Abstract

Hole-doped high-temperature cuprate superconductors below optimum doping have small electron-like Fermi surfaces occupying a small fraction of the Brillouin zone. There is strong evidence that this is linked to charge density wave (CDW) order, which reconstructs the large hole-like Fermi surfaces predicted by band structure calculations . Recent experiments have revealed the structure of the two CDW components in the benchmark bilayer material YBa$_2$Cu$_3$O$_{7-x}$ in high field where quantum oscillation (QO) measurements are performed. We have combined these results with a tight-binding description of the bands in an isolated bilayer to give a minimal model revealing the essential physics of the situation. Here we show that this approach, combined with the effects of spin-orbit interactions and the pseudogap, gives a good qualitative description of the multiple frequencies seen in the QO observations in this material. Magnetic breakdown through weak CDW splitting of the bands will lead to a field-dependence of the QO spectrum and to the observed fourfold symmetry of the results in tilted fields.

Highlights

  • In recent years, a clear picture of the variation of the electronic structure of cuprate high-Tc materials with doping has emerged

  • For the case considered here, the important process is magnetic breakdown from A to A or B to B at the red crossing points in Fig. 1. (We propose that breakdown out of the Fermi arcs towards the edges of the Brillouin zone (BZ) is prevented by the PG.) Assuming that the charge density wave (CDW) gaps are comparable with those due to A-B splitting, we may use the quantum oscillation (QO) data to give an order of magnitude for the gap kg between different Fermi surface (FS) areas, and this will indicate at what fields magnetic breakdown may be important

  • We have demonstrated how multiple QO frequencies observed in YBCO are naturally explained by the odd symmetry of the CDW order, combined with the effects of spin-orbit interaction and magnetic breakdown

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Summary

INTRODUCTION

A clear picture of the variation of the electronic structure of cuprate high-Tc materials with doping has emerged. Overdoped materials have large holelike cylindrical Fermi surfaces with cross sections reflecting the single hole on a Cu2+ plus the additional carriers due to doping [1], whereas on the underdoped side of the superconducting dome, quantum oscillation (QO) measurements [2] indicate small electronlike Fermi surface (FS) areas that occupy only ∼2% of the Brillouin zone (BZ). This strongly suggested a FS reconstruction arising from broken translational symmetry [3].

BASIC MECHANISM FOR THE FS RECONSTRUCTION
THE NATURE OF THE BILAYER WAVE FUNCTIONS
EFFECTS OF THE CDW–FERMI SURFACE CALCULATIONS
EFFECTS OF MAGNETIC FIELD AND SO INTERACTIONS ON FERMI
MAGNETIC BREAKDOWN
VIII. EFFECTS OF TILTING THE MAGNETIC FIELD AWAY FROM THE c axis
MAGNETIC BREAKDOWN AND ORBIT AREAS
Findings
DISCUSSION
CONCLUSIONS
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