Abstract
Symmetry breaking phase transitions play an important role in nature. When a system traverses such a transition at a finite rate, its causally disconnected regions choose the new broken symmetry state independently. Where such local choices are incompatible, topological defects can form. The Kibble-Zurek mechanism predicts the defect densities to follow a power law that scales with the rate of the transition. Owing to its ubiquitous nature, this theory finds application in a wide field of systems ranging from cosmology to condensed matter. Here we present the successful creation of defects in ion Coulomb crystals by a controlled quench of the confining potential, and observe an enhanced power law scaling in accordance with numerical simulations and recent predictions. This simple system with well-defined critical exponents opens up ways to investigate the physics of non-equilibrium dynamics from the classical to the quantum regime. © 2013 Macmillan Publishers Limited. All rights reserved.
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CITATION STYLE
Pyka, K., Keller, J., Partner, H. L., Nigmatullin, R., Burgermeister, T., Meier, D. M., … Mehlstäubler, T. E. (2013). Topological defect formation and spontaneous symmetry breaking in ion Coulomb crystals. Nature Communications, 4. https://doi.org/10.1038/ncomms3291
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