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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

Disorder in a quantum spin liquid: flux binding and local moment formation.

Phys Rev Lett 104:23 (2010) 237203

Authors:

AJ Willans, JT Chalker, R Moessner

Abstract:

We study the consequences of disorder in the Kitaev honeycomb model, considering both site dilution and exchange randomness. We show that a single vacancy binds a flux and induces a local moment. This moment is polarized by an applied field h: in the gapless phase, for small h the local susceptibility diverges as χ(h)∼ln(1/h); for a pair of nearby vacancies on the same sublattice, this even increases to χ(h)∼1/(h[ln(1/h)](3/2)). By contrast, weak exchange randomness does not qualitatively alter the susceptibility but has its signature in the heat capacity, which in the gapless phase is power law in temperature with an exponent dependent on disorder strength.

Quantum Hall Systems, and One-Dimensional Systems

World Scientific Publishing (2010) 156-199

Spin glass transition in geometrically frustrated antiferromagnets with weak disorder

(2010)

Authors:

A Andreanov, JT Chalker, TE Saunders, D Sherrington

Disorder in a quantum spin liquid: flux binding and local moment formation

(2010)

Authors:

AJ Willans, JT Chalker, R Moessner

Spin ice under pressure: symmetry enhancement and infinite order multicriticality

ArXiv 1003.4896 (2010)

Authors:

Ludovic DC Jaubert, JT Chalker, Peter CW Holdsworth, R Moessner

Abstract:

We study the low-temperature behaviour of spin ice when uniaxial pressure induces a tetragonal distortion. There is a phase transition between a Coulomb liquid and a fully magnetised phase. Unusually, it combines features of discontinuous and continuous transitions: the order parameter exhibits a jump, but this is accompanied by a divergent susceptibility and vanishing domain wall tension. All these aspects can be understood as a consequence of an emergent SU(2) symmetry at the critical point. We map out a possible experimental realisation.

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