For distribution
CM ICTP - Trieste
cm at ictp.it
Fri Jan 11 09:49:20 CET 2008
JOINT ICTP/SISSA STATISTICAL PHYSICS SEMINAR
Tuesday, 15 January - 12:30 hrs.
Lecture Room 'D' - SISSA Main Building
G. FALKOVICH ( The Weizmann Institute of Science, Rehovot )
" Broken and emerging symmetries of turbulence "
Abstract
This is a review of most fundamental (symmetry) aspects of turbulence
for a physical audience. To excite turbulence, one needs an external
pumping; to keep it in a steady state one needs dissipation. Pumping
and dissipation break symmetries like time-reversibility, isotropy,
scale invariance. Since pumping and dissipation act on vastly
different scales, the question appears what are the statistical
properties of a system at the intermediate scales (called inertial
interval or transparency window). I shall describe both anomalies
(when the symmetry is not restored even when the symmetry-breaking
factor goes to zero) and emerging symmetries like conformal invariance.
In the latter case, by using the language of Schramm-Loewner Evolution
for analysis of fractal clusters, one discovers a surprising similarity
between critical phenomena and turbulence.
==========
JOINT ICTP/SISSA STATISTICAL PHYSICS SEMINAR
Wednesday, 16 January - 11:30 a.m.
Seminar Room - ICTP Main Building (first floor)
A.C.C. COOLEN ( King's College London )
"Spin models on random graphs with controlled topologies beyond degree
constraints"
Abstract
We study Ising spin models on finitely connected random interaction
graphs which are drawn from an ensemble in which not only the degree
distribution p(k) can be chosen arbitrarily, but which allows for
further fine-tuning of the topology via preferential attachment of
edges on the basis of an arbitrary function Q(k,k') of the degrees of
the vertices involved. We solve these models using finite connectivity
equilibrium replica theory, within the replica symmetric ansatz. In our
ensemble of graphs, phase diagrams of the spin system are found to
depend no longer only on the chosen degree distribution, but also on
the choice made for Q(k,k'). The increased ability to control
interaction topology in solvable models beyond prescribing only the
degree distribution of the interaction graph enables a more accurate
modeling of real-world interacting particle systems by spin systems on
suitably defined random graphs.
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