A disordered spin model with a quantum-induced phase transition related to Bose condensation in a random potential
A disordered spin model with a quantum-induced phase transition related to Bose condensation in a random potential
The authors consider a random magnetic model which is related to Bose condensation in the presence of a random potential. It is an XY model with a random z field. The classical model always has an ordered ground state. The nature of the ground state is unusual: the main contribution to the spontaneous magnetisation comes from a dilute set of weakly interacting pairs of spins. Within each pair the spins are strongly coupled, so for low-energy dynamics only the motion of the total spin of the pair is relevant. This allows the construction of an effective Hamiltonian only involving the pairs' total spins. When this is semi-classically quantised via a 1/S expansion, they find that the zero-point spin wave motion destroys the magnetised ground state if either the number of spin states is sufficiently small (for fixed strength of disorder), or for sufficiently large disorder (for fixed number of spin states). Finally they discuss the relation of the model to the problem of Bose condensation in a random potential, where the interaction strength is related to the number of spin states in the spin model
5829-5837
Brackstone, M.A.
ec944365-2b0a-4f67-b331-936750d9d383
Gunn, S
d61115fe-7601-4f65-8929-1b4df2889eab
December 1987
Brackstone, M.A.
ec944365-2b0a-4f67-b331-936750d9d383
Gunn, S
d61115fe-7601-4f65-8929-1b4df2889eab
Brackstone, M.A. and Gunn, S
(1987)
A disordered spin model with a quantum-induced phase transition related to Bose condensation in a random potential.
Journal of Physics C: Solid State Physics, 20 (34), .
(doi:10.1088/0022-3719/20/34/018).
Abstract
The authors consider a random magnetic model which is related to Bose condensation in the presence of a random potential. It is an XY model with a random z field. The classical model always has an ordered ground state. The nature of the ground state is unusual: the main contribution to the spontaneous magnetisation comes from a dilute set of weakly interacting pairs of spins. Within each pair the spins are strongly coupled, so for low-energy dynamics only the motion of the total spin of the pair is relevant. This allows the construction of an effective Hamiltonian only involving the pairs' total spins. When this is semi-classically quantised via a 1/S expansion, they find that the zero-point spin wave motion destroys the magnetised ground state if either the number of spin states is sufficiently small (for fixed strength of disorder), or for sufficiently large disorder (for fixed number of spin states). Finally they discuss the relation of the model to the problem of Bose condensation in a random potential, where the interaction strength is related to the number of spin states in the spin model
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Published date: December 1987
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Local EPrints ID: 75533
URI: http://eprints.soton.ac.uk/id/eprint/75533
ISSN: 0022-3719
PURE UUID: 26db5d86-db42-40c2-acfc-00a11fdda9cb
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Date deposited: 11 Mar 2010
Last modified: 13 Mar 2024 22:57
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Author:
M.A. Brackstone
Author:
S Gunn
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