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Abstract
We study the ground state for many interacting bosons in a double-well potential,
in a joint limit where the particle number and the distance between the
potential wells both go to infinity. Two single-particle orbitals (one for each
well) are macroscopically occupied, and we are concerned with deriving the
corresponding effective Bose–Hubbard Hamiltonian. We prove an energy
expansion, including the two-mode Bose–Hubbard energy and two independent
Bogoliubov corrections (one for each potential well), and a variance bound for
the number of particles falling inside each potential well. The latter is a
signature of a correlated ground state in that it violates the central limit
theorem.
Keywords
many-body quantum mechanics, Bose–Einstein condensation,
Bose–Hubbard model, Bogoliubov theory
Mathematical Subject Classification
Primary: 35Q40, 81V73, 82B10
Secondary: 47A75, 49S05
Milestones
Received: 31 May 2021
Revised: 28 January 2022
Accepted: 16 March 2022
Published: 16 October 2023
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