Abstract

We obtain a rigorous solution of universal Bose gases near resonance and offer an answer to one of the long-standing challenges of quantum gases at large scattering lengths, where the standard dilute theory breaks down. The solution was obtained by using an εε expansion near four spatial dimension. In dimension d=4−εd = 4 - ε, the chemical potential of Bose gases near resonances is shown to approach the universal value ε(2/(4−ε))εF2/3(1+0.474ε−i1.217ε+...)ε^{(2/(4-ε))} ε_F \sqrt{2/3} (1 + 0.474 ε- i 1.217 ε+ ...), where εFε_F is the Fermi energy defined for a Fermi gas of density nn, and the condensation fraction is equal to 2/3(1+0.0877ε+...)2/3 (1 + 0.0877 ε+ ...). We also discuss the implications on ultra-cold gases in physical dimensions.

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