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Change of carrier density at the pseudogap critical point of a cuprate superconductor

Nature volume 531, pages 210–214 (2016)Cite this article

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Abstract

The pseudogap is a partial gap in the electronic density of states that opens in the normal (non-superconducting) state of cuprate superconductors and whose origin is a long-standing puzzle. Its connection to the Mott insulator phase at low doping (hole concentration, p) remains ambiguous1 and its relation to the charge order2,3,4 that reconstructs the Fermi surface5,6 at intermediate doping is still unclear7,8,9,10. Here we use measurements of the Hall coefficient in magnetic fields up to 88 tesla to show that Fermi-surface reconstruction by charge order in the cuprate YBa2Cu3Oy ends sharply at a critical doping p = 0.16 that is distinctly lower than the pseudogap critical point p* = 0.19 (ref. 11). This shows that the pseudogap and charge order are separate phenomena. We find that the change in carrier density n from n = 1 + p in the conventional metal at high doping (ref. 12) to n = p at low doping (ref. 13) starts at the pseudogap critical point. This shows that the pseudogap and the antiferromagnetic Mott insulator are linked.

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Figure 1: Temperature–doping phase diagram of YBCO.
Figure 2: Field dependence of the Hall coefficient in YBCO.
Figure 3: Temperature dependence of the normal-state Hall coefficient in YBCO at various dopings.
Figure 4: Doping evolution of the normal-state carrier density.

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Acknowledgements

We thank the following for discussions: Y. Ando, D. Basov, G. Boebinger, C. Bourbonnais, J. P. Carbotte, A. Carrington, J. Chang, A. V. Chubukov, J. C. Davis, A. Georges, N. E. Hussey, M.-H. Julien, H.-Y. Kee, S. A. Kivelson, P. A. Lee, T. Loew, G. G. Lonzarich, W. Metzner, A. J. Millis, M. R. Norman, C. Pépin, J. Porras, B. J. Ramshaw, T. M. Rice, G. Rikken, S. Sachdev, D. J. Scalapino, C. B. Taillefer, J. L. Tallon, S. Todadri, and A.-M. S. Tremblay. We also thank P. Frings and J.P. Nicolin for help during the measurements in Toulouse. L.T. thanks the Laboratoire National des Champs Magnétiques Intenses (LNCMI) in Toulouse for their hospitality and LABEX NEXT for their support while this work was being performed. A portion of this work was performed at the LNCMI, which is supported by the French ANR SUPERFIELD, the EMFL, and the LABEX NEXT. R.L., D.A.B. and W.N.H. acknowledge funding from the Natural Sciences and Engineering Research Council of Canada (NSERC). L.T. acknowledges support from the Canadian Institute for Advanced Research (CIFAR) and funding from NSERC, the Fonds de recherche du Québec – Nature et Technologies (FRQNT), the Canada Foundation for Innovation (CFI) and a Canada Research Chair.

Author information

Authors and Affiliations

  1. Département de physique, Regroupement Québécois sur les Matériaux de Pointe, Université de Sherbrooke, Sherbrooke, J1K 2R1, Québec, Canada

    S. Badoux, G. Grissonnanche, N. Doiron-Leyraud & Louis Taillefer

  2. Laboratoire National des Champs Magnétiques Intenses (CNRS, EMFL, INSA, UGA, UPS), Toulouse, 31400, France

    W. Tabis, F. Laliberté, B. Vignolle, D. Vignolles, J. Béard & Cyril Proust

  3. AGH University of Science and Technology, Faculty of Physics and Applied Computer Science, Krakow, 30-059, Poland

    W. Tabis

  4. Department of Physics and Astronomy, University of British Columbia, Vancouver, Columbia, V6T 1Z1, British, Canada

    D. A. Bonn, W. N. Hardy & R. Liang

  5. Canadian Institute for Advanced Research, Toronto, M5G 1Z8, Ontario, Canada

    D. A. Bonn, W. N. Hardy, R. Liang, Louis Taillefer & Cyril Proust

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  1. S. Badoux
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Contributions

S.B., W.T., F.L., B.V., D.V., J.B. and C.P. performed the transport measurements at the LNCMI. S.B. and N.D.-L. performed the transport measurements at Sherbrooke. G.G. performed the calculations of the transport coefficients. D.A.B., W.N.H. and R.L. prepared the YBCO single crystals at UBC. S.B., L.T. and C.P. wrote the manuscript, in consultation with all authors. L.T. and C.P. co-supervised the project.

Corresponding authors

Correspondence to Louis Taillefer or Cyril Proust.

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The authors declare no competing financial interests.

Extended data figures and tables

Extended Data Figure 1 Temperature dependence of resistivity of CuO chains in YBCO at p = 0.177.

Shown is the chain resistivity in YBCO at p = 0.177 (red), defined as ρchain = 1/[(1/ρb) − (1/ρa)], where ρa and ρb are the in-plane resistivities along the a and b directions of the orthorhombic structure, respectively, plotted versus T2. The black line is a linear fit that extrapolates to ρchain = 50 μΩ cm at T = 50 K.

Extended Data Figure 2 Isotherms of RH versus H in YBCO at p = 0.16.

Shown is the magnetic field dependence of the Hall coefficient RH in our YBCO sample with y = 6.92 (Tc = 93.5 K; p = = 0.161) at various temperatures, as indicated (key at right).

Extended Data Figure 3 Isotherms of RH versus H in YBCO at p = 0.177.

As for Extended Data Fig. 2 but for our YBCO sample with y = 6.97 (Tc = 91 K; p = 0.177).

Extended Data Figure 4 Isotherms of RH versus H in YBCO at p = 0.19.

As for Extended Data Fig. 2 but for our YBCO sample with y = 6.99 and 1.4% Ca doping (Tc = 87 K; p = 0.19).

Extended Data Figure 5 Isotherms of RH versus H in YBCO at p = 0.205.

As for Extended Data Fig. 2 but for our YBCO sample with y = 6.99 and 5% Ca doping (Tc = 77 K; p = 0.205).

Extended Data Figure 6 Doping dependence of Tmax.

Shown is the temperature Tmax at which RH versus T peaks in YBCO (Fig. 3a), plotted versus doping p. At p = 0.16, there is no downturn in the normal-state RH(T) down to 40 K. The p = 0.16 data are consistent with Tmax = 0 (lower bound), with an upper bound at Tmax = 40 K (shown as black vertical segment). The width of the grey band marks the upper and lower limits for Tmax versus p. The green diamond defines the critical doping above which FSR is no longer present, at pFSR = 0.16 ± 0.005, with an error bar defined from the minimal and maximal possible values of Tmax. Error bars on the three data points (black dots) represent the uncertainty in defining the peak position of the RH(T) curves in Fig. 3a.

Extended Data Figure 7 Zoom on RH versus T in Tl-2201 and YBCO at high doping.

a, Temperature dependence of RH in Tl-2201 (squares) at p = 0.3 (blue, Tc = 10 K; ref. 38) and p = 0.27 (green, Tc = 25 K; ref. 39). b, RH versus T in YBCO (circles, from Extended Data Figs 4, 5 and 8) at p = 0.205 (yellow) and p = 0.19 (blue). The dashed lines are an extrapolation of the low-T data to T = 0. The YBCO curve at p = 0.205 is qualitatively similar to the two Tl-2201 curves, all exhibiting an initial rise with increasing temperature from T = 0, and a characteristic peak at T ≈ 100 K—two features attributed to inelastic scattering on a large hole-like Fermi surface15. The YBCO curve at p = 0.19 is qualitatively different, showing no sign of a drop at low T (see Extended Data Fig. 8). We attribute the twofold increase in the magnitude of RH at T → 0 to a decrease in carrier density as the pseudogap opens at p*, with p* located between p = 0.205 and p = 0.19. The error bars are defined in the legend of Fig. 3.

Extended Data Figure 8 Comparison between p = 0.205 and p = 0.19.

a, b, The field dependence of the Hall coefficient RH in YBCO at p = 0.205 (a) and p = 0.19 (b), for different temperatures as indicated. The colour-coded lines are parallel linear fits to the high-field data. They show that at low temperature RH decreases upon cooling at p = 0.205, while it saturates at p = 0.19. The value of RH given by the fit line, at H = 80 T, is plotted in Fig. 3 and in Extended Data Fig. 7b. Similar fits are used to extract RH(80 T) for p = 0.16 and p = 0.177 (from data in Extended Data Figs 2 and 3).

Extended Data Figure 9 Scenario of inelastic scattering.

a, RH versus T in YBCO at four dopings p, as indicated (Fig. 3b). b, Electrical resistivity ρa versus T in YBCO at four dopings, as indicated. Lines are at H = 0; dots are in the normal state at high field. c, RH versus T calculated for five values of inelastic scattering, with Γ1 = 0, 1, 5, 15 and 25 THz K−1, showing that RH(T) grows with increasing Γ1 (see Methods). Dots are from a. d, Corresponding calculated values of the electrical resistivity ρa, plotted versus T, using the same parameters and values of Γ1 as for the colour-coded curves of c. The vertical grey lines mark T = 50 K, the temperature at which we see a sixfold increase in RH (a), yet no increase in ρa (b). The calculation can reproduce the large increase in RH (c), but it is accompanied by a tenfold increase in ρa (d).

Extended Data Figure 10 Magnetic field profile.

Time dependence of the magnetic field pulse in the 90 T dual-coil magnet at the LNCMI in Toulouse. Inset, zoom around maximum field.

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Badoux, S., Tabis, W., Laliberté, F. et al. Change of carrier density at the pseudogap critical point of a cuprate superconductor. Nature 531, 210–214 (2016). https://doi.org/10.1038/nature16983

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