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It is known that a random series $$ \sum_{n\geq 1} X_n $$ whose terms $X_n$ are independent converges a.s. if and only if it converges in probability.

Is it true that a martingale $(Y_n)$ converges a.s. if and only if it converges in probability? If not, are there any counter-examples? Thanks.

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$\newcommand{\N}{\mathbb N}\newcommand{\si}{\sigma}\newcommand{\F}{\mathcal{F}}\newcommand{\Om}{\Omega}\newcommand{\Z}{\mathbb{Z}}$A counterexample can be obtained as follows. Let $T_1,T_2,\dots$ be independent (say) geometrically distributed random variables with fast growing means, say with $ET_i=2^i$.

Let $Y_n=0$ for $0\le n\le T_1$. For time moments $n$ after that, let the values of $Y_n$ coincide with the positions of a simple random walk $W^{(1)}_\cdot$ starting from $0$ at time $T_1$ -- but only till the time, say $\nu_1$, of the first return of $W^{(1)}_\cdot$ to $0$. This is the first "step".

After this, let $Y_\cdot$ stay at $0$ for time $T_2$. After that, let the values of $Y_n$ coincide with the positions of a simple random walk $W^{(2)}_\cdot$ starting in state $0$ at time $\nu_1+T_2$ -- but only till the time, say $\nu_2$, of the first return of $W^{(2)}_\cdot$ to $0$, where $W^{(2)}_\cdot$ is independent of $W^{(1)}_\cdot$. This is the second "step".

Continue doing such "steps" indefinitely (assuming that the walks are independent of the $T_j$'s). Thus, we get a martingale $(Y_n)$, with respect to a certain filtration of $\sigma$-algebras. The walks occur increasingly rarely; they start at very uncertain times (with standard deviations $\asymp2^i$ and corresponding very flat distributions); and the walks last comparatively short times. Therefore, for any given large time moment $n$, $P(Y_n\ne0)$ is small. So, $Y_n\to0$ in probability.

However, because the walks occur infinitely many times, clearly $Y_n\not\to0$ almost surely.


Here are formal details.

Construction: Let $T_1,T_2,\dots$ be independent geometrically distributed random variables (r.v.'s) (defined on some probability space $(\Om,\F,P)$) with means $ET_i=1/p_i$, where $0<p_i<1/2$ and \begin{equation*} \sum_{i\in\N}p_i^{1/2}<\infty. \tag{1} \end{equation*} So, \begin{equation*} P(T_i=t)=p_i q_i^{t-1}\,1(t\in\N) \tag{2} \end{equation*} for real $t$, where $q_i:=1-p_i$.

Let $R_1,R_2,\dots$ be independent Rademacher r.v.'s (defined on the same probability space $(\Om,\F,P)$) that are independent of the $T_i$'s; so, $P(R_i=1|(T_j))=1/2=P(R_i=-1|(T_j))$ for all $i\in\N$.

Define (the starting times of the walks) $S_1,S_2,\dots$ and (the finishing times of the walks) $F_0,F_1,F_2,\dots$ by the following recursion: \begin{equation*} F_0:=0 \end{equation*} and, for $k\in\N$, \begin{equation*} S_k:=F_{k-1}+T_k,\quad F_k:=\inf\{n\in\N\colon n>S_k,W^{(k)}_n=0\}, \tag{3} \end{equation*} where \begin{equation*} W^{(k)}_n:=\sum_{i\in\N}R_i\,1(S_k<i\le n). \tag{3a} \end{equation*} Note that $F_0=0<\infty$ and $F_k=\min\{n\in\N\colon n>S_k,W^{(k)}_n=0\}<\infty$ for all $k\in\N$ almost surely (a.s.), because the simple random walk is recurrent. So, $S_k<\infty$ for all $k\in\N$ a.s.

Now, for all $n\in\N$ let \begin{equation*} Y_n:=\sum_{k\in\N}1(S_k<n\le F_k)W^{(k)}_n. \tag{4} \end{equation*} Note that a.s. at most one summand in (4) is nonzero, since $S_k=F_{k-1}+T_k>F_{k-1}$ a.s. for all $k\in\N$.

To complete the construction, for each $n\in\N$ let \begin{equation*} \F_n:=\si(R_1,\dots,R_n,\{1(T_k\le j)\colon k\in\N,j\in\N,j\le n\}), \end{equation*} the $\si$-algebra generated by $R_1,\dots,R_n,\{1(T_k\le j)\colon k\in\N,j\in\N,j\le n\}$. Clearly, $(\F_n)_{n\in\N}$ is a filtration.

Showing that $((Y_n,\F_n))_{n\in\N}$ is a martingale: Abusing notation as is commonly done, for a r.v. $X$ let us write $X\in\F_n$ to mean that $X$ is $\F_n$-measurable. Then obviously $1(F_0\le n)=1(0\le n)\in\F_0:=\{\Om,\emptyset\}\subseteq\F_1$ for all $n\in\N$. Using now the relations \begin{equation*} 1(S_k\le n)=\sum_{j=1}^{n-1}1(T_k=j)1(F_{k-1}\le n-j), \end{equation*} $1(T_k=j)=1(T_k\le j)-1(T_k\le j-1)$, and \begin{equation*} \{F_k\not\le n\}= \bigcap_{m=1}^n\Big(\{S_k\not\le m-1\}\cup\Big\{\sum_{i=1}^m R_i\,1(S_k\le i-1)\ne0\Big\}\Big) \end{equation*} for natural $k,j$ (which follow by (3) and (3a)), we conclude by induction on $k$ that \begin{equation*} \{S_k\le n\}\in\F_n,\quad \{F_k\le n\}\in\F_n \tag{5} \end{equation*} for all natural $k,n$.

Hence, by (4) and (3a), the sequence $(Y_n)_{n\in\N}$ is adapted to the filtration $(\F_n)_{n\in\N}$. Moreover, by (4), for all $n\in\N$ we have \begin{equation*} Y_{n+1}-Y_n=\sum_{k\in\N}R_{n+1}\,1(S_k\le n,F_k\not\le n); \end{equation*} also, $R_{n+1}$ is independent of $\F_n$. So, in view of (5), $((Y_n,\F_n))_{n\in\N}$ is a martingale.

Showing that $Y_n\to0$ in probability (as $n\to\infty$): By (4), \begin{equation*} 1(Y_n\ne0\}=\sum_{k\in\N}1(S_k<n\le F_k) \tag{6} \end{equation*} and hence \begin{equation*} P(Y_n\ne0\}=\sum_{k\in\N}P(S_k<n\le F_k). \tag{7} \end{equation*} Here and in what follows, $n$ and $k$ are natural numbers. Next, consider the duration \begin{equation*} D_k:=F_k-S_k \end{equation*} of the $k$th walk. Since the $R_i$'s are independent and independent of the $T_j$'s, the r.v.'s $D_1,D_2,\dots$ are independent and independent of the $T_j$'s, and the $T_j$'s are also independent. So, the r.v.'s $T_1,D_1,T_2,D_2,\dots$ are independent. Also, \begin{equation*} S_k=T_1+\sum_{j=2}^k(D_{j-1}+T_j). \tag{8} \end{equation*} So, $S_k$ and $D_k$ are independent and hence
\begin{equation*} P(S_k<n\le F_k)=\sum_{d\in\N}P(D_k=d)P(S_k<n\le S_k+d). \end{equation*} Using (8) and the independence of $T_1,D_1,T_2,D_2,\dots$, for all $d\in\N$ we have \begin{equation*} P(S_k<n\le S_k+d)= P(n-d\le S_k<n)\le\sup_{m\in\Z} P(m-d\le T_k<m) =\sum_{t=1}^d p_kq_k^{t-1}. \end{equation*} So, \begin{equation*} \begin{aligned} P(S_k<n\le F_k)&\le\sum_{d\in\N}P(D_k=d)\sum_{t=1}^d p_kq_k^{t-1} \\ &=\sum_{t\in\N}^d p_kq_k^{t-1}\sum_{d=t}^\infty P(D_k=d) \\ &=\sum_{t\in\N}^d p_kq_k^{t-1}P(D_k\ge t) \\ &=\sum_{t\in\N}^d p_kq_k^{t-1}P(D_1\ge t) \\ &\le\sum_{t\in\N} p_kq_k^{t-1}ct^{-1/2}, \end{aligned} \end{equation*} since, by (say) the reflection principle, $P(D_1\ge t)\le ct^{-1/2}$ for $t\in\N$. Here and in what follows, $c$ denotes various universal positive real constants. Therefore and because $0<p_k<1/2$, \begin{equation*} \begin{aligned} P(S_k<n\le F_k)&\le 2c\sum_{t\in\N} p_k(1-p_k)^t t^{-1/2} \\ &\le 2cp_k \sum_{t\in\N} e^{-p_k t}t^{-1/2} \\ &\le 2cp_k \int_0^\infty e^{-p_k t}t^{-1/2}\,dt =cp_k^{1/2}. \end{aligned} \tag{9} \end{equation*}

Also, for each $k\in\N$, $P(S_k<n\le F_k)\le P(F_k\ge n)\to0$ (as $n\to\infty$), since $F_k<\infty$ a.s. So, by (7), for each $K\in\N$, \begin{equation*} \limsup_n P(Y_n\ne0\}\le \limsup_n \sum_{k=K}^\infty cp_k^{1/2}. \end{equation*} Letting now $K\to\infty$ and recalling (1), we see that $\limsup_n P(Y_n\ne0\}=0$ and hence $Y_n\to0$ in probability (as $n\to\infty$).

Noting that $Y_n\not\to0$ a.s. (as $n\to\infty$): It follows (say by (6)) that $|Y_{S_k+1}|=1$ for all $k\in\N$. Also, $S_k\to\infty$ a.s. as $k\to\infty$. So, $Y_n\not\to0$ a.s. (as $n\to\infty$).

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    $\begingroup$ Splendid example! $\endgroup$ Commented Dec 9, 2021 at 10:40
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    $\begingroup$ An example of this phenomenon should be in the next generation of books that treat martingale theory. $\endgroup$ Commented Dec 9, 2021 at 16:09
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    $\begingroup$ @BillJohnson in the current generation of books, a counterexample (arguably simpler) appears as Example 5.2.4 in Rick Durett's "Probability: Theory and examples" $\endgroup$ Commented Dec 9, 2021 at 17:58
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    $\begingroup$ @GuillaumeAubrun : Thank you for your comment. (This is Example 4.2.14 in the version of the book at services.math.duke.edu/~rtd/PTE/PTE5_011119.pdf .) That example is indeed much simpler. I thought of something like this for a moment, but it did not occur to me how to nullify $X_n$ in just one step. Well, this turns out very easy to do. The lesson for me: read textbooks. :-) $\endgroup$ Commented Dec 9, 2021 at 18:24
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    $\begingroup$ For me, Iosif, it is be more sympathetic to students who do not read the text book as I have taught from Durrett's book. $\endgroup$ Commented Dec 10, 2021 at 21:47

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