Abstract Generated abstract
The paper characterizes standard Markov processes in Euclidean space whose exit distributions from domains are dominated by those of Brownian motion and which satisfy a local nondegeneracy condition. It proves a converse to the evident property of subprocesses of the Wiener process under random time change: any such standard process is equivalent to a process obtained by a random change of time from a subprocess of Brownian motion. The argument constructs approximating Markov chains based on successive exits from small balls, establishes weak convergence of their transition functions and exit measures, and identifies the limiting transition function with that of a Wiener subprocess. The result extends earlier work treating the case of infinite lifetime and equality of exit probabilities.
Full Text
Reports of the Academy of Sciences of the USSR
1962, Volume 147, No. 2
MATHEMATICS
M. G. Shur
ON A CLASS OF MARKOV PROCESSES WHOSE EXIT PROBABILITIES ARE MAJORIZED BY THE EXIT PROBABILITIES OF A WIENER PROCESS
(Presented by Academician P. S. Aleksandrov, 14 V 1962)
In the \(l\)-dimensional Euclidean space \(R^l\) let us consider the Wiener process \(\hat X=(\hat x_t,\hat{\mathcal M}_t,\hat P_x)\) and a strictly Markov process
\(X=(x_t,\xi,\mathcal M_t,P_x)\), obtained by a random change of time in some subprocess of the process \(\hat X\). Denote by \(\tau_U\) (respectively, \(\hat\tau_U\)) the moment of first exit of the process \(X\) (the process \(\hat X\)) from the domain \(U\)*, and put
\[ \pi_U(x,\Gamma)=P_x\{x(\tau_U)\in\Gamma\},\qquad \hat\pi_U(x,\Gamma)=\hat P_x\{\hat x(\hat\tau_U)\in\Gamma\} \]
for any Borel set \(\Gamma\) in \(R^l\). The system of measures \(\pi_U(x,\Gamma)\), evidently, satisfies the condition:
A. \(\pi_U(x,\Gamma)\leq \hat\pi_U(x,\Gamma)\) for all Borel \(\Gamma\).
If, moreover, \(P_x\{\xi>0\}=1\) for all \(x\in R^l\), then the following condition also holds:
B. \(\pi_{U_n}(x,R^l)\to 1\) as \(n\to\infty\) for any sequence of domains \(U_n\), each of which contains the point \(x\) and whose diameters tend to zero as \(n\to\infty\).
This assertion admits a converse. More precisely, the following theorem is true (by \(B^l\) is denoted the \(\sigma\)-algebra of Borel sets in \(R^l\)).
Theorem. Whatever standard process
\[
X=(x_t,\xi,\mathcal M_t,P_x),
\]
given in the measurable space \((R^l,B^l)\) and satisfying conditions A and B, there exists an equivalent process \(X\), obtained by means of a random change of time in some subprocess of the Wiener process**.
In the case when \(\xi\equiv\infty\) and in condition A the equality sign stands, this theorem was proved by Mackeene and Tanaka \((^6)\). The supposition of its validity in the general case was expressed by E. B. Dynkin \((^4)\).
- Denote by
\[ \bar X=(\bar x_t,\bar\xi,\bar{\mathcal M}_t,\bar P_x) \]
some subprocess of the Wiener process, and let \(\bar\tau_U\) be the moment of first exit of the process \(\bar X\) from the domain \(U\), while
\[ \bar\pi_U(x,\Gamma)=\bar P_x\{\bar x(\bar\tau_U)\in\Gamma\}. \]
Our immediate aim will be the construction of such a process \(\bar X\) for which the measures \(\bar\pi_U(x,\Gamma)\) coincide with \(\pi_U(x,\Gamma)\) for all domains \(U\) and all \(x\in R^l\). Everywhere, unless the contrary is stated, it is assumed that \(l\geq 2\).
* For the terminology, see \((^3,^4)\). The class of processes considered here was investigated in \((^4)\).
** Recall that \(\tau_U=\xi\), if \(x_t\in U\) for all \(t\) \((0\leq t<\xi)\), and
\[
\tau_U=\inf(t:t>0,\ x_t\notin U)
\]
otherwise.
*** Two Markov processes given on one and the same measurable space are called equivalent if their transition functions coincide. A homogeneous, right-continuous, strictly Markov process
\[
X=(x_t,\xi,\mathcal M_t,P_x),
\]
given in \((R^l,B^l)\), is called standard if \(\mathcal M_t\supset \mathcal N_{t+0}\) and if, for any \(x\in R^l\) and any nondecreasing sequence of random variables \(\tau_n\), not depending on the future, \(x(\tau_n)\) as \(n\to\infty\) tends to \(x(\tau)\), where
\[
\tau=\lim_{n\to\infty}\tau_n,
\]
\(P_x\)-almost surely on the set
\[
\Omega_1=\{\tau<\xi\}.
\]
Denote by \(\rho(x,y)\) the distance between points \(x\) and \(y\) in \(R^l\), and consider the sequence \(\tau_k^{(n)}\), defined as follows. We set \(\tau_0^{(n)} \equiv 0\). If \(\tau_k^{(n)}\) has already been defined, then \(\tau_{k+1}^{(n)}\) is set equal to the lower bound of the times \(t\) such that \(t>\tau_k^{(n)}\) and
\[
\rho\bigl(x(t),x(\tau_k^{(n)})\bigr)\geq \sqrt{l/2^{n+1}},
\]
provided that the set of such \(t\) is nonempty; otherwise \(\tau_{k+1}^{(n)}=\zeta\). The random variables \(x(\tau_k^{(n)})\), for any fixed \(n\), form a Markov chain.
Next, put \(x_n(t)=x(\tau_k^{(n)})\), if \(\tau_k^{(n)}<\zeta\) and \(k\cdot 2^{-n}\leq t<(k+1)2^{-n}\) (when \(\tau_k^{(n)}\geq \zeta\) and \(t\geq k\cdot 2^{-n}\), the quantity \(x_n(t)\) is not defined). The random functions \(x_n(t)\) are trajectories of a certain nonhomogeneous Markov process
\[
X_n=(x_n(t),\xi_n,\mathcal M_t^s(n),P_{s,x}^{(n)}),
\]
defined on the same set of elementary events as \(X\), and having transition function
\[
P_n(s,x,t,\Gamma)=P_x\{x(\tau_v^{(n)})\in\Gamma\},
\]
where \(v\) is the difference of the integer parts of the numbers \(2^n t\) and \(2^n s\). In an analogous way we construct the chains \(\hat x(\hat\tau_k^{(n)})\) and the process \(\hat X_n\) with transition function \(\hat P_n(s,x,t,\Gamma)\), starting from the Wiener process. From consideration of the sequences \(x(\tau_k^{(n)})\) it is not difficult to derive that, for any \(x\in R^l\), the trajectory \(x_t(\omega)\) is continuous in \(t\) \((0\leq t<\zeta)\) \(P_x\)-almost surely.
The transition function of the desired process \(\overline X\) will subsequently be constructed as the limit \(P_n(0,x,t,\Gamma)\).
It is important to note that
\[
\hat P_n(0,x,t,\Gamma)\geq P_n(0,x,t,\Gamma),
\]
and that the study of the distributions of the quantities \(\hat x(\hat\tau_k^{(n)})\) is in an obvious way reduced to the study of the distributions of normalized sums of independent random vectors \(\xi_i\), each of which is uniformly distributed on the circle of unit radius with center at the origin of the coordinates in \(R^l\). Using the theorem of paper \((^1)\) and the known estimates for the maximum of sums of independent quantities (see \((^2)\), Ch. 3, Theorem 2.2), we easily obtain\(^*\):
a) whatever \(T>0\) and \(\varepsilon>0\) may be, there exist numbers \(N\) and \(K\) such that for \(n>N\) the inequality
\[
\hat P_n(s,x,t,\Gamma)\leq K\lambda(\Gamma)+\varepsilon
\]
holds for all \(x\in R^l\) and all numbers \(s\geq 0,\ t\geq 0\) for which \(t-s>T\);
b) for fixed \(t\in\Lambda\) and \(n\to\infty\), the function \(\hat P_n(0,x,t,\Gamma)\) tends to the transition function \(\hat P(t,x,\Gamma)\) of the Wiener process, uniformly in \(x\in R^l\) and \(\Gamma\in B^l\);
c) \(\delta>0\) can be chosen so that, for all sufficiently large \(n\), the quantity \(\alpha_n^\varepsilon(\delta)/\delta\) does not exceed any preassigned number.
We shall say that the Borel measures \(\mu_n\) converge weakly as \(n\to\infty\) to the Borel measure \(\mu\), if
\[
\int f\,d\mu_n\to \int f\,d\mu
\]
for every continuous function \(f(x)\) tending to zero at infinity. Denote by \(\tau_n'\) the first exit time of \(X_n\) from \(U\) \((U\in C)\), and put
\[
\mu_n(x,\Gamma)=P_{0,x}^{(n)}\{x_n(\tau_n')\in\Gamma\}.
\]
Lemma 1. Whatever \(x\in U\) \((U\in C)\) may be, the measures \(\mu_n(x,\Gamma)\) converge weakly to \(\pi_U(x,\Gamma)\) as \(n\to\infty\).
From assertions a) and c), Lemma 1, and estimate (6.28) of book \((^3)\), one may conclude that
d) for any fixed \(x\in R^l\), \(t\geq 0\), and \(\varepsilon>0\), one can indicate so small an \(s>0\) that, for all sufficiently large \(n\), the following will be fulfilled—
\(^*\) In what follows, \(\lambda\) is the ordinary Lebesgue measure in \(R^l\); \(V_\varepsilon(x)\) is the exterior of the \(\varepsilon\)-neighborhood of the point \(x\); \(\alpha_n^\varepsilon(\delta)\) is the upper bound of the values of \(\hat P_n(s,x,t,V_\varepsilon(x))\) for \(x\in R^l\) and \(t-s\leq\delta\); \(C\) is the collection of domains whose boundaries are \((l-1)\)-dimensional smooth manifolds of class 2; \(\Lambda\) is the collection of nonnegative dyadic-rational numbers.
the inequalities hold
\[ P_n(0,x,s,V_\varepsilon(x))<\varepsilon,\qquad P^{(n)}_{0,x}\{\xi_n>s\}>1-\varepsilon,\qquad P^{(n)}_{0,x}\{t+\dot{s}>\xi_n>t\}<\varepsilon. \tag{1} \]
- Let us proceed to the construction of the transition function of the desired process \(\overline{X}\). Consider the family of functions
\[ \Phi_n(s,x,t,\Gamma)=\int \widehat{P}(s,x,dy)\,P_n(s,y,t,\Gamma) \qquad (n\geq 0,\ t\geq s,\ \Gamma\in B^l). \]
For any fixed \(s>0\) this family of functions is equicontinuous in \(x\). Moreover, if \(\varepsilon>0\), \(s_0>0\), and \(x\in R^l\) are fixed, then one can choose \(s>0\) such that, for all \(\Gamma\in B^l\), \(t>s_0\), and all sufficiently large \(n\),
\[ \left|P_n(0,x,t,\Gamma)-\Phi_n(s,x,t,\Gamma)\right|<2\varepsilon. \tag{2} \]
Indeed, assuming \(s\) to satisfy the second of inequalities (1) and recalling the Chapman–Kolmogorov equality for \(X_n\), we obtain, for large values of \(n\), that
\[ \left|P_n(0,x,t,\Gamma)-\int \widehat{P}_n(0,x,s,dy)\,P_n(s,y,t,\Gamma)\right|<\varepsilon, \]
whence, according to b), our assertion follows.
Lemma 2. There exists a numerical sequence \(\{n_k\}\) such that, for any \(x\in R^l\) and \(t\in\Lambda\), the measures \(P_{n_k}(0,x,t,\Gamma)\) converge weakly as \(k\to\infty\) to some measure \(\overline{P}(t,x,\Gamma)\).
Lemma 2 is easily derived from the assertion: for any \(s_0>0\) there exists a sequence \(\{n_k\}\) such that, for all \(x\in R^l\) and all \(t>s_0\) \((t\in\Lambda)\), the measures \(P_{n_k}(0,x,t,\Gamma)\) converge weakly to some measure \(Q(s_0,t,x,\Gamma)\). To prove this assertion, fix \(s_0>0\), \(t>s_0\) \((t\in\Lambda)\), and \(n\geq 0\).
For each \(x\in R^l\) choose \(s=s(n,x)\) \((0<s(n,x)\leq 2^{-n})\) so as to satisfy (2) with \(\varepsilon=2^{-n-1}\). Then about each \(x\) describe an open ball \(V(x,n)\) such that, for all points \(y\) in it,
\[ \left|\Phi_m(s(n,x),x,t,\Gamma)-\Phi_m(s(n,x),y,t,\Gamma)\right|<2^{-n} \]
for any \(m\geq 0\), \(\Gamma\in B^l\). Keeping \(n\) fixed for the time being, from the system of balls \(V(x,n)\) extract a countable covering of the whole of \(R^l\). Denote the centers of the balls entering this covering by \(x_{n,r}\), and choose \(\{n_k\}\) so that our assertion is true for all \(x_{n,r}\) for any \(n\) and \(r\). The sequence \(\{n_k\}\) is the desired one. Indeed, if \(x_0\in R^l\), \(2^{-n_0}\leq s(n,x_0)\), and \(x_0\in V(x_{n_0,r_0},n_0)\), then
\[ \left|P_m(0,x_0,t,\Gamma)-P_m(0,x_{n_0,r_0},t,\Gamma)\right|<4\cdot 2^{-n} \]
for all sufficiently large \(m\).
Lemma 2 and assertion a) allow us, from the Chapman–Kolmogorov equality for the process \(X_n\), to conclude that, for all \(x\in R^l\) and \(\Gamma\in C\) (and consequently also for all \(\Gamma\in B^l\)),
\[ \overline{P}(s+t,x,\Gamma)=\int \overline{P}(s,x,dy)\,\overline{P}(t,y,\Gamma), \tag{3} \]
where \(s,t\in\Lambda\). For \(t\notin\Lambda\) \((t>0)\), define the measure \(\overline{P}(t,x,\Gamma)\) as the weak limit of the measures \(\overline{P}(u,x,\Gamma)\) as \(u\downarrow t\) (the correctness of this definition follows from c)). Taking a) into account, one can verify that the measures \(\overline{P}(t,x,\Gamma)\) satisfy (3) for all \(s,t\geq 0\), and, thus, \(\overline{P}(t,x,\Gamma)\) is a transition function. In view of the fact that \(\overline{P}(t,x,\Gamma)\) is majorized by the transition function of the Wiener process, the transition function \(\overline{P}(t,x,\Gamma)\) corresponds to some subprocess of the Wiener process (7). We shall take this subprocess as \(\overline{X}\).
3. It is not difficult to verify that the finite-dimensional distributions of the processes \(X_{n_k}\) converge weakly, as \(k \to \infty\), to the finite-dimensional distributions of the process \(\overline{X}\).
By means of Theorem 3.1.2 from \((^5)\) we establish that the measures \(\mu_n(x,\Gamma)\), for every \(U \in C\), converge weakly to \(\overline{\pi}_U(x,\Gamma)\), and, consequently, in accordance with Lemma 1, \(\pi_U(x,\Gamma)=\overline{\pi}_U(x,\Gamma)\) if \(U \in C\). This equality is extended to all domains \(U\) with the aid of Lemma 3.
Lemma 3. Let \(Y=(y_t,\xi',\mathcal{M}'_t,Q_x)\) be a standard process satisfying conditions A and B. Let \(\xi_n\) be a nondecreasing sequence of random variables independent of the future, and let \(\xi=\lim_{n\to\infty}\xi_n\).
Let the event \(H\) consist in the fact that \(\sup_{0\le t<\xi}|y_t|<\infty\), where \(|y_t|\) denotes the distance of \(y_t\) from the origin in \(R^l\). Then the measures
\[ \mu_x^{(n)}(\Gamma)=Q_x\{H,\; y(\xi_n)\in\Gamma\} \]
converge weakly to the measures
\[ \mu_x(\Gamma)=Q_x\{H,\; y(\xi)\in\Gamma\} \]
as \(n\to\infty\).
Now, from a theorem of Blumenthal, Getoor, and McKean one may conclude that the process \(X\) is equivalent to some process obtained from \(\overline{X}\) by a random change of time. In the case \(l=1\), however, our theorem follows from the works \((^8,^9)\).
Received
11 V 1962
CITED LITERATURE
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\(^6\) H. P. McKean Jr., H. Tanaka, Mem. Coll. Sci. Univ. Kyoto, ser. A, 33, No. 3 (1961).
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