Abstract

Recently, Savaré-Toscani proved that the Rényi entropy power of general probability densities solving the p-nonlinear heat equation in is a concave function of time under certain conditions of three parameters , which extends Costa’s concavity inequality for Shannon’s entropy power to the Rényi entropy power. In this paper, we give a condition of under which the concavity of the Rényi entropy power is valid. The condition contains Savaré-Toscani’s condition as a special case and much more cases. Precisely, the points satisfying Savaré-Toscani’s condition consist of a two-dimensional subset of , and the points satisfying the condition consist a three-dimensional subset of . Furthermore, gives the necessary and sufficient condition in a certain sense. Finally, the conditions are obtained with a systematic approach.

Highlights

  • In 1948, Claude Elwood Shannon [1] first introduced his mathematical theory of information

  • Savaré-Toscani [22] proved that the concavity of entropy power is a property which is not restricted to the Shannon entropy power (3) in connection with the heat Equation (4), but it holds for the p-th Rényi entropy power (2)

  • We show that the points satisfying T(1, 2) consist of a three-dimensional subset of

Read more

Summary

Introduction

In 1948, Claude Elwood Shannon [1] first introduced his mathematical theory of information. Related to EPI, Costa [14] proved that the Shannon entropy power N (u) = 2πe e is a concave function in t; that is, (d/dt) N (u) ≥ 0 and (d /d t) N (u) ≤ 0. Savaré-Toscani [22] proved that the concavity of entropy power is a property which is not restricted to the Shannon entropy power (3) in connection with the heat Equation (4), but it holds for the p-th Rényi entropy power (2). We give a generalization for the concavity of the p-th Rényi entropy power (CREP).

Notations
Sketch of the Proof
The Equational Constraints
Proof of Lemma 1
A Generalized Version of CREP
Reduce to a Finite Problem
Simplify the Problem with the Equational Constraints
Compare with Existing Results
Proof of Theorem 3
Conclusions

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.