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Effective action for Bose-Einstein condensates

Published 21 May 2014 in cond-mat.quant-gas, cond-mat.supr-con, hep-ph, hep-th, and nucl-th | (1405.5291v1)

Abstract: We clarify basic properties of an effective action (i.e., self-consistent perturbation expansion) for interacting Bose-Einstein condensates, where field ψ\psi itself acquires a finite thermodynamic average ⟨ψ⟩\langle \psi\rangle besides two-point Green's function G^\hat G to form an off-diagonal long-range order. It is shown that the action can be expressed concisely order by order in terms of the interaction vertex and a special combination of ⟨ψ⟩\langle\psi\rangle and G^\hat G so as to satisfy both Noether's theorem and Goldstone's theorem (I) corresponding to the first proof. The self-energy is predicted to have a one-particle-reducible structure due to ⟨ψ⟩≠0\langle \psi\rangle\neq 0 to transform the Bogoliubov mode into a bubbling mode with a substantial decay rate.

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