Spectral analysis of multivariate stationary random functions on some massive groups

The spectral representations for wide sense stationary multivariate random functions and for their covariance functions on two classes of additive vector groups are obtained under some assumptions about continuity of such functions. The first class is nuclear topological groups and the second class i...

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Datum:2007
Hauptverfasser: Ponomarenko, O., Perun, Y.
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spelling irk-123456789-45212009-11-25T12:00:42Z Spectral analysis of multivariate stationary random functions on some massive groups Ponomarenko, O. Perun, Y. The spectral representations for wide sense stationary multivariate random functions and for their covariance functions on two classes of additive vector groups are obtained under some assumptions about continuity of such functions. The first class is nuclear topological groups and the second class is additive group of real vector space equipped with the finite topology. 2007 Article Spectral analysis of multivariate stationary random functions on some massive groups / O. Ponomarenko, Y. Perun // Theory of Stochastic Processes. — 2007. — Т. 13 (29), № 4. — С. 177–182. — Бібліогр.: 9 назв.— англ. 0321-3900 http://dspace.nbuv.gov.ua/handle/123456789/4521 en Інститут математики НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description The spectral representations for wide sense stationary multivariate random functions and for their covariance functions on two classes of additive vector groups are obtained under some assumptions about continuity of such functions. The first class is nuclear topological groups and the second class is additive group of real vector space equipped with the finite topology.
format Article
author Ponomarenko, O.
Perun, Y.
spellingShingle Ponomarenko, O.
Perun, Y.
Spectral analysis of multivariate stationary random functions on some massive groups
author_facet Ponomarenko, O.
Perun, Y.
author_sort Ponomarenko, O.
title Spectral analysis of multivariate stationary random functions on some massive groups
title_short Spectral analysis of multivariate stationary random functions on some massive groups
title_full Spectral analysis of multivariate stationary random functions on some massive groups
title_fullStr Spectral analysis of multivariate stationary random functions on some massive groups
title_full_unstemmed Spectral analysis of multivariate stationary random functions on some massive groups
title_sort spectral analysis of multivariate stationary random functions on some massive groups
publisher Інститут математики НАН України
publishDate 2007
url http://dspace.nbuv.gov.ua/handle/123456789/4521
citation_txt Spectral analysis of multivariate stationary random functions on some massive groups / O. Ponomarenko, Y. Perun // Theory of Stochastic Processes. — 2007. — Т. 13 (29), № 4. — С. 177–182. — Бібліогр.: 9 назв.— англ.
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fulltext Theory of Stochastic Processes Vol.13 (29), no.4, 2007, pp.177–182 OLEKSANDER PONOMARENKO AND YURIY PERUN SPECTRAL ANALYSIS OF MULTIVARIATE STATIONARY RANDOM FUNCTIONS ON SOME MASSIVE GROUPS The spectral representations for wide sense stationary multivariate random functions and for their covariance functions on two classes of additive vector groups are obtained under some assumptions about continuity of such functions. The first class is nuclear topological groups and the second class is additive group of real vector space equipped with the finite topology. 1. Introduction The spectral theory of stationary random functions of second order on abelian locally compact groups is well developed. This theory is based on spectral representations of such random functions and their covariance functions in one-dimensional and multivariate cases [1]-[3]. Now actual problems are connected with obtaining similar results for weakly stationary random functions on abelian massive groups, i.e. groups which are not generally locally compact. We consider two classes of abelian massive groups in this paper. The first class is nuclear topological groups, which theory was developed in [4]- [6]. Second class is related with additive groups of general real vector spaces and corresponding results of harmonic analysis on such groups [7]. The objects of investigation in this paper are spectral representations for generalized wide sense stationary random functions in Hilbert space H on nuclear groups and real vector spaces and for their covariance functions. Under some assumptions of continuity for stationary random functions these spectral representations are obtained in the form of Fourier transforms of orthogonally scattered random measures in H and operator positive finite measures in H respectively. 2000 Mathematics Subject Classifications. Primary 60G10, 60G57. Key words and phrases. Stationary random functions in Hilbert space,nuclear group, real vector space, spectral representation 177 178 OLEKSANDER PONOMARENKO AND YURIY PERUN 2. Wide sense stationary random functions in Hilbert space H on abelian groups Let L2(Ω) be Hilbert space of all complex-valued random variables of second order, which defined on some probability space (Ω,F ,P) and H be a complex Hilbert space. Then the set L(H, L2(Ω)) of all linear continuous mappings of the space H into L2(Ω) may be considered as the set of gener- alized random elements of second order in H , which defined on (Ω,F ,P). Such generalized random elements may be realized as usual random ele- ments in some quasinuclear extension H− of the space H (see [3], [8]). Denote by B(H) Banach algebra of all linear bounded operators in H and denote by B+(H) the convex cone of all nonnegative Hermitian opera- tors in B(H). The expectation m = EΞ ∈ H and covariance operator [Ξ, Ψ] ∈ B(H) for generalized random elements Ξ, Ψ ∈ L(H, L2(Ω)) are uniquely determi- nated by the relations (x|m) = E(Ξx), ([Ξ, Ψ]x|y) = E(Ξx)(Ψy), x, y ∈ H, where (·|·) is an inner product in H . Note that [Ξ, Ψ] is sesquilinear form on L(H, L2(Ω)) and [Ξ, Ξ] ∈ B+(H). If dimH = d < ∞ and {ej}d j=1 is orthonormal basis in H , then random element Ξ ∈ L(H, L2(Ω)) may be identified with random vector ξ = {ξj}d j=1, with ξj = Ξej and expectation EΞ - with vector Eξ = {Eξj}d j=1 and covari- ance operator [Ξ, Ψ], Ψ ∈ L(H, L2(Ω)) - with matrix {Eξjϕk}d j,k=1, where ϕk = Ψek, k = 1, .., d. Definition 2.1 The (generalized) random function of second order Ξt, t ∈ T , in a Hilbert space H defined on set T is the family of generalized random elements Ξt ∈ L(H, L2(Ω)) indexed by t ∈ T . The mean function mt and covariance function Q(s, t) of Ξt, t ∈ T are defined by the equalities mt = EΞt, Q(t, s) = [Ξt, Ξs], t, s ∈ T. Note that Q is positive definite operator kernel on T , i.e. for all integers n ∈ N, elements tk ∈ T and vectors xk ∈ H, k = 1, ..n n∑ k=1 n∑ j=1 (Q(tk, tj)xk|xj) ≥ 0. Conversely, every positive definite operator kernel Q on T with values in B(H) is a covariance function of some (in particulary gaussian) generalized random function of second order Ξt, t ∈ T (see [3]). Let G be some Abelian group with operation which is written as addi- tion. RANDOM FIELDS WITH ISOTROPIC PROPERTY 179 Definition 2.2 A random function of second order Ξg, g ∈ G on group G in H is called a wide-sense (or weakly) stationary if its mean function is constant mg = EΞg = m, g ∈ G and its covariance function Q(g, s) depends only on difference g − s: Q(g, s) = R(g − s), g, s ∈ G. (1) The function R(g) in (1) is called a covariance function of stationary function Ξg, g ∈ G. Note that definition of stationarity for random function Ξg, g ∈ G is equivalent to assumption of shift invariance its two moment function mg and Q(g, s). 3. Spectral representations for stationary random functions in H on nuclear group Let V be a real vector space and A, B be non-empty balanced subsets of V such that A is absorbed by B. For vector subspace Y of V we set d(A, B; Y ) = inf{t > 0 : A ⊆ tB + Y }. The Kolmogorov diameter dk of A with respect to B, k ∈ N is defined by the equality dk(A, B) = inf {d(A, B; X) : X}, where X ranges through the vector subspaces of V with dim(X) < k. Definition 3.1 A locally convex vector group is a real vector space V , equipped with a Hausdorff group topology such that the filter of zero- neighborhoods possesses a base of symmetric convex sets. A locally convex vector group V is called nuclear if for every balanced zero-neighborhood W there exists a balanced zero-neighborhood W0 such that W0 is absorbed by W and for all k ∈ N dk(W0, W ) ≤ k−1. Note that that every locally convex space is a locally convex vector group. Definition 3.2 An Abelian topological group is called nuclear if it is isomorphic to a Hausdorff quotient group of subgroup of some nuclear vector group. Note that the class of nuclear groups is a variety of topological Hausdorff groups, i.e., is closed under the formation of cartesian products, subgroups, Hausdorff quotients, and passage to isomorphic topological groups; it com- prises the classes of locally compact Abelian groups and nuclear locally convex spaces [6]. A topological vector space is a nuclear group if and only 180 OLEKSANDER PONOMARENKO AND YURIY PERUN if it is a nuclear locally convex space [6]. The further information of nuclear group is contained in [4]-[6]. Let G be a nuclear group with operation, which is written as addition, and with dual group Ĝ, equipped by admissible topology τ , and for g ∈ G 〈χ, g〉 denotes the value of character χ ∈ Ĝ on g. The ultra-weak operator topology on B(H) is the initial topology on B(H) with respect to family of linear functionals from B(H) into C of the form: A → tr(BA), A ∈ B(H), where B ranges through the set of trace class operators in B(H). Theorem 3.3 1. Let {Ξg, g ∈ G} be a generalized wide sense stationary random function on nuclear group G in H, which covariance function R(g) is continuous in ultra-weak topology on B(H).Then exists uniquely defined random L(H, L2(Ω))-valued strongly regular measure Φ on (Ĝ, τ) such that Ξg is the Fourier transform of Φ: Ξg = ∫ G 〈χ, g〉Φ(dχ), g ∈ G. (2) 2.The covariance function R(g) of the stationary random function Ξg ad- mits the spectral representation in form of the Fourier transform of B+(H)- valued finite strongly regular operator measure F on (Ĝ, τ): R(g) = ∫ G 〈χ, g〉F (dχ), g ∈ G. (3) The random spectral measure Φ of stationary random function Ξg is connected with its spectral measure F by the following relation: [Φ(Δ1), Φ(Δ2)] = F (Δ1 ∩ Δ2) (4) Proof. Denote by K(Ξ) the subspace of L2(Ω) generated by family of random variables {Ξgx : g ∈ G, x ∈ H}. Define on set of elements in K(Ξ) of the form ∑n j=1 Ξgj xj , which is dense in K(Ξ), the shift operators Ũs, s ∈ G by equalities Ũs( n∑ j=1 Ξgj xj) = n∑ j=1 Ξgj+sxj It is easy to see that these operators are isometric (because Ξg is sta- tionary function) and may extended by unique way to unitary operators Us, s ∈ G on K(Ξ). It is follows from the definition that the family {Us, s ∈ G} forms unitary representation of group G in K(Ξ). These unitary representation is connected with stationary function Ξg and its covariance function R(g) by the equalities Ξg = UgΞ0, Rg = Ξ∗ 0UgΞ0, g ∈ G, (5) RANDOM FIELDS WITH ISOTROPIC PROPERTY 181 where 0 is neutral element in G and Ξ∗ 0 : L2(Ω) → H is adjoint operator for Ξ0, and also is ultra-weak continuous. Then from the theorem 13.3 in [6] and theorem 15.4 in [7] it follows that unitary representation Ug, g ∈ G is the Fourier transform of uniquely defined strongly regular Radon spectral measure P on (Ĝ, τ) with values in B(K(Ξ)). Now spectral representations (2),(3) and property of orthogo- nality (4) are consequences of equalities (5) with Φ(Δ) = P (Δ)Ξ0, F (Δ) = Ξ∗ 0P (Δ)Ξo. Remark 3.4. If group G is k-space, i.e., if it is the direct limit of its compact subsets, than the assumption of ultra-weak continuity of covariance function R(g) in theorem 3.3 is equivalent to condition of weak continuity of R(G) in B(H). In particular, this is true for locally compact or metrizable groups G. The result of Remark 3.4 follows from corollary 1.9 and Remark 15.5 from [7]. 4. Spectral representations for stationary random function in H on vector space For real vector space, equipped with its finest locally convex topology, denote by V ∗ its topological dual space, equipped with weak -*-topology. Let Σ(V ∗) the coarsest σ-algebra on V ∗, which makes the point evalua- tions λ → λ(ν), λ ∈ V ∗ measurable for all vector ν ∈ V . Let us consider generalized wide sense stationary random function Ξν , ν ∈ V in Hilbert space H with covariance function R(ν−u) = [Ξν , Ξu], ν, u ∈ V . Theorem 4.1. Suppose that B(H)-valued covariance function R(ν), ν ∈ V of stationary random function Ξν , ν ∈ V in H is ultra-weakly continuous on each finite-dimensional subspace Y of space V . Then it exists such B+(H)- valued operator measure F on (V ∗, Σ(V ∗)) that R(g) admits the spectral representation in the form of the Fourier transform of measure F : R(ν) = ∫ V ∗ exp{iλ(ν)}F (dλ), ν ∈ V, (6) Itself stationary random function Ξν , ν ∈ V admits the spectral representa- tion Ξν = ∫ V ∗ exp{iλ(ν)}Φ(dλ), ν ∈ V, (7) where Φ is random L(H, L2(Ω)) -valued measure on (V ∗, Σ(V ∗)) with the following orthogonal property [Φ(Δ1), Φ(Δ2)] = F (Δ1 ∩ Δ2). (8) 182 OLEKSANDER PONOMARENKO AND YURIY PERUN Proof. One possible way to prove this theorem - it is using the method, which is similar to the approach of proving of theorem 3.4 above. This method is based on spectral expansion of unitary representation of additive group V ,which connected with stationary random function Ξν , ν ∈ V . We choose here another short way. First of all we use the fact that R(ν) is positive definite B(H)-valued function on V . Then through the generalized Bochner theorem for vector space (Theorem 15.6 from [7]) the spectral representation (6) is valid and we have the equality R(ν − u) = ∫ V ∗ exp{iλ(ν)}exp{iλ(u)}F (dλ), ν, u ∈ V. (9) Now by mean of application to expansion (9)Theorem 3 from (9) about integral spectral representations of generalized random function of second order in vector space we have representation (7) with property (8). References 1. Ponomarenko, A.I., Stochastic problems of optimization (in Russian). Kiev University Press, Kiev (1980). 2. Kakihara Y., Multidimensional second order stochastic processes. World Scientific, Singapore, New Jersey, London, Hong Kong, (1997). 3. Ponomarenko O.I., To spectral theory of infinite-dimensional homogeneous in wide sense random fields on groups. Vysnik of Kiev Univ., sec. math. and mech., N11, (1969), p.144–121. 4. Auβenhofer L., Contributions to the Duality theory on Topological groups and to the Theory of nuclear groups., Diss. Math. 389 (1999). 5. Auβbenhofer L., A survey on nuclear groups.pp. 1-30, in: Nuclear groups and Lie groups. Heldermann Verlag Lemgo (2001). 6. Banaszczyk W., Additive Subgroups of Topological Vector Space. Lecture Notes in Math., 1466, Springer Verlag, Berlin (1991). 7. Glöckner H., Positive definite functions on infinite-dimensional convex cones. Mem. of AMS, no. 789, vol 166 (2003). 8. Ponomarenko O.I., Random linear functionals of Second Order I. Theory Probab. and Math. Stat., N54, (1997), p.145–154. 9. Ponomarenko O.I., Integral representation of random functions with values in locally convex spaces. Theory Probab. and Math. Stat., N46, (1992), p.132–141. Department of Probability and Mathematical Statistics, Kiev Na- tional Tarasa Shevchenko University, Kiev, Ukraine E-mail: probability@mechmat.univ.kiev.ua Department of Auditing, National Bank of Ukraine, Kiev, Ukraine E-mail: perun@bank.gov.ua