The joint probability mass function is
It is nonnegative and its sum over is one. Summing over one coordinate gives the other marginal probability mass function.
For , the conditional probability mass function is
The denominator is the sum of the numerator over all possible , so these conditional probabilities sum to one.
A partition of a sample space is a finite or countable family of pairwise disjoint events whose union is the whole sample space. If is integrable, the law of total expectation states
This follows by summing over the partition of a sample space; absolute integrability justifies the countable sum. For nonnegative , the identity also holds with infinite expectations. Zero-probability parts contribute zero without requiring a conditional value on them.
The first swap necessarily removes one red ball from urn 1 and replaces it with a blue ball. Thus with probability one.
Conditional on , urn 1 has red and blue balls, while urn 2 has red and blue balls. The independent selections therefore give
Every other conditional probability is zero. The out-of-range terms at or already have zero probability. These are the transition probabilities of the Bernoulli-Laplace diffusion model.
Only upward and downward moves change the value, so the conditional expectation is
Thus .
Apply the law of total expectation to the partition of a sample space given by the possible values of . Since the conditional mean is affine,
Here . This uses linearity of expectation and does not assert independence of successive urn counts.
The equilibrium of the first-order linear recurrence is . Subtracting it gives
Consequently
For , interpret the formula at through the initial condition: , while for . For every , .

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