Abstract Generated abstract
This note studies linear extrapolation for discrete homogeneous random fields indexed by one spatial and one temporal integer variable. Using the spectral function of the field, it gives necessary and sufficient conditions for regularity and singularity, including logarithmic integrability criteria and an equivalent factorization form. It derives formulas for the mean square error of extrapolation several time steps ahead, analogous to Kolmogorov’s formulas for stationary sequences. The paper also characterizes fields of Markov type through their spectral representation and gives the corresponding form of the one-step linear projection for regular Markov-type fields.
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MATHEMATICS
TSIAN TSE-PEI
ON LINEAR EXTRAPOLATION OF A DISCRETE HOMOGENEOUS RANDOM FIELD
(Presented by Academician A. N. Kolmogorov on 20 VIII 1956)
Definition. A discrete homogeneous random field is a family of complex random variables \(x(s,t)\), where \(s,t\) are integers and \(-\infty < s < \infty\), \(-\infty < t < \infty\), such that \(M|x(s,t)|^2 < \infty\) and
\[ B_x(s,t)=M[x(s+m,t+n)\overline{x(s+t)}] \tag{1} \]
does not depend on \(m\) and \(n\).
The function \(B_x(s,t)\) is, obviously, positive definite and therefore (see, for example, \(\left({}^{1}\right)\)):
\[ B_x(s,t)=\int_{-\pi}^{\pi}\int_{-\pi}^{\pi} e^{i(s\lambda+t\mu)}\,dF_x(\lambda,\mu), \tag{2} \]
where \(F_x(\lambda,\mu)\) is an unnormalized two-dimensional distribution function, called the spectral function of the field \(\{x(s,t)\}\).
Let \(H_x\) be the minimal closed linear subspace containing all the variables \(x(s,t)\), and let \(H_x(t)\) be the minimal closed linear subspace containing all \(x(m,n)\) with \(-\infty < m < \infty\) and \(n \le t\). Denote
\[ S_x=\bigcap_t H_x(t). \tag{3} \]
If
\[ S_x=H_x, \tag{4} \]
then the homogeneous random field \(\{x(s,t)\}\) will be called singular.
Every element \(x(s,t)\) of the field \(\{x(s,t)\}\) is uniquely represented in the form of the sum
\[ x(s,t)=\eta(s,t)+\xi(s,t), \tag{5} \]
where \(\xi(s,t)\in H_x(0)\), and \(\eta(s,t)\) is orthogonal to \(H_x(0)\).
Put
\[ \rho(s,t)=\|\eta(s,t)\|^2. \tag{6} \]
Obviously,
\[ \rho(s,t)=\rho(s',t)=\rho(t), \]
\[ \rho(t_1)\leq \rho(t_2)\quad \text{for } t_1\leq t_2, \tag{7} \]
so that there exists
\[ \lim_{t\to+\infty}\rho(t)=\sigma_\infty^2. \tag{8} \]
If
\[ \sigma_\infty^2=M|x(s,t)|^2=\|x\|^2, \tag{9} \]
then the homogeneous random field \(\{x(s,t)\}\) will be called regular (cf. \(\left({}^{1-3}\right)\)).
It is not difficult to see that, in order for the homogeneous random field \(\{x(s,t)\}\) to be regular, it is necessary and sufficient that the equality \(S_x=0\) hold.
We shall indicate the conditions imposed on the spectral function which guarantee the regularity or singularity of the field \(\{x(s,t)\}\).
Theorem 1. In order that the homogeneous random field \(\{x(s,t)\}\) be regular, it is necessary and sufficient that the following conditions be satisfied:
a) the measures \(dF_x(\lambda,\mu)\) and \(dF_x(\lambda,\pi)\,d\mu\) (i.e., the product of the measure \(dF_x(\lambda,\pi)\) by the measure \(d\mu\)) be absolutely continuous with respect to each other on the square \(-\pi \leq \lambda \leq \pi,\ -\pi \leq \mu \leq \pi\);
b) for almost all values of \(\lambda\) (with respect to the measure \(dF_x(\lambda,\pi)\)),
\[ \left| \int_{-\pi}^{\pi} \log\left( \frac{dF_x(\lambda,\mu)} {dF_x(\lambda,\pi)\,d\mu} \right)d\mu \right|<+\infty . \tag{10} \]
Theorem 2. In order that the homogeneous random field \(\{x(s,t)\}\) be regular, it is necessary and sufficient that its spectral function can be represented in the form
\[ F_x(\lambda,\mu)= \int_{-\pi}^{\lambda}\int_{-\pi}^{\mu} |L(\lambda,\mu)|^2\,dG(\lambda)\,d\mu, \tag{11} \]
where \(G(\lambda)\) is some function, nondecreasing on the interval \([-\pi,\pi]\) and such that \(G(\pi)-G(-\pi)>0\), and \(L(\lambda,\mu)\) is a complex-valued function, different from zero almost everywhere with respect to \(dG(\lambda)\,d\mu\), representable in the form
\[ L(\lambda,\mu)=\sum_{n=0}^{+\infty} l_n(\lambda)e^{-in\mu} \qquad \bigl(l_n(\lambda)\in L^2(dG(\lambda)),\ n=0,1,2,\ldots\bigr). \]
Theorems 1 and 2 give two forms of the necessary and sufficient condition for regularity. Let us note that the spectral function of a regular homogeneous random field need not be absolutely continuous, as the following simple example shows:
\[ x(s,t)\equiv x(t), \]
where \(x(t)\) is a regular stationary random sequence.
Theorem 3. In order that the spectral function of a regular homogeneous random field \(\{x(s,t)\}\) be absolutely continuous, it is necessary and sufficient that \(x(s,t)\) can be represented in the form
\[ x(s,t)=\sum_{n=0}^{+\infty}\sum_{m=-\infty}^{+\infty} a_{mn}u(s-m,t-n), \tag{12} \]
where \(\{u(s,t)\}\) is a family of pairwise uncorrelated random variables with constant variance.
Theorem 4. In order that the homogeneous random field \(\{x(s,t)\}\) be singular, it is necessary and sufficient that on the interval \(-\pi \leq \lambda \leq \pi\) the condition
\[ \int_{-\pi}^{\pi} \log\left( \frac{dF_x(\lambda,\mu)} {dF_x(\lambda,\pi)\,d\mu} \right)d\mu=-\infty \tag{13} \]
hold almost everywhere (with respect to the measure \(dF_x(\lambda,\pi)\)), where
\[ \frac{dF_x(\lambda,\mu)}{dF_x(\lambda,\pi)\,d\mu} \]
is the absolutely continuous part of the measure \(dF_x(\lambda,\mu)\) with respect to the measure \(dF_x(\lambda,\pi)\,d\mu\).
We shall assume that \(Mx(s,t)=0\). Let
\[ x(s,m)=\beta(s,m)+\gamma(s,m), \tag{14} \]
where \(\gamma(s,m)=\operatorname{proj}_{H_x(-1)} x(s,m)\), and \(\beta(s,m)\) is orthogonal to \(H_x(-1)\). Denote
\[ \sigma_m^2=\|\beta(s,m)\|^2 . \tag{15} \]
(It is clear that this quantity does not depend on \(s\).) Then \(\sigma_m\) will be the mean-square error of linear extrapolation of the field \(\{x(s,t)\}\) \(m+1\) steps ahead with respect to the variable \(t\). In applications such a problem naturally arises in cases where \(t\) plays the role of a time variable, and \(s\) of a spatial one.
Theorem 5.
\[ \sigma_m^2=2\pi\int_{\eta_\lambda}\sum_{k=0}^{m}|\varphi_k(\lambda)|^2\,dF_x(\lambda,\pi), \tag{16} \]
where
\[ \eta_\lambda=\left\{\lambda;\ \left|\int_{-\pi}^{\pi}\log\left(\frac{dF_x(\lambda,\mu)}{dF_x(\lambda,\pi)\,d\mu}\right)d\mu\right|<+\infty\right\}, \tag{17} \]
and the functions \(\varphi_k(\lambda)\), \((\lambda\in\eta_\lambda)\), are determined from the relations
\[ \exp\left[\frac12 A_0(\lambda)+\sum_{k=1}^{+\infty}A_k(\lambda)\zeta^k\right] =\varphi_0(\lambda)+\varphi_1(\lambda)\zeta+\varphi_2(\lambda)\zeta^2+\cdots; \tag{18} \]
\[ A_k(\lambda)=\frac{1}{2\pi}\int_{-\pi}^{\pi}e^{ik\mu}\log\left(\frac{dF_x(\lambda,\mu)}{dF_x(\lambda,\pi)\,d\mu}\right)d\mu . \tag{19} \]
In particular,
\[ \sigma_0^2=2\pi\int_{-\pi}^{\pi} \exp\left\{\frac{1}{2\pi}\int_{-\pi}^{\pi} \log\left(\frac{dF_x(\lambda,\mu)}{dF_x(\lambda,\pi)\,d\mu}\right)d\mu\right\} dF_x(\lambda,\pi). \tag{20} \]
Formulas (16), (20) are analogous to Kolmogorov’s formulas \((2,3)\) for the mean square of the error of extrapolation of stationary random sequences.
Definition. A homogeneous random field \(\{x(s,t)\}\) is called a field of Markov type if \(\operatorname{proj}_{H_x(t-1)} x(s,t)\) belongs to the closed linear manifold spanned by the quantities \(x(s,t-1)\), \(-\infty<s<+\infty\).
Theorem 6. I. In order that a homogeneous random field \(\{x(s,t)\}\) be a field of Markov type, it is sufficient that the condition
\[ F_x(\omega)=\iint_{\omega}\frac{1}{|1-l(\lambda)e^{-i\mu}|^2}\,dG(\lambda)\,d\mu \quad\text{for all }\omega\subseteq\Omega, \tag{21} \]
be satisfied, where:
a) \(G(\lambda)\) is some real nondecreasing bounded function on the interval \(-\pi\leq\lambda\leq\pi\), with \(G(\pi)-G(-\pi)>0\);
b) \(l(\lambda)\) is a complex function such that \(|l(\lambda)|\leq 1\) and
\[ \int_{-\pi}^{\pi}\frac{dG(\lambda)}{1-|l(\lambda)|^2}<+\infty; \tag{22} \]
c)
\[ \Omega=\{(\lambda,\mu);\ 1-l(\lambda)e^{-i\mu}\ne0\}. \tag{23} \]
II. If the field \(\{x(s,t)\}\) is a field of Markov type, then there exist functions \(l(\lambda)\) and \(q(\lambda)\) such that
\[ F_x(\omega)=\iint_{\omega}\frac{q(\lambda)}{|1-l(\lambda)e^{-i\mu}|^2}\,dF_x(\lambda,\pi)\,d\mu \tag{24} \]
for all \(\omega \subseteq \Omega\), where
\[ \text{a)}\quad \Omega=\{(\lambda,\mu);\;1-l(\lambda)e^{-i\mu}\ne 0\}; \]
\[ \text{b)}\quad |l(\lambda)|\leq 1 \qquad (-\pi\leq \lambda\leq \pi); \]
\[ \text{c)}\quad q(\lambda)\geq 0 \qquad (-\pi\leq \lambda\leq \pi). \]
III. The field \(\{x(s,t)\}\) is singular if and only if \(q(\lambda)\equiv 0\), and is regular if and only if \(F_x(\overline{\Omega})=0\), where \(\overline{\Omega}\) is the complement of \(\Omega\).
Theorem 7. If the homogeneous random field \(\{x(s,t)\}\) is a regular field of Markov type, then
\[ \operatorname{proj}_{H_{x(t-1)}} x(s,t) = \int_{-\pi}^{\pi}\int_{-\pi}^{\pi} e^{i[s\lambda+(t-1)\mu]} l(\lambda)\,dr_x(\lambda,\mu), \tag{25} \]
where
\[ l(\lambda)= \int_{-\pi}^{\pi} e^{i\mu}\, \frac{dF_x(\lambda,\mu)} {dF_x(\lambda,\pi)\,d\mu} \,d\mu . \]
The proofs of Theorems 1–3 and 5 are carried out analogously to the proofs of the corresponding theorems for the one-dimensional case (see \((^2,^3)\), and also \((^{4-6})\)).
The author is grateful to A. M. Yaglom for posing the problems considered in the present note.
Received
20 VIII 1956
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