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Corrigendum to: Asymptotic shape and the speed of propagation of continuous-time continuous-space birth processes

Published online by Cambridge University Press:  03 December 2020

V. Bezborodov*
Affiliation:
Wrocław University of Science and Technology
*
*Postal address: Wrocław University of Science and Technology, Faculty of Electronics, Janiszewskiego 11, Wrocław, Poland.
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Abstract

We would like to correct the statement of Lemma 4.1 in [BDK+18].

Type
Corrigendum
Copyright
© Applied Probability Trust 2020

1. Introduction

Let $(S, \mathscr{B}(S))$ be a Polish (state) space. Consider a (time-homogeneous) Markov chain on $(S, \mathscr{B}(S))$ as a family of probability measures on $S^ \infty$. Namely, on the measurable space ${(\bar \Omega,\mathscr{F}) = (S^ \infty , \mathscr{B}(S ^\infty ))}$ consider a family of probability measures $\{P_s \}_{s \in S}$ such that for the coordinate mappings

\begin{align*}X_n\,:\, \bar \Omega \rightarrow S, \ \ \ \ X_n (s_1,s_2,...) = s_n,\end{align*}

the process $X \coloneqq \{X_n \}_{n \in \mathbb{Z} _+ }$ is a Markov chain such that for all $s \in S$

\begin{equation*}\mathbb{P}_s \{X_0 =s \} =1, \ \ \ \mathbb{P}_s \{ X_{n+m_j}\in A_j, j=1,...,l \mid \mathscr{F} _n \}= \mathbb{P}_{X_n} \{ X_{m_j} \in A_j, j=1,...,l \}.\end{equation*}

Here $A_j \in \mathscr{B} (S)$, $m_j \in \mathbb{N}$, $ l \in \mathbb{N}$, $\mathscr{F} _n = \sigma \{ X_1,...,X_n \}$. The space S is separable, hence there exists a transition probability kernel $Q\,:\,S \times \mathscr{B} (S) \rightarrow [0,1]$ such that

\begin{equation*}Q(s,A) = \mathbb{P}_s \{ X_1 \in A \}, \ \ \ s\in S, \ A \in \mathscr{B} (S).\end{equation*}

Consider a transformation of the chain X, $Y_n = f(X_n)$, where $f\,:\,S\to \mathbb{R} $ is a Borel-measurable function. Lemma 4.1 in [Reference B., P., K., L. and O.BDK+18] gives sufficient conditions for $Y = \{Y_n \}_{n \in \mathbb{Z} _+ }$ to be a Markov chain. The original erroneous Lemma 4.1 had the following formulation.

Lemma 4.1 old. Assume that for any bounded Borel function $h\,:\,S\rightarrow S$

\begin{equation*} \mathbb{E}_s h (X_1) = \mathbb{E}_q h (X_1) \text{\ whenever \ } f(s)= f(q). \end{equation*}

Then Y is a Markov chain.

Lemma 4.1 and the remark succeeding it in [Reference B., P., K., L. and O.BDK+18] should instead read as follows.

Lemma 4.1. Assume that for any bounded Borel function $h\,:\,S\rightarrow S$

(1) \begin{equation} \mathbb{E}_s h (Y_1) = \mathbb{E}_q h (Y_1) \text{\ whenever \ } f(s)= f(q). \end{equation}

Then Y is a Markov chain.

Remark 4.1. Condition (1) is the equality of distributions of $Y_1$ under two different measures, $\mathbb{P}_s$ and $ \mathbb{P}_q$.

Note that the statement of Lemma 4.1 old is actually correct in the sense that it is true, but it is very weak. In particular, in the proof of Theorem 2.6 in [Reference B., P., K., L. and O.BDK+18] Lemma 4.1 is required because Lemma 4.1 old is not sufficient.

Proof of Lemma 4.1. For the natural filtrations of the processes X and Y we have an inclusion

(2) \begin{equation} \mathscr{F} ^X _n \supset \mathscr{F} ^Y _n, \ \ \ n \in \mathbb{N}, \end{equation}

since Y is a function of X. For $n\in \mathbb{N}$ and bounded Borel functions $h_j\,:\,\mathbb{R} \rightarrow \mathbb{R}$, $j=1,2,...,n$,

\begin{align*}\mathbb{E}_s \left[ \prod\limits _{j=1} ^n h_j(Y_{k+j}) \mid \mathscr{F} ^ X _k \right] & = \mathbb{E}_{X_k} \prod\limits _{j=1} ^n h_j(f(X_{j})) \\ & = \int _S Q(x_0 , dx_1) h_1(f(x_1)) \int _S Q(x_1 , dx_2) h_2(f(x_2))...\\ & \quad \times\int _S Q(x_{n-1} , dx_n) h_n(f(x_n)) \Bigg| _{x_0 = X _k}\end{align*}

To transform the last integral, we introduce a new kernel: for $y \in f(S)$ chose $x \in S$ with $f(x) = y$, and then for $B \in \mathscr{B}(\mathbb{R})$ define

\begin{equation*} \overline Q (y, B) = Q (x, f^{-1}(B)). \end{equation*}

The expression on the right-hand side does not depend on the choice of x because of (1). To make the kernel $\overline Q$ defined on $\mathbb{R} \times \mathscr {B} (\mathbb{R}) $, we set

\begin{equation*} \overline Q (y, B) = \mathds{1}_{\{0 \in B \}}, \ y \notin f(S). \end{equation*}

Then, setting $z_{n} = f(x_{n})$, we obtain from the change of variables formula for the Lebesgue integral that

\begin{equation*} \int _S Q(x_{n-1} , dx_n) h_n(f(x_n)) = \ \int _{\mathbb{R}} \overline Q (f(x_{n-1}) , dz_n) h_n(z_n). \end{equation*}

Likewise, setting $z_{n-1} = f(x_{n-1})$, we get

\begin{align*} & \int _S Q(x_{n-2} , dx_{n-1}) h_n(f(x_{n-1})) \int _S Q(x_{n-1} , dx_n) h_n(f(x_n)) \\[2pt] &\quad = \int _S Q(x_{n-2} , dx_{n-1}) h_n(f(x_{n-1})) \int _{\mathbb{R}} \overline Q (f(x_{n-1}) , dz_n) h_n(z_n) \\[2pt] &\quad = \int _{\mathbb{R}} \overline Q(f(x_{n-2}) , dz_{n-1}) h_n(z_{n-1}) \int _{\mathbb{R}} \overline Q (z_{n-1} , dz_n) h_n(z_n). \end{align*}

Proceeding further, we obtain

\begin{align*} &\int _S Q(x_0 , dx_1) h_1(f(x_1)) \int _S Q(x_1 , dx_2) h_2(f(x_2))... \int _S Q(x_{n-1} , dx_n) h_n(f(x_n)) \\[2pt] &\quad = \int _{\mathbb{R}} \overline Q(z_0 , dz_1) h_1(z_1) \int _{\mathbb{R}} \overline Q(z_1 , dz_2) h_2(z_2)... \int _{\mathbb{R}} \overline Q(z_{n-1} , dz_n) h_n(z_n), \end{align*}

where $z_0 = f (x _0 )$.

Thus,

\begin{equation*} \mathbb{E}_s \!\left[ \prod\limits _{j=1} ^n h_j(Y_{k+j}) \mid \mathscr{F} ^ X _k \right] = \int _{\mathbb{R}} \overline Q(f(X_k) , dz_1) h_1(z_1) \int _{\mathbb{R}} \overline Q(z_1 , dz_2) h_2(z_2)... \int _{\mathbb{R}} \overline Q(z_{n-1} , dz_n) h_n(z_n). \end{equation*}

This equality and (2) imply that Y is a Markov chain.□

References

B., Viktor, P., Luca Di, K., Tyll, L., Mykola, and O., Tomasz Asymptotic shape and the speed of propagation of continuous-time continuous-space birth processes. Adv. Appl. Probab., 50(1):74101, 2018.Google Scholar