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UDC 519.210
MATHEMATICS
Academician of the Academy of Sciences of the Uzbek SSR T. A. SARYMSAKOV, Ya. Kh. KUCHKAROV
ON THE ERGODIC PRINCIPLE FOR A PARTIALLY SEMIGROUP FAMILY OF OPERATORS ON TOPOLOGICAL SEMIFIELDS
In this article we shall adhere to the definitions and notation of works \((^1,^2)\).
- Let a family \(\{E_k,\ 1 \leq k \leq \infty\}\) be given, where \(E_k\) is a complete topological semifield; \(K_k\) is the cone of nonnegative elements in \(E_k\), and \(\nabla_k\) is the topological Boolean algebra of all idempotents, on which a certain measure is defined. Elements of \(E_k\) for which the integral with respect to this measure exists are called summable; denote their set by \(L_k\). Obviously, \(L_k\) is a linear topological space in the topology induced from \(E_k\). An element \(x \in L_k \cap K_k\) will be called a distribution if \(\mu(x)=1\), where \(\mu\) denotes the integral sign.
Introduce the notation
\[ P_k=\{x:x\in L_k\cap K_k,\quad \mu(x)=1\}. \]
Consider, generally speaking, a noncommutative family \(\{T_k^{[k+1]},\ 1\leq k\leq \infty\}\) of linear operators, where \(T_k^{[k+1]}:L_k\to L_{k+1}\) and
\[ T_k^{[m]}=T_{m-1}^{[m]}\times T_{m-2}^{[m-1]}\cdots T_k^{[k+1]}\quad (k<m). \]
Definition 1. A linear operator \(T_k^{[k+1]}\) \((1\leq k\leq \infty)\) will be called stochastic if it satisfies the following conditions:
1) \(T_k^{[k+1]}(L_k)\subset L_{k+1}\);
2) \(\mu(T_k^{[k+1]}x)=\mu(x)\) for \(x\in L_k\);
3) \(T_k^{[k+1]}x^{(n)}\to T_k^{[k+1]}x^{(0)}\), if \(x^{(n)}\to x^{(0)}\) \((x^{(0)},x^{(n)}\in L_k)\).
Here convergence is to be understood in the sense of the topology in \(E_k\).
Definition 2. A family \(\{T_k^{[k+1]},\ 1\leq k\leq \infty\}\) of stochastic operators will be called ergodic if, for any \(k\) and any \(x,y\) from \(P_k\) and \(g\in\nabla_2\), the relation
\[ \lim_{r\to\infty}\mu(gT_k^{[r]}(x-y))=0 \]
holds.
We shall say that a family \(\{\widetilde T_k^{[k+1]},\ 1\leq k\leq \infty\}\) of operators includes the family \(\{T_k^{[k+1]},\ 1\leq k\leq \infty\}\) if, for some \(i_1,i_2,\ldots,i_h,\ldots\) \((i_h=i_j\ \text{when }h=j)\),
\[ \widetilde T_{i_h}^{[i_{h+1}]}=T_h^{[h+1]}. \]
Definition 3. A family \(\{\widetilde T_k^{[k+1]},\ 1\leq k\leq \infty\}\) of stochastic operators will be called strongly ergodic if any family \(\{\widetilde T_k^{[k+1]},\ 1\leq k\leq \infty\}\) of stochastic operators that includes the family \(\{T_k^{[k+1]},\ 1\leq k\leq \infty\}\) is ergodic.
Condition A. Whatever \(x,y\) from \(P_k\) may be, there exist a natural number \(m\), elements \(z\in L_m\), \(u\) and \(v\) from \(P_m\), depending on \(x,y\), and a number \(\lambda(T_k^{[m]})\) \((0<\lambda(T_k^{[m]})<1)\) such that
\[ T_k^{[m]}x-z=(1-\lambda(T_k^{[m]}))u, \]
\[ T_k^{[m]}y-z=(1-\lambda(T_k^{[m]}))v, \]
where \(z<T_k^{[m]}x,\ z<T_k^{[m]}y,\ k=1,2,\ldots\)
1.1. If, for the family \(\{T_k^{[k+1]},\ 1\leq k\leq\infty\}\) of stochastic operators, condition (A) is satisfied, then the equality holds
\[ T_1^{[n]}(x-y)=(1-\lambda(T_1^{[m_1]}))(1-\lambda(T_{m_1}^{[m_2]}))\cdots(1-\lambda(T_{m_{h-1}}^{[m_h]}))T_{m_h}^{[m_h+r]}(u-v), \]
\[ x,y\in P_1,\qquad u,v\in P_{m_h}\qquad \text{for } n=m_1+m_2+\cdots+m_h+r,\quad r<m_{h+1}-m_h. \]
1.2. If, for the family \(\{T_k^{[k+1]},\ 1\leq k\leq\infty\}\) of stochastic operators, condition (A) is satisfied and the series
\[ \lambda(T_1^{[m_1]})+\sum_{h=2}^{\infty}\lambda(T_{m_{h-1}}^{[m_h]})=\infty, \tag{1} \]
then for any \(x,y\) from \(P_1\) the relation holds
\[ \lim_{n\to\infty}\mu\bigl(gT_1^{[n]}(x-y)\bigr)=0. \]
1.3. In order that the family \(\{T_k^{[k+1]},\ 1\leq k\leq\infty\}\) of stochastic operators satisfying condition (A) be strongly ergodic, it is necessary and sufficient that relation (1) hold.
All known criteria of ergodicity for inhomogeneous Markov chains (see \((^3),(^4)\), p. 206, \((^5,^6)\)) are sufficient conditions for strong ergodicity and constitute special cases of condition (1). From proposition 1.3, as a consequence, follow the results of papers \((^7)\) (Theorem 11), \((^8)\) (Lemma 2), \((^9)\) (Theorem 1).
2. Consider a topological semifield \(E_k(t)\), depending on a numerical parameter \(t\), and denote by \(\mathscr E_k(t)\) the direct sum
\[ \mathscr E_k(t)=E_k(t)\oplus iE_k(t). \]
As in item 1, it is assumed that on \(\nabla_k(t)\) a certain proper measure is defined.
Let there be given, generally speaking, a noncommutative family of linear operators \(\{T_k^{[k+1]}(t),\ 1\leq k\leq\infty\}\), where \(T_k^{[k+1]}(t):\mathscr L_k(t)\to\mathscr L_{k+1}(t)\) and
\[ T_k^{[m]}(t)=T_{m-1}^{[m]}(t)\times T_{m-2}^{[m-1]}(t)\cdots T_k^{[k+1]}(t) \]
for \(k<m\). Here \(\mathscr L_k(t)\) is the set of summable elements of the complex semifield \(\mathscr E_k(t)\).
Definition 4. A family \(\{T_k^{[k+1]}(t),\ 1\leq k\leq\infty\}\) of linear operators continuously depending on the numerical parameter \(t\) will be called a family of characteristic operators if the following relations are fulfilled:
1) \(T_k^{[k+1]}(t)(\mathscr L_k(t))\subseteq \mathscr L_{k+1}(t)\);
2) \(T_k^{[k+1]}(0)=T_k^{[k+1]}\) is a stochastic operator;
3) \(T_k^{[k+1]}(t)x^{(n)}(t)\to T_k^{[k+1]}(t)x^{(0)}(t)\), if
\[ x^{(n)}(t)\to x^{(0)}(t)\quad (x^{(0)}(t),x^{(n)}(t)\in\mathscr L_k(t)). \]
If, for the family \(\{T_k^{[k+1]}(t),\ 1\leq k\leq\infty\}\) of characteristic operators, a condition analogous to (A), taking into account the parameter \(t\), is satisfied, then results 1.1 and 1.2 remain valid for this family.
From the results of item 2, as a consequence, follows the result of paper \((^{10})\) (Lemma 5).
Tashkent State University
named after V. I. Lenin
Received
19 V 1970
CITED LITERATURE
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