Independence of random variables factors the joint probability mass function as . Therefore
With finite expected values, these rearrangements are justified by absolute convergence: the analogous sum with absolute values equals . Thus
This numbered item specifies the model used below. A convenient sample space is the collection of ordered pairs , each with probability . The corresponding random variables are determined by the sum and difference. Inverting the two equations gives
Thus a candidate pair is possible exactly when and are both integers between and . In particular, and must have the same parity. This inverse description will determine the joint probability mass function.
Summing the two nonzero entries with gives
The remaining probability is , so has the Bernoulli distribution with parameter .
For the other marginal, the two entries at add to , the entry at is , and for the only nonzero entry is already . Thus
and has the Poisson distribution with parameter . This also checks normalization of the joint probability mass function by summing the marginal.
There is no such value of in the specified interval. Indeed, , and the joint probability mass function gives
This contradicts independence for every . Equivalently, has joint probability zero but the product of its marginal probabilities is .
At the suggested value , the covariance is zero, but the same conditional probability contradiction still applies. This is an explicit example of how uncorrelated Bernoulli and Poisson variables need not be independent. Zero covariance controls one mixed moment, whereas independence requires the entire joint probability mass function to factor.
For nonnegative integer-valued independent random variables , factor the expected value of a product:
The Cauchy product explains what this means for individual probability masses:
Every way of splitting the total contributes once. This is convolution of independent random variables; multiplying probability generating functions performs the bookkeeping automatically.
For an original example, take independent and , using the Bernoulli distribution and binomial distribution. Then
so
Direct enumeration of the six pairs gives the same probability masses. For example, total one collects and , with contributions . The coefficients sum to one. The expected value is ; since , the variance is , agreeing with .
Figure 1.
Multiplying probability generating functions accounts for every pair with the same total
. The six cells give the exact joint probability mass function for the chosen independent Bernoulli distribution and binomial distribution. Colors group equal totals; the stacked bars collect their contributions to the coefficients of the product probability generating function. These are calculated model probabilities. Details.
Uncorrelated random variables are insufficient for the product identity. For a concrete counterexample, let be uniform on and set , . Then , but , whereas . Zero covariance controls one mixed moment, not the full joint probability mass function.