Thermal Hall conductivity in the strongest cuprate superconductor: Estimate of the mean free path in the trilayer cuprate HgBa2Ca2Cu3O8+δ
Munkhtuguldur Altangerel, Quentin Barthélemy, Étienne Lefrançois, Jordan Baglo, Manel Mezidi, Gaël Grissonnanche, Ashvini Vallipuram, Emma Campillo, Anne Forget, Dorothée Colson, Ruixing Liang, D. A. Bonn, W. N. Hardy, Cyril Proust, Louis Taillefer
DOI 10.1103/1gp5-h875 · Physical Review B
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Abstract
The thermal Hall conductivity of the trilayer cuprate HgBa2Ca2Cu3O8+δ (Hg1223)—the superconductor with the highest critical temperature Tc at ambient pressure—was measured at temperatures down to 2 K for three dopings in the underdoped regime (p=0.09,0.10,0.11). By combining a previously introduced simple model and prior theoretical results, we derive a formula for the inverse mean free path, 1/ℓ, which allows us to estimate the mean free path of d-wave quasiparticles in Hg1223 below Tc. We find that 1/ℓ grows as T3, in agreement with the theoretical expectation for a clean d-wave superconductor. Measurements were also conducted on the single layer mercury-based cuprate HgBa2CuO6+δ (Hg1201), revealing that the mean free path in this compound is roughly half that of its three-layered counterpart at the same doping (p=0.10). This observation is attributed to the protective role of the outer planes in Hg1223, which results in a more pristine inner plane. We also report data in an ultraclean crystal of YBa2Cu3Oy (YBCO) with full oxygen content (p=0.18), believed to be the cleanest of any cuprate, and find that ℓ is not longer than in Hg1223.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| HgBa2Ca2Cu3O8+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 78 | Pressure not reported | onset |
| HgBa2Ca2Cu3O8+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 95 | Pressure not reported | onset |
| HgBa2Ca2Cu3O8+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 112 | Pressure not reported | onset |
| HgBa2CuO6+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 76 | Pressure not reported | unknown |
| YBa2Cu3Oy Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 90.5 | Pressure not reported | unknown |
| Tl2Ba2CuO6+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 15 | Pressure not reported | unknown |
| Bi2Sr2CaCu2O8+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 50 | Pressure not reported | unknown |
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