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

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Chapter 7<strong>Quantum</strong> simulations <strong>of</strong> evaporativelycooled <strong>Bose</strong>-<strong>Einstein</strong> condensates7.1 Introduction7.1.1 Important issuesWe now undertake to study the quantum dynamics governed by the atom-optics Hamiltonian(Eq. (2.1)) without recourse to the two-mode approximation. Our tools are thequantum optics phase-space techniques introduced in Ch. 6. In the quantum soliton calculations,the initial state is taken to be the coherent output <strong>of</strong> a laser; in other words acoherent state. However, the precise state <strong>of</strong> a <strong>Bose</strong> condensate in an atom trap is currentlyunknown, as it forms by a dynamical evaporative cooling process, in which particleinteractions play a vital role. Also the condensate may never reach equilibrium duringits lifetime. Thus to determine the properties <strong>of</strong> the condensate state, one must study itsformation via the cooling process.The <strong>Bose</strong>-<strong>Einstein</strong> condensate that has been produced with trapped atomic samples<strong>of</strong> neutral atoms[3, 16, 35] is <strong>of</strong>ten described as the atomic equivalent to laser light.Condensates are certainly matter waves characterised by what is called the <strong>of</strong>f-diagonallong-range order parameter. Precise measurements <strong>of</strong> the momentum spread in recentexperiments[165] have shown that the long-range order extends over the entire length <strong>of</strong> thecondensate. Other interference and diffraction experiments[2, 4, 74] have also confirmedthe existence <strong>of</strong> this long-range coherence. But this does not mean that the condensateexists in a coherent state, for which it would have to possess coherence <strong>of</strong> all orders at all140

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