.

Case 1. The case thatPis strongly representable.

Case 2. The case thatPis not only weakly representable but also weakly irrepresentable.

Case 3. The case thatPis strongly irrepresentable.

For example, if we take continuity as an example ofP, then owing to Kolmogorov and Arnold, we can say that continuity satisfies Case1. As for the proof, we refer to 1,3. Moreover, if we take analyticity as an example ofP, then, owing to Babenko, Erohin, and Akashi, we can say that analyticity satisfies Case3. As for the proof, we refer to4–7. If we take finite differentiability as an example ofP, then, owing to Vituskin, we can say that finite differentiability satisfies Case3. As for the proof, we refer to2. It is clear that polynomial condition satisfies Case 2. In the following section, this result will be formulated as a generalized relation between polynomial condition and infinite differentiability condition.

Recently, it is discussed that Hilbert’s 13th problem can be applied to the theory of multidimensional numerical data compression. Since the results stated above show that it is important for any functions of three variables to find the appropriate superpositions which can approximate most efficiently to the original function. Therefore, nonlinear theoretic approximation methods will play important roles in the theory of multidimensional numerical data compression. As for the nonlinear theoretic approximation methods, we can refer to Takahashi’s results8.

2. Weak Irrepresentability of Polynomial Condition

In this section, we prove that polynomial condition is weakly irrepresentable.

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Proof. Let i,j, and k be three nonnegative integers. Then, for any infinitely differentiable functionsf·,·andg·,·,·, we definecfi,j andcgi,j,kas

cfi,j ∂ijp ∂ix∂jy

x 0,y

0

,

cgi,j,k ∂ijkp ∂ix∂jy∂kz

x 0,y 0.z

0

,

2.1

respectively. Here, assume that there exists a positive integer satisfying that all the polynomials can be represented as-time nested superpositions. Then, the total number of infinitely differentiable functions of two variables, from which we use to construct the -time nested superposition, is less than or equal to 2−1. Letp·,·,·be a polynomial of three variables and{fp,m·,·; 1 ≤ m ≤ 2 −1}is a family of infinitely differentiable functions of two variables from which we use to construct the-time nested superposition ofp. For any positive integermwhich is less than or equal to 2−1 and for any nonnegative integerr, we have

cardcfp,mi,j;ij r

2Hr

r1!

r!1!

r1,

cardcpi,j,k;ijk r 3Hr

r2!

r!2!

r2r1 2 .

2.2

Since Taylor’s expansion theorem assures that, for any nonnegative integerr,{cpi,j,k; 0 ≤

ijkr}can be exactly characterized as 2m11{cfp,mi,j; 0≤ijr}, we have

cardcpi,j,k; 0≤ijkr≤ 2−1

m 1

cardcfp,mi,j; 0≤ijr

. 2.3

This implies that, for any positive integers, the following inequality holds:

s

r 0

r2r1 2 ≤

s

r 0

2−1r1. 2.4

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Remark 2.2. This lemma shows that polynomial condition satisfies Case 2, because this condition is also weakly representable.

3. Strong Irrepresentability of Infinite Differentiability Condition

In this section, we prove that infinite differentiability condition is strongly irrepresentable.

Theorem 3.1. There exists an infinitely differentiable function defined on 0,13 with values inR, which cannot be represented as any superposition constructed from several infinitely differentiable functions defined on0,12with values inR.

Proof. Letφ·be the function onRwith values inRdefined as

φx

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

0, x≤0,

exp

x1 − 1 1−x

, 0< x <1,

0, x≥1.

3.1

Then, it can be easily proved thatφ is infinitely differentiable. Moreover, for any positive integern, letpn·andqn·be the functions onRwith values inRdefined as

pnx 1−x

1− 1 2n−1

x

1− 1

2n

qnx pn1x,

3.2

respectively. For any positive integer n, Lemma 2.1assures that there exists a polynomial

hn·,·,·, which is defined on0,13and cannot be represented asn-time nested superposition constructed from several polynomials of two variables. Therefore, it is sufficient that the following functiong·,·,·, which is defined as

gx, y, z

n 0

hnqnx, qny, qnzφqnxφqnyφqnz, 0< x, y, z <1, 3.3

cannot be represented as any superposition constructed from several infinitely differentiable functions defined on0,12. Here, assume that, for a certain positive integerk,g·,·,·can be represented ask-time nested superposition. Then, for any positive integern,hn·,·,·is also characterized by the following equality:

hnx, y, z g

pnx, pny, pnz

φxφyφz , 0< x, y, z <1. 3.4

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Remark 3.2. Theorem 3.1shows that infinite differentiability condition satisfies Case3. For any real variablesx,y,z, it is clear thatxyyzzxcan be represented as the following two-time nested superposition:

xyyzzx xyzyz. 3.5

Actually, if we apply the same method as stated above to this polynomial, it can be proved thatxyyzzxcannot be represented as any one-time nested superposition.

Acknowledgments

The authors would like to express their hearty thanks to the referee who has given several pieces of suggestive advice to make the original manuscript more comprehensible, and they are also so thankful to Professor Anthony To-Ming Lau for having communicated several times with us in the course of reviewing procedure.

References

1 A. N. Kolmogorov, “On the representation of continuous functions of many variables by superposition of continuous functions of one variable and addition,”Doklady Akademii Nauk SSSR, vol. 114, pp. 953– 956, 1957Russian.

2 A. G. Vitushkin, “Some properties of linear superpositions of smooth functions,”Doklady Akademii Nauk SSSR, vol. 156, pp. 1003–1006, 1964.

3 G. G. Lorentz,Approximation of Functions, Holt Rinehart & Winston, New York, NY, USA, 1966.

4 K. I. Babenko, “Best approximations to a class of analytic functions,”Izvestiya Akademii Nauk SSSR. Seriya Matematicheskaya, vol. 22, pp. 631–640, 1958Russian.

5 V. D. Erohin, “Asymptotic theory of theε-entropy of analytic functions,”Doklady Akademii Nauk SSSR, vol. 120, pp. 949–952, 1958Russian.

6 S. Akashi, “A version of Hilbert’s 13th problem for analytic functions,” The Bulletin of the London Mathematical Society, vol. 35, no. 1, pp. 8–14, 2003.

7 S. Akashi, “A version of Hilbert’s 13th problem for entire functions,”Taiwanese Journal of Mathematics, vol. 12, no. 6, pp. 1335–1345, 2008.

References

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