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Sensitivity of Tc to pressure and magnetic field in the cuprate superconductor YBa2Cu3Oy: Evidence of charge-order suppression by pressure

O. Cyr-Choinière, D. LeBoeuf, S. Badoux, S. Dufour-Beauséjour, D. A. Bonn, W. N. Hardy, R. Liang, D. Graf, N. Doiron-Leyraud, Louis Taillefer

DOI 10.1103/PhysRevB.98.064513 · Physical Review B

T1

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Abstract

Cuprate superconductors have a universal tendency to form charge density-wave (CDW) order which competes with superconductivity and is strongest at a doping p≃0.12. Here we show that in the archetypal cuprate YBa2Cu3Oy (YBCO) pressure suppresses charge order but does not affect the pseudogap phase. This is based on transport measurements under pressure, which reveal that the onset of the pseudogap at T* is independent of pressure, while the negative Hall effect, a clear signature of CDW order in YBCO, is suppressed by pressure. We also find that pressure and magnetic field shift the superconducting transition temperature Tc of YBCO in the same way as a function of doping—but in opposite directions—and most effectively at p≃0.12. This shows that the competition between superconductivity and CDW order can be tuned in two ways, either by suppressing superconductivity with field or suppressing CDW order by pressure. Based on existing high-pressure data and our own work, we observe that when CDW order is fully suppressed at high pressure, the so-called “1/8 anomaly” in the superconducting dome vanishes, revealing a smooth Tc dome which now peaks at p≃0.13. We propose that this Tc dome is shaped by the competing effects of the pseudogap phase below its critical point p★∼0.19 and spin order at low doping.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
YBa2Cu3Oy

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54.5Pressure unresolvedzero_resistance
YBa2Cu3Oy

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

60.2Pressure unresolvedzero_resistance
YBa2Cu3Oy

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

65.3Pressure unresolvedzero_resistance
YBa2Cu3Oy

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

61.3Pressure unresolvedzero_resistance
YBa2Cu3Oy

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66Pressure unresolvedzero_resistance
YBa2Cu4O8

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

80Pressure not reportedunknown

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