Phase transitions in highly constrained spin systems:
Ordering from the Coulomb phase.
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If you have a question about this talk, please contact Joe Bhaseen.
Many classical, geometrically frustrated antiferromagnets have
macroscopically degenerate ground states. In a class of
three-dimensional systems, the set of degenerate ground states has
power-law correlations and is an example of a Coulomb phase, with
long-wavelength fluctuations described by a Gaussian solenoidal
field. A perturbation applied to the system can lift the degeneracy
and induce a phase transition. Because of the power-law correlations
(or, equivalently, the solenoidal nature of the degrees of freedom),
phase transitions of this kind are unusual.
In this seminar, I aim to give a straightforward introduction to the
area and to discuss these phase transitions from several points of view.
This talk is part of the TCM Blackboard Series series.
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