Effect of pointlike impurities on dx2−y2 charge-density waves in cuprate superconductors
W. A. Atkinson, A. P. Kampf
DOI 10.1103/PhysRevB.91.104509 · Physical Review B
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Abstract
Many cuprate superconductors possess an unusual charge-ordered phase that is characterized by an approximate dx2−y2 intraunit cell form factor and a finite modulation wave vector q*. We study the effects of impurities on this charge-ordered phase via a single-band model in which bond order is the analog of charge order in the cuprates. Impurities are assumed to be pointlike and are treated within the self-consistent t-matrix approximation. We show that suppression of bond order by impurities occurs through the local disruption of the dx2−y2 form factor near individual impurities. Unlike d-wave superconductors, where the sensitivity of Tc to impurities can be traced to a vanishing average of the dx2−y2 order parameter over the Fermi surface, the response of bond order to impurities is dictated by a few Fermi surface “hotspots.” The bond order transition temperature Tbo thus follows a different universal dependence on impurity concentration ni than does the superconducting Tc. In particular, Tbo decreases more rapidly than Tc with increasing ni when there is a nonzero Fermi surface curvature at the hotspots. Based on experimental evidence that the pseudogap is insensitive to Zn doping, we conclude that a direct connection between charge order and the pseudogap is unlikely. Furthermore, the enhancement of stripe correlations in the La-based cuprates by Zn doping is evidence that this charge order is also distinct from stripes.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Bi2Sr2-xLaxCuO6+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Nd2-xCexCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| La2-xBaxCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| La2-xSrxCuO4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| YBa2Cu3O6+x Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| YBa2Cu3O6.6 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| YBa2Cu3O6.54 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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