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The event (m=N) represents no change within the observed sequence: every observation belongs to the first-rate segment, and the second-rate segment is empty. It is not the event $\lambda =\varphi$; under continuous independent rate priors that exact equality has posterior probability zero. The endpoint is instead a distinct index value with positive prior mass.

For retained Markov chain Monte Carlo draws $({\lambda }^{(b)},{\varphi }^{(b)},m^{(b)})$, the direct estimate isIts consistency follows from the ergodic theorem for a positive Harris recurrent Markov chain. The draws are correlated, so an independent-binomial standard error would generally be incorrect; uncertainty should account for the Markov chain Monte Carlo asymptotic variance.

A conditional Monte Carlo alternative averages the conditional probability from the preceding solution:The tower property of conditional expectation shows that its posterior expectation is the same target. This replaces an indicator by its conditional expectation; for correlated chains one should assess efficiency rather than automatically assume its entire asymptotic variance is smaller.

An exact finite-sum check is available by integrating out both rates. The marginal posterior weights of a Poisson count change point areThese follow from the Gamma function integral ${\int }_0^{\infty }{z}^{a-1}{e}^{-bz}dz=\Gamma (a)/b^a$. All omitted prior-normalization and factorial factors are independent of $j$, so they cancel from this ratio. This exact calculation provides a useful independent check on either simulation estimate.

The posterior kernel gives two gamma full conditional distributions directly:with rates as the second parameters. For the index, terms independent of the proposed value $j$ cancel. Its conditional weights areDefine ${\ell }_j=j(\varphi -\lambda )+S_j\log (\lambda /\varphi )$ and ${\ell }_{\max }={\max }_j{\ell }_j$. The normalized categorical probabilities areSubtracting the largest log weight prevents needless numerical overflow, an application of the log-sum-exp function.

Precompute the cumulative counts $S_j$. Initialize any $m\in \{1,\dots ,N\}$ and positive rates. At each iteration, draw $\lambda$ from its gamma conditional given the current index, draw $\varphi$ from its gamma conditional given that index, and draw a new index from the categorical probabilities using the newly drawn rates. Repeat and retain the parameter triples after initialization effects have diminished. These are the Gibbs updates for a Poisson count change point.

To verify invariance rather than just identify a sampler, a coordinate update integrates the old joint density as $\pi (\lambda ,\varphi ,m\mid x)=\pi (\lambda \mid \varphi ,m,x)\pi (\varphi ,m\mid x)$ and replaces the first factor by an independent draw from the same conditional. The joint posterior distribution is therefore unchanged. The same argument applies to the other two updates, so their composition preserves the posterior. All gamma densities and all categorical weights are positive on their supports. The full-sweep transition density is consequently positive across the joint support, giving the usual irreducibility and aperiodicity conditions for this proper-posterior Gibbs sampler. This supports posterior long-run averages under the ergodic theorem for a positive Harris recurrent Markov chain.

A convenient general-state-space ergodic theorem is the following. For a positive Harris recurrent Markov chain with invariant probability measure $\pi$, and a measurable function $h$ with $\pi |h|<\infty$,Here $\pi h=\int hd\pi$ is the stationary expected value. Harris recurrence means that every set of positive irreducibility measure is visited almost surely from every state; positive recurrence supplies an invariant probability rather than only an infinite invariant measure. The ergodic theorem for a positive Harris recurrent Markov chain holds from any starting state under these Harris hypotheses. aperiodicity is not necessary just for averages.

A useful sufficient form of the central limit theorem for a geometrically ergodic Markov chain adds aperiodicity, geometric ergodicity, and $\pi (|h{|}^{2+\delta })<\infty$ for some $\delta >0$. It givesThese are sufficient hypotheses, not a claim that irreducibility alone ensures a central limit theorem. The Markov chain Monte Carlo asymptotic variance uses stationary covariances ${\gamma }_h(k)={\mathrm{Cov}}_{\pi }(h(X_0),h(X_k))$, with ${\gamma }_h(0)={\mathrm{Var}}_{\pi }h$. The series is absolutely convergent under the stated sufficient assumptions. If ${\gamma }_h(0)>0$, write ${\rho }_h(k)={\gamma }_h(k)/{\gamma }_h(0)$ and $v_h={\gamma }_h(0){\tau }_{\mathrm{int}}$, where the integrated autocorrelation time is ${\tau }_{\mathrm{int}}=1+2{\sum }_{k\ge 1}{\rho }_h(k)$. When $v_h>0$, the effective sample size of a Markov chain is approximately $n/{\tau }_{\mathrm{int}}$. Negative correlations can reduce the asymptotic variance; a zero asymptotic variance gives a degenerate normal limit. For constant $h$, variance is zero and the autocorrelation normalization is undefined.

Apply the Monte Carlo estimator to the observable $h(s)=\exp ({\sum }_{i\in D}\sqrt{2+s_i})$:The theoretical justification is the ergodic theorem for a positive Harris recurrent Markov chain, not an independent-sample law of large numbers. The Markov chain has finite state space, is irreducible, and has the strictly positive posterior distribution as invariant law, so it is positive recurrent and Harris recurrent with counting measure. The observable is bounded: $e^{K^2}\le h(s)\le e^{\sqrt{3}{K}^2}$. Thus the estimator converges almost surely to the posterior expected value from any initial configuration.

Each state also has positive self-transition probability, so the chain is an aperiodic Markov chain. Finiteness then gives geometric convergence and the relevant central limit theorem; serial dependence determines the Markov chain Monte Carlo asymptotic variance if error bars are required. A fixed finite burn-in can be discarded without changing consistency, but independence of the retained states should not be assumed.

Use the ergodic theorem for a positive Harris recurrent Markov chain: for an invariant distribution $\pi$ and an integrable function $h$, the time average converges almost surely to $\int hd\pi$ under the usual ergodicity conditions. This is the relevant theorem for correlated Metropolis–Hastings algorithm output, rather than the strong law of large numbers. Here $h(x)=x_1$ is integrable. Indeed, puttingwe have $V(x)\ge (x_1-4{)}^2+(x_2-4{)}^2-32$, which bounds the unnormalized density by a constant times an integrable Gaussian density and also gives finite first moments.

For a proposal scale $s>0$, initialize $X_0$ anywhere in ${\mathbb{R}}^2$. At each step draw independent random variables $Z_1,Z_2$ with the standard normal distribution and an independent uniform $U$, propose $Y=X_t+s(Z_1,Z_2)$, and accept whenOtherwise set $X_{t+1}=X_t$. The normal proposal is symmetric, so its density cancels; the target normalizing constant $c$ also cancels. Include every state in the average, including repeated states after rejection. The ergodic theorem for a positive Harris recurrent Markov chain then givesA fixed discarded initial segment does not change this limit.

Small proposal variance gives high acceptance but tiny moves and strong serial dependence. Large variance gives more ambitious moves, but many proposals enter very low-density regions and are rejected, creating long runs at one state. An intermediate scale should be assessed by exploration and effective sample size of a Markov chain, not acceptance rate alone.

This density has two modes, at $(2+\sqrt{3},2-\sqrt{3})$ and their interchange. To see this, stationary points satisfy $x_1(1+x_2^2)=x_2(1+x_1^2)=4$, implying either $x_1=x_2$ or $x_1{x}_2=1$. The unequal solutions have $x_1+x_2=4$ and are local minima of $V$; the equal solution is a saddle. Mode switching is therefore a material part of proposal-scale selection: a chain confined to one mode can have high acceptance and a misleading finite-run estimate.

A Harris recurrent chain visits every measurable set of positive irreducibility measure almost surely. Positive Harris recurrence additionally supplies an invariant probability measure. The ergodic theorem for a positive Harris recurrent Markov chain gives consistency of time averages of integrable functions.