dorsal/arxiv
View SchemaAn investigation into why macroscopic systems behave classically
| Authors | David W. Hallwood, Keith Burnett, Jacob Dunningham |
|---|---|
| Categories | |
| ArXiv ID | quant-ph/0609077 |
| URL | https://arxiv.org/abs/quant-ph/0609077 |
| Journal | J. Mod. Opt. 54, 2129 (2007) |
Abstract
We study why it is quite so hard to make a superposition of superfluid flows in a Bose-Einstein condensate. To do this we initially investigate the quantum states of $N$ atoms trapped in a 1D ring with a barrier at one position and a phase applied around it. We show how macroscopic superpositions can in principle be produced and investigate factors which affect the superposition. We then use the Bose-Hubbard model to study an array of Bose-Einstein condensates trapped in optical potentials and coupled to one another to form a ring. We derive analytic expressions for the quality of the superposition for this system, which agrees well with direct diagonalisation of the Hamiltonian for relatively small numbers of atoms. We show that for macroscopic superpositions to be realised there are essentially three straightforward requirements, other than an absence of decoherence, which become harder to achieve as the system size increases. Firstly, the energies of the two distinct superfluid states must be sufficiently close. Secondly, coupling between the two states must be sufficiently strong, and thirdly, other states must be well separated from those participating in the superposition.
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"abstract": "We study why it is quite so hard to make a superposition of superfluid flows\nin a Bose-Einstein condensate. To do this we initially investigate the quantum\nstates of $N$ atoms trapped in a 1D ring with a barrier at one position and a\nphase applied around it. We show how macroscopic superpositions can in\nprinciple be produced and investigate factors which affect the superposition.\nWe then use the Bose-Hubbard model to study an array of Bose-Einstein\ncondensates trapped in optical potentials and coupled to one another to form a\nring. We derive analytic expressions for the quality of the superposition for\nthis system, which agrees well with direct diagonalisation of the Hamiltonian\nfor relatively small numbers of atoms. We show that for macroscopic\nsuperpositions to be realised there are essentially three straightforward\nrequirements, other than an absence of decoherence, which become harder to\nachieve as the system size increases. Firstly, the energies of the two distinct\nsuperfluid states must be sufficiently close. Secondly, coupling between the\ntwo states must be sufficiently strong, and thirdly, other states must be well\nseparated from those participating in the superposition.",
"arxiv_id": "quant-ph/0609077",
"authors": [
"David W. Hallwood",
"Keith Burnett",
"Jacob Dunningham"
],
"categories": [
"quant-ph"
],
"journal_ref": "J. Mod. Opt. 54, 2129 (2007)",
"title": "An investigation into why macroscopic systems behave classically",
"url": "https://arxiv.org/abs/quant-ph/0609077"
},
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