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Strictly speaking, Eq. (32) applies at times not exceeding the inverse Thouless energy, while at longer times a somewhat different dependence holds.
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64
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2 (0), can be interpreted as an effective renormalization of the non-interacting result (13). This assumption turns out to be inconsistent with our exact result (25) either.
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35448995900
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φ{symbol} obtained from fits with the Airy function [6,10] should be adjusted (moved upwards) by a numerical factor ∼ 4. For further discussion of this point we refer the reader to Appendix B in Ref. [7]. We also note that the adjustment of the data points [6,10] was carried out only in Fig. 7 but not in Fig. 6.
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75
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35448930951
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φ{symbol} to our theory. This procedure was described in details in Ref. [46].
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35448997977
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φ{symbol} for the samples G and H are, respectively, 1.9 μ m and 2.6 μ m [78]. Their ratio ≈ 0.73 matches perfectly with our theoretical prediction ≈ 0.75, cf. Table II in Ref. [11].
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D. Natelson, private communication, 2007.
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