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In the general d-dimensional case, 〈Ψ†(r)Ψ(0) 〉 ∝ r-(d-2+η) exp-r/ξ, where η is a critical exponent. The calculated and measured values of η are on the order of 10-2, and therefore we neglect η in our analysis
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The numerical coefficient may be different for a trapped gas and has been omitted in (25).
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The numerical coefficient may be different for a trapped gas and has been omitted in (25).
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We thank G. Blatter, F. Brennecke, A. Kuklov, G. Shlyapnikov, M. Troyer, and W. Zwerger for insightful discussions. Supported by a European Union Marie Curie fellowship under contract MEIF-CT-2005-023612 (T.B, SEP Information Sciences, the Optical lattices and Quantum Information (OLAQUI) project of the European Union, and the Quantum Systems for Information Technology (QSIT) project of ETH Zürich
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We thank G. Blatter, F. Brennecke, A. Kuklov, G. Shlyapnikov, M. Troyer, and W. Zwerger for insightful discussions. Supported by a European Union Marie Curie fellowship under contract MEIF-CT-2005-023612 (T.B.), SEP Information Sciences, the Optical lattices and Quantum Information (OLAQUI) project of the European Union, and the Quantum Systems for Information Technology (QSIT) project of ETH Zürich.
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