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Bounded densities with finite second moments have finite differential entropy
Statement
Let be a Lebesgue probability density on with and . Then , so the differential entropy in Differential entropy for real densities is a finite real number.
Facts & Assumptions
Given: A Lebesgue probability density with finite essential supremum and finite second moment.
Differential entropy for real densities: differential entropy is defined by in the absolutely integrable case.
Proof
Let and . On , , so the positive part is integrable. For , ; with , this gives . Thus on , The right side is integrable because is a probability density and is bounded by a constant plus . Hence the negative part of is integrable.
Both parts of are integrable by step 1.1. Therefore , and [F1] defines a finite differential entropy.
Depends on
Used by
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Sources
- Yury Polyanskiy and Yihong Wu, Information Theory: From Coding to Learning, author prepublication (standard reference, not scraped)
- John Duchi, Lecture Notes on Statistics and Information Theory (standard reference, not scraped)