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Marginals and positive-mass conditionals of a finite joint law are probability vectors
Statement
Let be finite nonempty alphabets and let satisfy . Define and . Then both marginals are probability vectors. For each with , the conditional vector is a probability vector; likewise for conditioning on positive-mass . Consequently, if is a finite joint pmf, then for every with , and its two marginals are probability vectors.
Facts & Assumptions
Given: Finite nonempty alphabets and a joint pmf .
Finite distributions, entropy, divergence, and stochastic matrices: a finite probability vector has nonnegative coordinates whose sum is .
Finite commutative-monoid sums are invariant under bijective reindexing, split over disjoint unions, and satisfy the finite Fubini rule: for finite sets and a real array , the sum over equals either iterated sum, and finite sums are invariant under bijective reindexing.
Proof
Every marginal coordinate is nonnegative because it is a finite sum of nonnegative entries of . By [F2], , and the same calculation with the order reversed gives . Thus both marginals are probability vectors by [F1].
Fix with . Each ratio is nonnegative, and . Hence is a probability vector by [F1]. The same argument with fixed gives . If is a joint pmf and , first apply this argument to the pair of finite alphabets and ; then apply step 1.1 to the resulting conditional pmf on . This gives the last assertion.
Depends on
Used by
- Finite conditional entropy Definition
- Finite conditional mutual information Definition
- Finite mutual information Definition
- Conditional block law factors across IID coordinates Lemma
- Conditional type-class cardinality bound Lemma
- Continuity of finite conditional entropy in the joint law Lemma
- Finite conditional mutual information identities and equality Theorem
- Finite entropy and mutual-information chain rules Theorem
Dependency tree · two levels
12 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Robert M. Gray, Entropy and Information Theory, corrected first edition (standard reference, not scraped)
- Yury Polyanskiy and Yihong Wu, Information Theory: From Coding to Learning, author prepublication (standard reference, not scraped)