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Theoretical physicists working at a blackboard collaboration pod in the Beecroft building.
Credit: Jack Hobhouse

John Chalker

Professorial Research Fellow

Research theme

  • Fields, strings, and quantum dynamics
  • Quantum materials

Sub department

  • Rudolf Peierls Centre for Theoretical Physics

Research groups

  • Condensed Matter Theory
John.Chalker@physics.ox.ac.uk
Telephone: 01865 (2)73973
Rudolf Peierls Centre for Theoretical Physics, room 70.07
  • About
  • Teaching
  • Publications

Publisher's Note: Site dilution in the Kitaev honeycomb model [Phys. Rev. B 84, 115146 (2011)]

Physical Review B American Physical Society (APS) 84:20 (2011) 209901

Authors:

AJ Willans, JT Chalker, R Moessner
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3D loop models and the CP(n-1) sigma model.

Phys Rev Lett 107:11 (2011) 110601

Authors:

Adam Nahum, JT Chalker, P Serna, M Ortuño, AM Somoza

Abstract:

Many statistical mechanics problems can be framed in terms of random curves; we consider a class of three-dimensional loop models that are prototypes for such ensembles. The models show transitions between phases with infinite loops and short-loop phases. We map them to CP(n-1) sigma models, where n is the loop fugacity. Using Monte Carlo simulations, we find continuous transitions for n=1, 2, 3, and first order transitions for n≥5. The results are relevant to line defects in random media, as well as to Anderson localization and (2+1)-dimensional quantum magnets.
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Site dilution in Kitaev's honeycomb model

ArXiv 1106.0732 (2011)

Authors:

AJ Willans, JT Chalker, R Moessner

Abstract:

We study the physical consequences of site dilution in Kitaev's honeycomb model, in both its gapped and gapless phases. We show that a vacancy binds a flux of the emergent $Z_2$ gauge field and induces a local moment. In the gapped phase this moment is free while in the gapless phase the susceptibility has the dependence $\chi(h)\sim\ln(1/h)$ on field strength $h$. Vacancy moments have interactions that depend on their separation, their relative sublattice, and the phase of the model. Strikingly, in the gapless phase, two nearby vacancies on the same sublattice have a parametrically larger $\chi(h)\sim(h[\ln(1/h)]^{3/2})^{-1}$. In the gapped phase, even a finite density of randomly distributed vacancies remains tractable, via a mapping to a bipartite random hopping problem. This leads to a strong disorder form of the low-energy thermodynamics, with a Dyson-type singularity in the density of states for excitations.
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Spin quantum Hall effect and plateau transitions in multilayer network models

ArXiv 1101.5921 (2011)

Authors:

JT Chalker, M Ortuño, AM Somoza

Abstract:

We study the spin quantum Hall effect and transitions between Hall plateaus in quasi two-dimensional network models consisting of several coupled layers. Systems exhibiting the spin quantum Hall effect belong to class C in the symmetry classification for Anderson localisation, and for network models in this class there is an established mapping between the quantum problem and a classical one involving random walks. This mapping permits numerical studies of plateau transitions in much larger samples than for other symmetry classes, and we use it to examine localisation in systems consisting of $n$ weakly coupled layers. Standard scaling ideas lead one to expect $n$ distinct plateau transitions, but in the case of the unitary symmetry class this conclusion has been questioned. Focussing on a two-layer model, we demonstrate that there are two separate plateau transitions, with the same critical properties as in a single-layer model, even for very weak interlayer coupling.
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Geometrically Frustrated Antiferromagnets: Statistical Mechanics and Dynamics

Chapter in Introduction to Frustrated Magnetism, Springer Nature 164 (2011) 3-22
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