The fate of superconductivity and charge order in underdoped YBa2Cu3O6.7 under high magnetic fields

ORAL

Abstract

Due to the small coherence lengths, large anisotropies and high critical temperatures cuprate superconductors exhibit extremely strong superconducting fluctuations. High-resolution capacitance dilatometry on YBa2Cu3Ox has proven to be particularly useful in studying these fluctuation [1-3]. At optimal doping the sc transition is described well by a 3D-XY phase-ordering transition (analogous to the lambda transition in superfluid 4He) [1,2]. For underdoped crystals fluctuations increase and were attributed to anisotropic 3D-XY behavior [3]. Here, using magnetostriction measurements up to 30 T, we investigate how large a magnetic field is necessary to suppress the superconducting transition in an underdoped crystal with an oxygen content of 6.7. We find that 30 T is far from sufficient to fully suppress the transition, in stark contrast to previous work claiming an Hc2 of roughly 20-25 T for this doping [4,5]. Further, we see little thermodynamic evidence in the magnetostriction data at 10 K for a field-induced charge-ordering transition [6].

[1] V. Pasler et al., Phys. Rev. Lett. 81, 1094 (1998).

[2] R. Lortz et al., Phys. Rev. Lett. 91, 207001 (2003).

[3] C. Meingast et al., Phys. Rev. Lett. 86, 1606 (2001).

[4] G. Grissonnanche et al., Nat. Comm. 5, 3280 (2014).

[5] C. Marcenat et al., Nature Comm. 6, 7927 (2015).

[6] J. Chang et al., Nat. Comm 7, 11494 (2016).

Presenters

  • Christoph Meingast

    Karlsruhe Institute of Technology, IQMT, Karlsruhe Institute of Technology, Institut für QuantenMaterialien und Technologien, Karlsruhe Institute of Technology

Authors

  • Christoph Meingast

    Karlsruhe Institute of Technology, IQMT, Karlsruhe Institute of Technology, Institut für QuantenMaterialien und Technologien, Karlsruhe Institute of Technology

  • Anmol Shukla

    IQMT, Karlsruhe Institute of Technology

  • Thom Ottenbros

    High Field Magnet Laboratory, Radboud University, Nijmegen

  • Steffen Wiedmann

    High Field Magnet Laboratory, Radboud University, Nijmegen

  • Matthieu Le Tacon

    IQMT, Karlsruhe Institute of Technology

  • Bernhard Keimer

    Max Planck Institute for Solid State Physics, Max Planck Institute for Solid State Research

  • Frederic Hardy

    Karlsruhe Institute of Technology, Institut für QuantenMaterialien und Technologien, Karlsruhe Institute of Technology