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Finite Bernoulli difference laws and parity of moments
Statement
Let and let be independent Bernoulli random variables on a finite probability space. Put . Then and . For every positive integer , is zero if is odd and if is even; , with the constant one.
More generally, let be a finite set of unordered edges, meaning two-element subsets of a finite vertex set, and suppose that the family of all its Bernoulli coordinates is mutually independent. Then the differences are mutually independent. This hypothesis holds for the coordinate variables on the finite product of two Bernoulli spaces per edge. Defining for distinct vertices makes : reflection is the same random variable, not another independent copy.
Statement references
Facts & Assumptions
By Bernoulli random variables and binomial random variables as sums of independent Bernoulli trials, a Bernoulli variable has probabilities and at and , respectively.
By Pairwise and mutual independence of finite-valued random variables, mutual independence means that every simultaneous assignment to any nonempty subfamily has probability equal to the product of its coordinate probabilities.
By The finite product of finite probability spaces, a product outcome has weight equal to the product of its coordinate weights; the empty product has weight one.
By Expectation of a real random variable on a finite probability space, expectation is the sum of a random variable's values weighted by outcome probabilities.
By Finite probability spaces, outcome weights, events, and event probabilities, a finite probability space has nonnegative outcome weights summing to one, and for each event . Summing over disjoint events therefore sums their probabilities.
By Real random variables on finite probability spaces and their finite distributions, a finite real random variable is a function , and its law assigns each value the probability of its fibre. Differences and nonnegative integer powers here are formed pointwise as functions on the same finite outcome set, with zeroth powers defined as the constant one.
Proof
Given: The finite probability spaces and variables in the statement.
Goal: Establish the difference law, its moments, and independence across edge blocks.
By independence, the four assignments have respective probabilities . Their differences are respectively , giving the asserted law, including at and .
For , the weighted sum over these values is , since the zero term vanishes. This gives the two parity cases. The zeroth power is the constant one, whose expectation is one by normalization.
For a nonempty and prescribed values , sum the joint coordinate-assignment probabilities over the disjoint assignments satisfying for each . Mutual independence factors every summand into its edge-block factors, and finite distributivity factors the sum into . Thus the differences are mutually independent; impossible values have probability zero, and the empty family is independent by convention.
On the stated finite product, summing product weights over all unprescribed coordinates gives one for each such coordinate, so every prescribed coordinate assignment has the product of its marginal weights. The coordinates are therefore mutually independent. Finally, , so the two reflected entries are literally the same difference variable.
Depends on
- Bernoulli random variables and binomial random variables as sums of independent Bernoulli trials
- Pairwise and mutual independence of finite-valued random variables
- The finite product of finite probability spaces
- Expectation of a real random variable on a finite probability space
- Finite probability spaces, outcome weights, events, and event probabilities
- Real random variables on finite probability spaces and their finite distributions
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