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Date:
Wednesday, November 13, 2002
Time: 4:30 PM
Location: 117, Hayes-Healy Hall, Notre Dame
Speaker:
Joel L. Lebowitz
From: Rutgers, The State University of New Jersey
A
prolific researcher in equilibrium and nonequilibrium statistical mechanics,
Joel Lebowitz, together with Elliot Lieb, proved in 1970 the existence
of the thermodynamic limit for Coulomb systems. In recent years, he has
contributed to our understanding of nonequilibrium systems. Prof. Lebowitz,
a member of the National Academy of Sciences, is not only a renowned mathematician
and physicist but also a tireless organizer and editor in statistical
mechanics. For over thirty-five years, his famous informal Conferences
on Statistical mechanics, known as the "Lebowitz Meetings",
have attracted top international experts and have been invaluable to young
people. He is the editor-in-chief of the Journal of Statistical Physics.
Host:
Mark S. Alber (Mathematics)
Title:
Microscopic Origin of Macroscopic Behavior
Abstract:
Statistical Mechanics provides a framework for describing how well-defined
behavior may result from the nondirected activity of a multitude of interacting
individual entities. The subject was developed for, and has had its greatest
success so far in, relating mesoscopic and macroscopic thermal phenomena
to the microscopic world of atoms and molecules. Some
of the phenomena are simple additive effects of the actions of individual
atoms, e.g., the pressure exerted by gas in the walls of its container,
while others are paradigms of emergent behavior, having no direct counterpart
in the properties of dynamics of individual atoms.Particularly fascinating
and important examples of such emergent phenomena are phase transitions
which would (or should) be astonishing if they were not so familiar.
I will give
an overview of recent developments in this field and discuss ways in which
one may adapt the methods of statistical mechanics to higher level collective
systems in which the relevant basic constituents are themselves more complex
than those for which the theory was developed.
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