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The local density of states power spectrum of optimally doped Bi₂Sr₂CaCu₂O₈₊ₓ (BSCCO) has been interpreted in terms of quasiparticle interference peaks corresponding to an ``octet'' of scattering wave vectors connecting k points where the density of states is maximal. Until now, theoretical treatments have not been able to reproduce the experimentally observed weights and widths of these octet peaks; in particular, the predominance of the dispersing ``q₁'' peak parallel to the Cu-O bond directions has remained a mystery. In addition, such theories predict ``background'' features which are not observed experimentally. Here, we show that most of the discrepancies can be resolved when a realistic model for the out-of-plane disorder in BSCCO is used. Weak extended potential scatterers, which are assumed to represent cation disorder, suppress large-momentum features and broaden the low-energy ``q₇'' peaks, whereas scattering at order parameter variations, possibly caused by a dopant-modulated pair interaction around interstitial oxygens, strongly enhances the dispersing q₁ peaks.
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Nunner et al. (2006) studied this question.
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