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See, e.g., A.J. Millis, H. Monien, and D. Pines, Phys. Rev. B 42, 167 (1990).
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note
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2 regime for Im Σ is rather narrow in energy and will be washed out by finite temperature effects, precluding their observation experimentally except in the heavily overdoped limit.
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27
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and references therein
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30
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1542333779
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A similar observation has been made by B. Farid, Philos. Mag. 84, 909 (2004).
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This S shape from phonons is obvious in earlier work as well; see S. Verga, A. Knigavko, and F. Marsiglio, Phys. Rev. B 67, 054503 (2003); E. Schachinger, J. J. Tu, and J. P. Carbotte, ibid. 67, 214508 (2003); A.W. Sandvik, D.J. Scalapino, and N.E. Bickers, ibid. 69, 094523 (2004).
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32
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0038038401
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This S shape from phonons is obvious in earlier work as well; see S. Verga, A. Knigavko, and F. Marsiglio, Phys. Rev. B 67, 054503 (2003); E. Schachinger, J. J. Tu, and J. P. Carbotte, ibid. 67, 214508 (2003); A.W. Sandvik, D.J. Scalapino, and N.E. Bickers, ibid. 69, 094523 (2004).
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33
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2142701488
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This S shape from phonons is obvious in earlier work as well; see S. Verga, A. Knigavko, and F. Marsiglio, Phys. Rev. B 67, 054503 (2003); E. Schachinger, J. J. Tu, and J. P. Carbotte, ibid. 67, 214508 (2003); A.W. Sandvik, D.J. Scalapino, and N.E. Bickers, ibid. 69, 094523 (2004).
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34
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12244272887
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note
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In real materials, the phonon density of states has a large spread in energy which also acts to smear the S shape; see Verga et al. and Schachinger et al. of Ref. 27. However, this broadening also reduces the renormalization of the Fermi velocity, as can be seen from Eq. (49).
-
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-
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35
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-
12244274817
-
-
cond-mat/0402457 (unpublished)
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But if the bare Green's function is assumed to be a Luttinger liquid, then the S shape from an Einstein mode is also smeared out; see I.P. Bindloss and S.A. Kivelson, cond-mat/0402457 (unpublished).
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Bindloss, I.P.1
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0037809383
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Similar results have been obtained from FLEX calculations by D. Manske, I. Eremin, and K.H. Bennemann, Phys. Rev. Lett. 87, 177005 (2001); Phys. Rev. B 67, 134520 (2003).
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