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

Prof John Cardy FRS

Emeritus Professor

Sub department

  • Rudolf Peierls Centre for Theoretical Physics
john.cardy@all-souls.ox.ac.uk
  • About
  • Publications

Quantum quenches in extended systems

JOURNAL OF STATISTICAL MECHANICS-THEORY AND EXPERIMENT (2007) ARTN P06008

Authors:

Pasquale Calabrese, John Cardy
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Schramm-Loewner evolution in the three-state Potts model - a numerical study

JOURNAL OF STATISTICAL MECHANICS-THEORY AND EXPERIMENT (2007) ARTN P08020

Authors:

Adam Gamsa, John Cardy
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Identification of the stress-energy tensor through conformal restriction in SLE and related processes

Communications in Mathematical Physics 268:3 (2006) 687-716

Authors:

B Doyon, V Riva, J Cardy

Abstract:

We derive the Ward identities of Conformal Field Theory (CFT) within the framework of Schramm-Loewner Evolution (SLE) and some related processes. This result, inspired by the observation that particular events of SLE have the correct physical spin and scaling dimension, and proved through the conformal restriction property, leads to the identification of some probabilities with correlation functions involving the bulk stress-energy tensor. Being based on conformal restriction, the derivation holds for SLE only at the value κ = 8/3, which corresponds to the central charge c = 0 and the case when loops are suppressed in the corresponding O(n) model. © Springer-Verlag 2006.
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Time dependence of correlation functions following a quantum quench

Physical Review Letters 96:13 (2006)

Authors:

P Calabrese, J Cardy

Abstract:

We show that the time dependence of correlation functions in an extended quantum system in d dimensions, which is prepared in the ground state of some Hamiltonian and then evolves without dissipation according to some other Hamiltonian, may be extracted using methods of boundary critical phenomena in d+1 dimensions. For d=1 particularly powerful results are available using conformal field theory. These are checked against those available from solvable models. They may be explained in terms of a picture, valid more generally, whereby quasiparticles, entangled over regions of the order of the correlation length in the initial state, then propagate classically through the system. © 2006 The American Physical Society.
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Time dependence of correlation functions following a quantum quench

Physical Review Letters 96 (2006) 136801 4pp

Authors:

JL Cardy, P. Calabrese
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