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Magnetic oscillations measure interlayer coupling in cuprate superconductors

P. D. Grigoriev and Timothy Ziman
Phys. Rev. B 96, 165110 – Published 5 October 2017

Abstract

The magnetic oscillations in YBCO high-temperature superconductors have been widely studied over the last decade and consist of three equidistant low frequencies with a central frequency several times more intense than its two shoulders. This remains a puzzle in spite of numerous attempts to explain the corresponding small Fermi-surface pockets. Furthermore, the ARPES data indicate only four Fermi arcs with bilayer splitting, and show no sign of such small areas in the Fermi surface. Here we argue that the magnetic oscillations measured in underdoped bilayer high-temperature superconductors, in particular YBa2Cu3O6+δ, provide a measure of the interplanar electronic coupling rather than the areas of fine-grain reconstruction of the Fermi surfaces coming from induced charge density waves. This identification is based on the relative intensities of the different peaks, as well as their angular dependence, which points to an effective Fermi surface that is larger than the oscillation frequencies, and is compatible with several indications from ARPES. The dominance of such frequencies with respect to the fundamental frequencies from the Fermi surface is natural for a strongly correlated quasi-two-dimensional electronic system where nonlinear mixings of frequencies are more resistant to sample inhomogeneity.

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  • Received 7 June 2016
  • Revised 19 September 2017

DOI:https://doi.org/10.1103/PhysRevB.96.165110

©2017 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

P. D. Grigoriev1,2,3 and Timothy Ziman4,5

  • 1L. D. Landau Institute for Theoretical Physics, 142432 Chernogolovka, Russia
  • 2National University of Science and Technology “MISiS”, Moscow 119049, Russia
  • 3P.N. Lebedev Physical Institute, RAS, 119991, Moscow, Russia
  • 4Institut Laue-Langevin, BP 156, 41 Avenue des Martyrs, 38042 Grenoble Cedex 9, France
  • 5LPMMC (UMR 5493), Université de Grenobles-Alpes and CNRS, Maison des Magistères, BP 166, 38042 Grenoble Cedex 9, France

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Issue

Vol. 96, Iss. 16 — 15 October 2017

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Images

  • Figure 1
    Figure 1

    The bilayer crystal structure and Fermi surface of YBCO. (a) The crystal structure in YBCO, producing the bilayer splitting to bonding (B) and antibonding (AB) electron states and Fermi-surface parts. (b) The schematically shown in-plane Fermi surface (FS) in YBCO, seen by ARPES and without fine-grained reconstruction. The solid green lines show Fermi arcs of bonding FS, and the red lines show the antibonding FS. The dashed lines show the FS parts shifted by the vector Q=(π/a,π/b). The dashed and solid lines together form two closed FS pockets, corresponding to bonding and antibonding states and responsible for the Fβ1.6kT frequency, about 6% of the Brillouin zone. The most prominent Fα frequency 2% of Brillouin zone corresponds to double the difference between green and red FS pockets, i.e., between B and AB FS pockets, the area shaded in purple. (c) The illustration of a quasi-2D Fermi surface with interlayer warping due to 2tz and double bilayer splitting due to 2t.

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  • Figure 2
    Figure 2

    Predicted magnetic oscillations in quasi-2D conductor with bilayer splitting. (a) The Fourier transform of magnetic oscillations given by Eq. (7) at four different Dingle temperatures πTD/ωc(Bz=1T)=1 (dashed black line), 3 (solid blue line), 5 (dotted red line), and 7 (dash-dotted green line). Insert shows the initial function σSlO1/Bz at πTD/ωc(Bz=1T)=3. (b) The Fourier transform of conductivity in Eq. (7) at TD=0 but in the finite field intervals 20T<Bz<100T (solid black line), 20T<Bz<65T (dashed green line), 25T<Bz<65T (dash-dotted blue line), and 30T<Bz<65T (dotted red line).

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