SC740 SEMINAR REPORT 14 for Frederick L. Jones
PRESENTERS: Dr. Jiu Ding and Dr. Lawrence Mead
TOPIC: Maximum Entropy Method: Ideas and Applications
OVERVIEW
Noting the importance of Maximum Entropy Method to scientific research in such fields as Thermal Physics and Statistical Physics, Dr. Lawrence Mead provided a general mathematical introduction to the Maximum Entropy function, before Dr. Jiu Ding provided an overview of the Maximum Entropy Method.
The Maximum Entropy Method is a useful numerical scheme for constructing the unknown density function, and it can also be used to compute invariant measures of chaotic dynamics.
AN INTRODUCTION TO MAXIMUM ENTROPY
Dr. Lawrence Mead provided a general mathematical introduction to the Maximum Entropy function. Dr. Mead noted that in order to construct a maximum entropy function, one must reconstruct a density function p(x) from limited information. The density function p(x) defines power moments as follows :
ó
1m
n = ô x n p(x) dxõ
The least biased or most likely function p(x) is the one that maximizes the following function:
ó
1 N ó 1S =
- ô p(x) [ ln p(x) - 1] dx + å l n [ m n - ô x M p(x) dx ]õ
0 M=1 õ 0
THE MAXIMUM ENTROPY METHOD
Dr. Jiu Ding provided an overview of the Maximum Entropy Method. The Maximum Entropy Method is a useful numerical scheme for constructing the unknown density function, and it can also be used to compute invariant measures of chaotic dynamics.
Dr. Ding covered entropy transforms such as the Birkhoff (1933) I.E.T., i.e,
1 N-1
ó _______lim ---
å xI (Sn(x)) = ô ( 1 / p Ö p (1 - x) ) dxN
® ¥ N n=0 õ Iand entropy operators such as the Probenius-Penon operator, i.e,
ó
óô
P f(x) dx = ô f(x) dxõ
A õ S-1 (A)
SUMMARY AND CONCLUSIONS
Noting the importance of Maximum Entropy Method to scientific research in such fields as Thermal Physics and Statistical Physics, Dr. Lawrence Mead provided a general mathematical introduction to the Maximum Entropy function, before Dr. Jiu Ding provided an overview of the Maximum Entropy Method.
The Maximum Entropy Method is a useful numerical scheme for constructing the unknown density function, and it can also be used to compute invariant measures of chaotic dynamics.