The ``Coulomb Phase'' in Frustrated Systems
By Christopher L. Henley. 2009
357 citations recorded by the source corpus.
The “Coulomb phase” is an emergent state for lattice models (particularly highly frustrated antiferromagnets), which have local constraints that can be mapped to a divergence-free “flux.” The coarse-grained versions of this flux or polarization behave analogously to electric or magnetic fields; in particular, defects at which the local constraint is violated behave as effective charges with Coulomb interactions. I survey the derivation of the characteristic power-law correlation functions and the pinch points in reciprocal space plots of diffuse scattering, as well as applications to magnetic relaxation, quantum-mechanical generalizations, phase transitions to long-range-ordered states, and the effects of disorder.
Subfields: Condensed Matter Physics, Electronic, Optical and Magnetic Materials
View Paper: https://www.semanticscholar.org/paper/b21a04eb3334561923a9bf930b9817757734ff65
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In Condensed Matter Physics
- Salvatore Torquato
- Frank H. Stillinger
- Weihua Wang
- Stephen R. Williams
- C. Royall
- Tom C. Lubensky
- C. L. Kane
In Electronic, Optical and Magnetic Materials
Citations in the corpus
- Ensemble Theory for Stealthy Hyperuniform Disordered Ground States (2015, background): “[22] C.”