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Open Quantum Dynamics of Mesoscopic Bose-Einstein ... - Physics

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Chapter 2Properties <strong>of</strong> an atomic <strong>Bose</strong> condensatein a double-well potentialThis chapter introduces the model <strong>of</strong> the condensate that will be used throughout thefirst half <strong>of</strong> this thesis. We will overview some <strong>of</strong> the semiclassical and quantum properties<strong>of</strong> the double-well condensate in isolation, before considering coupling to the environmentin Sec. 2.3.4. Dynamical properties, including Josephson tunnelling and macroscopicself-trapping, will be analysed, as well as equilibrium properties, such as the transitiontemperature, energy eigenstates and spatial correlations.2.1 Condensate modelWe consider a dilute gas <strong>of</strong> atoms moving in a symmetric double-well tapping potential.This is described by the normally-ordered many-body Hamiltonian[72]:∫ [ ]Ĥ(t) = d 3 2r2m ∇ ˆψ † ·∇ˆψ + V ˆψ † U 0 ˆψ +2 ˆψ † ˆψ† ˆψ ˆψ , (2.1)where m is the atomic mass, U 0 =4π 2 a 0 /m measures the strength <strong>of</strong> the two-bodyinteraction, and a 0 is the s-wave scattering length. The binary hard-sphere collision modelused here to describe interparticle interactions presupposes that all relevant distance scalesare larger then a 0 ∼ 1nm. The Heisenberg picture field operators, ˆψ(r,t)and ˆψ† (r,t),annihilate and create atoms at position r and commute at equal times according to[ˆψ(r), ˆψ† (r )]′ = δ 3 (r − r ′ ). (2.2)20

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