Existence of separators for biased random walk.












2












$begingroup$


Let us consider a biased random walk in $mathbf{Z}$ whose step-lengths satisfy $mathbf{P}(xi = +1) = p > mathbf{P}(xi = -1) = q$ (with $p+q = 1$).



A value $k in mathbf{Z}$ is a "separator" of the random walk if the random walk started before $k$ passes through $k$ only once.



By the strong Markov property $mathbf{P}_k(0 text{ is separator}) = mathbf{P}_0(text{The random walk never returns to zero}).$ Denote by $A_k$ the probability of the random walk, started at $k neq 0,$ to never visit zero and $A_0$ be the probability of never return to zero. By the strong law of large numbers, $A_k = 0$ for all $k$ negative. Now, using first step analysis is easy to deduce $A_{k + 1} = q A_k + pA_{k + 2}$ for $k geq 1,$ $A_0 = p A_1$ and $A_1 = p A_2.$ Then, we have
$$A_{k + 2} - A_{k + 1} = dfrac{q}{p}(A_{k + 1} - A_k) quad (k geq 1).$$
It is easy to show $A_{k+2}-A_{k+1}=(frac{q}{p})^{k+1} A_1$ which then leads to, by means of a telescopic sum,
$$A_k=dfrac{1}{p} left[ sum_{j=0}^k left( dfrac{q}{p} right)^j right] A_0.$$
This shows that $A_k to dfrac{1}{p} dfrac{1}{1 - frac{q}{p}} A_0 = dfrac{1}{p-q}A_0.$




My intuition suggests strongly that $A_k to 1.$ How to prove this formally?




Having this, I can conclude $A_0 = p - q,$ which is very reasonable. So, the probability of zero being separator, starting at $k < 0$ is simply $p - q.$



Consider now the set $mathrm{X}_a = {atext{ is a separator}}.$ The previous can be restated as $$mathbf{P}_0(mathrm{X}_a) = p - q$$ for every $a geq 0.$




Can I use the previous formula to conclude $mathbf{P}_0left(bigcuplimits_{a = 0}^N mathrm{X}_aright) to 1$ as $N to infty$?











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$endgroup$

















    2












    $begingroup$


    Let us consider a biased random walk in $mathbf{Z}$ whose step-lengths satisfy $mathbf{P}(xi = +1) = p > mathbf{P}(xi = -1) = q$ (with $p+q = 1$).



    A value $k in mathbf{Z}$ is a "separator" of the random walk if the random walk started before $k$ passes through $k$ only once.



    By the strong Markov property $mathbf{P}_k(0 text{ is separator}) = mathbf{P}_0(text{The random walk never returns to zero}).$ Denote by $A_k$ the probability of the random walk, started at $k neq 0,$ to never visit zero and $A_0$ be the probability of never return to zero. By the strong law of large numbers, $A_k = 0$ for all $k$ negative. Now, using first step analysis is easy to deduce $A_{k + 1} = q A_k + pA_{k + 2}$ for $k geq 1,$ $A_0 = p A_1$ and $A_1 = p A_2.$ Then, we have
    $$A_{k + 2} - A_{k + 1} = dfrac{q}{p}(A_{k + 1} - A_k) quad (k geq 1).$$
    It is easy to show $A_{k+2}-A_{k+1}=(frac{q}{p})^{k+1} A_1$ which then leads to, by means of a telescopic sum,
    $$A_k=dfrac{1}{p} left[ sum_{j=0}^k left( dfrac{q}{p} right)^j right] A_0.$$
    This shows that $A_k to dfrac{1}{p} dfrac{1}{1 - frac{q}{p}} A_0 = dfrac{1}{p-q}A_0.$




    My intuition suggests strongly that $A_k to 1.$ How to prove this formally?




    Having this, I can conclude $A_0 = p - q,$ which is very reasonable. So, the probability of zero being separator, starting at $k < 0$ is simply $p - q.$



    Consider now the set $mathrm{X}_a = {atext{ is a separator}}.$ The previous can be restated as $$mathbf{P}_0(mathrm{X}_a) = p - q$$ for every $a geq 0.$




    Can I use the previous formula to conclude $mathbf{P}_0left(bigcuplimits_{a = 0}^N mathrm{X}_aright) to 1$ as $N to infty$?











    share|cite|improve this question











    $endgroup$















      2












      2








      2


      0



      $begingroup$


      Let us consider a biased random walk in $mathbf{Z}$ whose step-lengths satisfy $mathbf{P}(xi = +1) = p > mathbf{P}(xi = -1) = q$ (with $p+q = 1$).



      A value $k in mathbf{Z}$ is a "separator" of the random walk if the random walk started before $k$ passes through $k$ only once.



      By the strong Markov property $mathbf{P}_k(0 text{ is separator}) = mathbf{P}_0(text{The random walk never returns to zero}).$ Denote by $A_k$ the probability of the random walk, started at $k neq 0,$ to never visit zero and $A_0$ be the probability of never return to zero. By the strong law of large numbers, $A_k = 0$ for all $k$ negative. Now, using first step analysis is easy to deduce $A_{k + 1} = q A_k + pA_{k + 2}$ for $k geq 1,$ $A_0 = p A_1$ and $A_1 = p A_2.$ Then, we have
      $$A_{k + 2} - A_{k + 1} = dfrac{q}{p}(A_{k + 1} - A_k) quad (k geq 1).$$
      It is easy to show $A_{k+2}-A_{k+1}=(frac{q}{p})^{k+1} A_1$ which then leads to, by means of a telescopic sum,
      $$A_k=dfrac{1}{p} left[ sum_{j=0}^k left( dfrac{q}{p} right)^j right] A_0.$$
      This shows that $A_k to dfrac{1}{p} dfrac{1}{1 - frac{q}{p}} A_0 = dfrac{1}{p-q}A_0.$




      My intuition suggests strongly that $A_k to 1.$ How to prove this formally?




      Having this, I can conclude $A_0 = p - q,$ which is very reasonable. So, the probability of zero being separator, starting at $k < 0$ is simply $p - q.$



      Consider now the set $mathrm{X}_a = {atext{ is a separator}}.$ The previous can be restated as $$mathbf{P}_0(mathrm{X}_a) = p - q$$ for every $a geq 0.$




      Can I use the previous formula to conclude $mathbf{P}_0left(bigcuplimits_{a = 0}^N mathrm{X}_aright) to 1$ as $N to infty$?











      share|cite|improve this question











      $endgroup$




      Let us consider a biased random walk in $mathbf{Z}$ whose step-lengths satisfy $mathbf{P}(xi = +1) = p > mathbf{P}(xi = -1) = q$ (with $p+q = 1$).



      A value $k in mathbf{Z}$ is a "separator" of the random walk if the random walk started before $k$ passes through $k$ only once.



      By the strong Markov property $mathbf{P}_k(0 text{ is separator}) = mathbf{P}_0(text{The random walk never returns to zero}).$ Denote by $A_k$ the probability of the random walk, started at $k neq 0,$ to never visit zero and $A_0$ be the probability of never return to zero. By the strong law of large numbers, $A_k = 0$ for all $k$ negative. Now, using first step analysis is easy to deduce $A_{k + 1} = q A_k + pA_{k + 2}$ for $k geq 1,$ $A_0 = p A_1$ and $A_1 = p A_2.$ Then, we have
      $$A_{k + 2} - A_{k + 1} = dfrac{q}{p}(A_{k + 1} - A_k) quad (k geq 1).$$
      It is easy to show $A_{k+2}-A_{k+1}=(frac{q}{p})^{k+1} A_1$ which then leads to, by means of a telescopic sum,
      $$A_k=dfrac{1}{p} left[ sum_{j=0}^k left( dfrac{q}{p} right)^j right] A_0.$$
      This shows that $A_k to dfrac{1}{p} dfrac{1}{1 - frac{q}{p}} A_0 = dfrac{1}{p-q}A_0.$




      My intuition suggests strongly that $A_k to 1.$ How to prove this formally?




      Having this, I can conclude $A_0 = p - q,$ which is very reasonable. So, the probability of zero being separator, starting at $k < 0$ is simply $p - q.$



      Consider now the set $mathrm{X}_a = {atext{ is a separator}}.$ The previous can be restated as $$mathbf{P}_0(mathrm{X}_a) = p - q$$ for every $a geq 0.$




      Can I use the previous formula to conclude $mathbf{P}_0left(bigcuplimits_{a = 0}^N mathrm{X}_aright) to 1$ as $N to infty$?








      probability probability-theory random-walk






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      edited Jan 17 at 18:32







      Will M.

















      asked Jan 16 at 23:38









      Will M.Will M.

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          2 Answers
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          1












          $begingroup$

          You can show that
          $$
          (1-A_k)=(1-A_1)^kqquadtext{for all $kge 1$}tag{$*$}
          $$

          Why? You know $1-A_k$ is the probability of starting from $k$ and eventually hitting $0$. This is equal to the probability of starting from $k$ and moving eventually to $k-1$, then starting from $k-1$ and moving eventually to $k-2$, then $dots$ then starting from $1$ and moving to $0$. But moving from $i$ to $i-1$ is the same as moving from $1$ to $0$, so each event in that list of $k$ events has probability $(1-A_1)$.



          Plugging $(*)$ with $k=2$ and $k=3$ into
          $$
          A_2=pA_3+qA_1,
          $$

          you can solve for $A_1$. You will find that $A_1<1$, so that $(*)$ implies $A_kto 1$ as $ktoinfty$ .






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            I would change "But moving from $i$ to $i−1$ is the same as moving from $1$ to $0$" to "But 'moving from $i$ to $i−1$ eventually' is the same as moving from '$1$ to $0$ eventually'." Any idea how to tackle the main question?
            $endgroup$
            – Will M.
            Jan 18 at 22:14










          • $begingroup$
            I cannot think of how to use your previous formulas to show $P(bigcup_{a=0}^N X_a)to 1$. Perhaps you can use the principle of inclusion exclusion/ Bonferroni inequalities to get bounds on the probability of this union?
            $endgroup$
            – Mike Earnest
            Jan 18 at 22:51



















          0












          $begingroup$

          I found a nice solution after a while.



          My first question is yes. The reason is much simpler than not. It is well known that for an irreducible Markov chain that is is recurrent we have that: for whatever the initial state $k$ may be and whatever another stat $o$ may be, the probability of starting at $k$ and eventually reaching $o$ is one.



          To my second question. We consider $alpha_n = mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_a^complementright)$ and notice that $(alpha_n)$ is increasing and therefore convergent. We show now that $(alpha_{n^2})$ converges to 1. To see this simply notice that



          $$0 leq 1 - alpha_{n^2} leq mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complementright).$$



          We can define now stopping times $tau_p$ to be the first entrance to state $p$ and measurable times $theta_p$ which are the first returns to $p.$ Then we divide
          $$begin{align*}
          mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complementright) &= mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complement cap{theta_0 < tau_n leq theta_n < tau_{2n}leq theta_{2n}<ldots<tau_{n^2}leqtheta_{n^2}<infty}right)\
          &+mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complement capbigcup_{j=1}^n{tau_j < theta_{(j-1)n}}right)\
          &leqmathbf{P}_0left(theta_0 < tau_n leq theta_n < tau_{2n}leq theta_{2n}<ldots<tau_{n^2}leqtheta_{n^2}<inftyright) + sum_{j=1}^nmathbf{P}_0(tau_j<theta_{(j-1)n})\
          &mathop{=}^triangle gamma_n +sum_{j=1}^n omega_j.
          end{align*}$$



          To deal with $gamma_n$ simply use conditional expectation conditioning on the sigma field generated by $S_0,xi_1, ldots, xi_{tau_n}$ to reach the inequality $gamma_nleq(1-(p-q))gamma_{n-1}$ and so $gamma_n to 0$ (exponentially fast!)



          Observe that $omega_j leq mathbf{P}_0(text{The random walk will ever hit} -n)$ and this is well known to be $(frac{q}{p})^n$ and clearly $n(frac{q}{p})^n to 0$ as well. Q.E.D.






          share|cite|improve this answer









          $endgroup$














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            2 Answers
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            2 Answers
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            active

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            active

            oldest

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            active

            oldest

            votes









            1












            $begingroup$

            You can show that
            $$
            (1-A_k)=(1-A_1)^kqquadtext{for all $kge 1$}tag{$*$}
            $$

            Why? You know $1-A_k$ is the probability of starting from $k$ and eventually hitting $0$. This is equal to the probability of starting from $k$ and moving eventually to $k-1$, then starting from $k-1$ and moving eventually to $k-2$, then $dots$ then starting from $1$ and moving to $0$. But moving from $i$ to $i-1$ is the same as moving from $1$ to $0$, so each event in that list of $k$ events has probability $(1-A_1)$.



            Plugging $(*)$ with $k=2$ and $k=3$ into
            $$
            A_2=pA_3+qA_1,
            $$

            you can solve for $A_1$. You will find that $A_1<1$, so that $(*)$ implies $A_kto 1$ as $ktoinfty$ .






            share|cite|improve this answer









            $endgroup$













            • $begingroup$
              I would change "But moving from $i$ to $i−1$ is the same as moving from $1$ to $0$" to "But 'moving from $i$ to $i−1$ eventually' is the same as moving from '$1$ to $0$ eventually'." Any idea how to tackle the main question?
              $endgroup$
              – Will M.
              Jan 18 at 22:14










            • $begingroup$
              I cannot think of how to use your previous formulas to show $P(bigcup_{a=0}^N X_a)to 1$. Perhaps you can use the principle of inclusion exclusion/ Bonferroni inequalities to get bounds on the probability of this union?
              $endgroup$
              – Mike Earnest
              Jan 18 at 22:51
















            1












            $begingroup$

            You can show that
            $$
            (1-A_k)=(1-A_1)^kqquadtext{for all $kge 1$}tag{$*$}
            $$

            Why? You know $1-A_k$ is the probability of starting from $k$ and eventually hitting $0$. This is equal to the probability of starting from $k$ and moving eventually to $k-1$, then starting from $k-1$ and moving eventually to $k-2$, then $dots$ then starting from $1$ and moving to $0$. But moving from $i$ to $i-1$ is the same as moving from $1$ to $0$, so each event in that list of $k$ events has probability $(1-A_1)$.



            Plugging $(*)$ with $k=2$ and $k=3$ into
            $$
            A_2=pA_3+qA_1,
            $$

            you can solve for $A_1$. You will find that $A_1<1$, so that $(*)$ implies $A_kto 1$ as $ktoinfty$ .






            share|cite|improve this answer









            $endgroup$













            • $begingroup$
              I would change "But moving from $i$ to $i−1$ is the same as moving from $1$ to $0$" to "But 'moving from $i$ to $i−1$ eventually' is the same as moving from '$1$ to $0$ eventually'." Any idea how to tackle the main question?
              $endgroup$
              – Will M.
              Jan 18 at 22:14










            • $begingroup$
              I cannot think of how to use your previous formulas to show $P(bigcup_{a=0}^N X_a)to 1$. Perhaps you can use the principle of inclusion exclusion/ Bonferroni inequalities to get bounds on the probability of this union?
              $endgroup$
              – Mike Earnest
              Jan 18 at 22:51














            1












            1








            1





            $begingroup$

            You can show that
            $$
            (1-A_k)=(1-A_1)^kqquadtext{for all $kge 1$}tag{$*$}
            $$

            Why? You know $1-A_k$ is the probability of starting from $k$ and eventually hitting $0$. This is equal to the probability of starting from $k$ and moving eventually to $k-1$, then starting from $k-1$ and moving eventually to $k-2$, then $dots$ then starting from $1$ and moving to $0$. But moving from $i$ to $i-1$ is the same as moving from $1$ to $0$, so each event in that list of $k$ events has probability $(1-A_1)$.



            Plugging $(*)$ with $k=2$ and $k=3$ into
            $$
            A_2=pA_3+qA_1,
            $$

            you can solve for $A_1$. You will find that $A_1<1$, so that $(*)$ implies $A_kto 1$ as $ktoinfty$ .






            share|cite|improve this answer









            $endgroup$



            You can show that
            $$
            (1-A_k)=(1-A_1)^kqquadtext{for all $kge 1$}tag{$*$}
            $$

            Why? You know $1-A_k$ is the probability of starting from $k$ and eventually hitting $0$. This is equal to the probability of starting from $k$ and moving eventually to $k-1$, then starting from $k-1$ and moving eventually to $k-2$, then $dots$ then starting from $1$ and moving to $0$. But moving from $i$ to $i-1$ is the same as moving from $1$ to $0$, so each event in that list of $k$ events has probability $(1-A_1)$.



            Plugging $(*)$ with $k=2$ and $k=3$ into
            $$
            A_2=pA_3+qA_1,
            $$

            you can solve for $A_1$. You will find that $A_1<1$, so that $(*)$ implies $A_kto 1$ as $ktoinfty$ .







            share|cite|improve this answer












            share|cite|improve this answer



            share|cite|improve this answer










            answered Jan 18 at 0:36









            Mike EarnestMike Earnest

            27.6k22152




            27.6k22152












            • $begingroup$
              I would change "But moving from $i$ to $i−1$ is the same as moving from $1$ to $0$" to "But 'moving from $i$ to $i−1$ eventually' is the same as moving from '$1$ to $0$ eventually'." Any idea how to tackle the main question?
              $endgroup$
              – Will M.
              Jan 18 at 22:14










            • $begingroup$
              I cannot think of how to use your previous formulas to show $P(bigcup_{a=0}^N X_a)to 1$. Perhaps you can use the principle of inclusion exclusion/ Bonferroni inequalities to get bounds on the probability of this union?
              $endgroup$
              – Mike Earnest
              Jan 18 at 22:51


















            • $begingroup$
              I would change "But moving from $i$ to $i−1$ is the same as moving from $1$ to $0$" to "But 'moving from $i$ to $i−1$ eventually' is the same as moving from '$1$ to $0$ eventually'." Any idea how to tackle the main question?
              $endgroup$
              – Will M.
              Jan 18 at 22:14










            • $begingroup$
              I cannot think of how to use your previous formulas to show $P(bigcup_{a=0}^N X_a)to 1$. Perhaps you can use the principle of inclusion exclusion/ Bonferroni inequalities to get bounds on the probability of this union?
              $endgroup$
              – Mike Earnest
              Jan 18 at 22:51
















            $begingroup$
            I would change "But moving from $i$ to $i−1$ is the same as moving from $1$ to $0$" to "But 'moving from $i$ to $i−1$ eventually' is the same as moving from '$1$ to $0$ eventually'." Any idea how to tackle the main question?
            $endgroup$
            – Will M.
            Jan 18 at 22:14




            $begingroup$
            I would change "But moving from $i$ to $i−1$ is the same as moving from $1$ to $0$" to "But 'moving from $i$ to $i−1$ eventually' is the same as moving from '$1$ to $0$ eventually'." Any idea how to tackle the main question?
            $endgroup$
            – Will M.
            Jan 18 at 22:14












            $begingroup$
            I cannot think of how to use your previous formulas to show $P(bigcup_{a=0}^N X_a)to 1$. Perhaps you can use the principle of inclusion exclusion/ Bonferroni inequalities to get bounds on the probability of this union?
            $endgroup$
            – Mike Earnest
            Jan 18 at 22:51




            $begingroup$
            I cannot think of how to use your previous formulas to show $P(bigcup_{a=0}^N X_a)to 1$. Perhaps you can use the principle of inclusion exclusion/ Bonferroni inequalities to get bounds on the probability of this union?
            $endgroup$
            – Mike Earnest
            Jan 18 at 22:51











            0












            $begingroup$

            I found a nice solution after a while.



            My first question is yes. The reason is much simpler than not. It is well known that for an irreducible Markov chain that is is recurrent we have that: for whatever the initial state $k$ may be and whatever another stat $o$ may be, the probability of starting at $k$ and eventually reaching $o$ is one.



            To my second question. We consider $alpha_n = mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_a^complementright)$ and notice that $(alpha_n)$ is increasing and therefore convergent. We show now that $(alpha_{n^2})$ converges to 1. To see this simply notice that



            $$0 leq 1 - alpha_{n^2} leq mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complementright).$$



            We can define now stopping times $tau_p$ to be the first entrance to state $p$ and measurable times $theta_p$ which are the first returns to $p.$ Then we divide
            $$begin{align*}
            mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complementright) &= mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complement cap{theta_0 < tau_n leq theta_n < tau_{2n}leq theta_{2n}<ldots<tau_{n^2}leqtheta_{n^2}<infty}right)\
            &+mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complement capbigcup_{j=1}^n{tau_j < theta_{(j-1)n}}right)\
            &leqmathbf{P}_0left(theta_0 < tau_n leq theta_n < tau_{2n}leq theta_{2n}<ldots<tau_{n^2}leqtheta_{n^2}<inftyright) + sum_{j=1}^nmathbf{P}_0(tau_j<theta_{(j-1)n})\
            &mathop{=}^triangle gamma_n +sum_{j=1}^n omega_j.
            end{align*}$$



            To deal with $gamma_n$ simply use conditional expectation conditioning on the sigma field generated by $S_0,xi_1, ldots, xi_{tau_n}$ to reach the inequality $gamma_nleq(1-(p-q))gamma_{n-1}$ and so $gamma_n to 0$ (exponentially fast!)



            Observe that $omega_j leq mathbf{P}_0(text{The random walk will ever hit} -n)$ and this is well known to be $(frac{q}{p})^n$ and clearly $n(frac{q}{p})^n to 0$ as well. Q.E.D.






            share|cite|improve this answer









            $endgroup$


















              0












              $begingroup$

              I found a nice solution after a while.



              My first question is yes. The reason is much simpler than not. It is well known that for an irreducible Markov chain that is is recurrent we have that: for whatever the initial state $k$ may be and whatever another stat $o$ may be, the probability of starting at $k$ and eventually reaching $o$ is one.



              To my second question. We consider $alpha_n = mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_a^complementright)$ and notice that $(alpha_n)$ is increasing and therefore convergent. We show now that $(alpha_{n^2})$ converges to 1. To see this simply notice that



              $$0 leq 1 - alpha_{n^2} leq mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complementright).$$



              We can define now stopping times $tau_p$ to be the first entrance to state $p$ and measurable times $theta_p$ which are the first returns to $p.$ Then we divide
              $$begin{align*}
              mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complementright) &= mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complement cap{theta_0 < tau_n leq theta_n < tau_{2n}leq theta_{2n}<ldots<tau_{n^2}leqtheta_{n^2}<infty}right)\
              &+mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complement capbigcup_{j=1}^n{tau_j < theta_{(j-1)n}}right)\
              &leqmathbf{P}_0left(theta_0 < tau_n leq theta_n < tau_{2n}leq theta_{2n}<ldots<tau_{n^2}leqtheta_{n^2}<inftyright) + sum_{j=1}^nmathbf{P}_0(tau_j<theta_{(j-1)n})\
              &mathop{=}^triangle gamma_n +sum_{j=1}^n omega_j.
              end{align*}$$



              To deal with $gamma_n$ simply use conditional expectation conditioning on the sigma field generated by $S_0,xi_1, ldots, xi_{tau_n}$ to reach the inequality $gamma_nleq(1-(p-q))gamma_{n-1}$ and so $gamma_n to 0$ (exponentially fast!)



              Observe that $omega_j leq mathbf{P}_0(text{The random walk will ever hit} -n)$ and this is well known to be $(frac{q}{p})^n$ and clearly $n(frac{q}{p})^n to 0$ as well. Q.E.D.






              share|cite|improve this answer









              $endgroup$
















                0












                0








                0





                $begingroup$

                I found a nice solution after a while.



                My first question is yes. The reason is much simpler than not. It is well known that for an irreducible Markov chain that is is recurrent we have that: for whatever the initial state $k$ may be and whatever another stat $o$ may be, the probability of starting at $k$ and eventually reaching $o$ is one.



                To my second question. We consider $alpha_n = mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_a^complementright)$ and notice that $(alpha_n)$ is increasing and therefore convergent. We show now that $(alpha_{n^2})$ converges to 1. To see this simply notice that



                $$0 leq 1 - alpha_{n^2} leq mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complementright).$$



                We can define now stopping times $tau_p$ to be the first entrance to state $p$ and measurable times $theta_p$ which are the first returns to $p.$ Then we divide
                $$begin{align*}
                mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complementright) &= mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complement cap{theta_0 < tau_n leq theta_n < tau_{2n}leq theta_{2n}<ldots<tau_{n^2}leqtheta_{n^2}<infty}right)\
                &+mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complement capbigcup_{j=1}^n{tau_j < theta_{(j-1)n}}right)\
                &leqmathbf{P}_0left(theta_0 < tau_n leq theta_n < tau_{2n}leq theta_{2n}<ldots<tau_{n^2}leqtheta_{n^2}<inftyright) + sum_{j=1}^nmathbf{P}_0(tau_j<theta_{(j-1)n})\
                &mathop{=}^triangle gamma_n +sum_{j=1}^n omega_j.
                end{align*}$$



                To deal with $gamma_n$ simply use conditional expectation conditioning on the sigma field generated by $S_0,xi_1, ldots, xi_{tau_n}$ to reach the inequality $gamma_nleq(1-(p-q))gamma_{n-1}$ and so $gamma_n to 0$ (exponentially fast!)



                Observe that $omega_j leq mathbf{P}_0(text{The random walk will ever hit} -n)$ and this is well known to be $(frac{q}{p})^n$ and clearly $n(frac{q}{p})^n to 0$ as well. Q.E.D.






                share|cite|improve this answer









                $endgroup$



                I found a nice solution after a while.



                My first question is yes. The reason is much simpler than not. It is well known that for an irreducible Markov chain that is is recurrent we have that: for whatever the initial state $k$ may be and whatever another stat $o$ may be, the probability of starting at $k$ and eventually reaching $o$ is one.



                To my second question. We consider $alpha_n = mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_a^complementright)$ and notice that $(alpha_n)$ is increasing and therefore convergent. We show now that $(alpha_{n^2})$ converges to 1. To see this simply notice that



                $$0 leq 1 - alpha_{n^2} leq mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complementright).$$



                We can define now stopping times $tau_p$ to be the first entrance to state $p$ and measurable times $theta_p$ which are the first returns to $p.$ Then we divide
                $$begin{align*}
                mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complementright) &= mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complement cap{theta_0 < tau_n leq theta_n < tau_{2n}leq theta_{2n}<ldots<tau_{n^2}leqtheta_{n^2}<infty}right)\
                &+mathbf{P}_0left( bigcuplimits_{a=0}^n mathrm{X}_{an}^complement capbigcup_{j=1}^n{tau_j < theta_{(j-1)n}}right)\
                &leqmathbf{P}_0left(theta_0 < tau_n leq theta_n < tau_{2n}leq theta_{2n}<ldots<tau_{n^2}leqtheta_{n^2}<inftyright) + sum_{j=1}^nmathbf{P}_0(tau_j<theta_{(j-1)n})\
                &mathop{=}^triangle gamma_n +sum_{j=1}^n omega_j.
                end{align*}$$



                To deal with $gamma_n$ simply use conditional expectation conditioning on the sigma field generated by $S_0,xi_1, ldots, xi_{tau_n}$ to reach the inequality $gamma_nleq(1-(p-q))gamma_{n-1}$ and so $gamma_n to 0$ (exponentially fast!)



                Observe that $omega_j leq mathbf{P}_0(text{The random walk will ever hit} -n)$ and this is well known to be $(frac{q}{p})^n$ and clearly $n(frac{q}{p})^n to 0$ as well. Q.E.D.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Feb 13 at 22:53









                Will M.Will M.

                2,890315




                2,890315






























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