The expected number in a spherical shell is . Since
the normalized radial density is the Gamma distribution
In the stated units, . The change of variables formula gives
Thus, with ,
Writing , the log likelihood is
Hence
The score variance and negative expected Hessian give Fisher information
Since is Gamma with mean and variance ,
The estimator is unbiased and attains the Cramér-Rao lower bound.
The inverse-square law gives , so observation is equivalent to
For , integrating the Gamma density gives
Therefore
At distance , inclusion requires . Thus
It equals when
The squared chord distance is
Hence the restricted Gaussian process has covariance
It depends only on , so it is stationary. It is periodic in either argument with period , and Gaussian-process realizations inherit that period almost surely because has zero variance.
Let have entries and let
Independent Gaussian measurement errors give the multivariate normal density
The posterior is
A random-walk Metropolis–Hastings algorithm proposes from a symmetric density about the current and accepts with probability
For distinct states, multiplying the transition density by the target density gives
which is symmetric and proves detailed balance. Run multiple dispersed chains, tune proposals during warm-up, inspect traces, effective sample sizes and convergence diagnostics, then estimate the period mean by averaging over retained draws.
For draw , let be the observed covariance matrix, , and
The posterior predictive distribution is a mixture of these conditional Gaussians. Its Monte Carlo mean and variance are
The scale separation makes correlations between distinct observation times negligible, so . Put . With a flat prior,
The next latent value is likewise approximately independent of the past conditional on , with . Marginalizing gives
When every , , , and the predictive variance is .
Normal-normal conjugacy gives
With ,
Write . Then
The terms are independent and centered, so
The unpooled estimate has mean squared error , so population shrinkage improves it.
Convolving the population and measurement distributions gives
Put . With a flat prior on ,
Let . Integrating out gives
Near zero, integrability requires ; at infinity it requires
For integer the posterior is proper exactly when
The choice is allowed for and yields a proper posterior, but it is an improper flat prior on a scale parameter and is not invariant under reparameterization, so sensitivity to more principled scale priors should be checked.
Up to normalization, the joint posterior is
A Gibbs sampler cycle consists of:
  • independently draw every from the normal conditional in part a;
  • draw ;
  • draw
Each proposal is the exact full conditional and is therefore accepted. If the cycle begins with density , integrating the product of the current posterior and successive conditional kernels over all overwritten coordinates leaves
so a full Gibbs sweep preserves the joint posterior.
Completing the square gives
The evidence is the convolution of the likelihood with the prior:
Since
we obtain
The Kullback-Leibler divergence between the posterior normal distribution and is
Substituting and into parts c and d and simplifying gives
Thus the equality holds.
It holds generally whenever the posterior is well defined and the expectations exist. Bayes' theorem gives
Taking posterior expectations yields
which rearranges to the claimed evidence decomposition.

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