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

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2. Properties <strong>of</strong> an atomic <strong>Bose</strong> condensate in a double-well potentialIn the two-mode approximation, we expand the field operators in terms <strong>of</strong> the localmodes and introduce the Heisenberg picture annihilation and creation operators∫ĉ j (t) = d 3 ru ∗ j (r) ˆψ(r,t) (2.12)so that [ĉ j , ĉ † k ] ≈ δ jk. The validity <strong>of</strong> this expansion is ensured when the overlap is small:RE 0= Ω ω 0≪ 1. (2.13)The ratio <strong>of</strong> the separation <strong>of</strong> the minima <strong>of</strong> the global potential V (r) tothepositionuncertainty in the states u j (r) can be as small as 2q 0 /r 0 = 6 (as in some <strong>of</strong> the simulationspresented in this thesis), and yet still satisfy this condition. The many-body Hamiltonianthen reduces to the following two-mode approximation:Ĥ 2a (t) = E 0 (ĉ † 1ĉ1 +ĉ † 2ĉ2)+ Ω ()2 (ĉ 1ĉ † 2 +ĉ† 1ĉ2)+κ (ĉ † 1 )2 ĉ 2 1 +(ĉ † 2 )2 ĉ 2 2 , (2.14)where κ = U 0 /2V eff ,andV −1eff= ∫ d 3 r|u 0 (r)| 4 is the effective mode volume <strong>of</strong> each well.Here we have retained only the self-interaction contribution to the nonlinearity, as thecross-interaction contributions are <strong>of</strong> order ɛ 2 .The two-mode approximation is valid when many-body interactions produce only smallmodifications <strong>of</strong> the ground state properties <strong>of</strong> the individual potentials. This is true whenω 0 =22mr 2 0≫ N|U 0|V eff. (2.15)Using V eff ≈ 8π 3/2 r 3 0atoms:for this case, we obtain the following condition on the number <strong>of</strong>N ≪ r 0|a 0 | . (2.16)If we choose values <strong>of</strong> r 0 =5µm and a 0 =5nm, thenN = 100 satisfies this criterion.Thus the two-mode approximation is valid for small number <strong>of</strong> atoms compared to currentexperiments with N =10 3 ↔ 10 6 .In studying the semiclassical and quantum dynamics <strong>of</strong> the two-mode condensate, wewill only be concerned with the case where κ>0, corresponding to repulsive interactionbetween atoms. A negative κ is also possible, although gasses with this attractive interactionare rarely used in experiments. Because we have chosen to study condensates inspatially separated wells, the nonlinear cross-interaction between the condensates is negligible.However, one may also study overlapping two-species condensates, as is commonin the literature, where such terms are important.23

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