Energy gaps in failed superconductor La$_{1.875}$Ba$_{0.125}$CuO$_{4}$

ORAL

Abstract

By angle-resolved photoemission spectroscopy with improved energy and momentum resolution, we find in the normal state of La$_{2-x}$Ba$_{x}$CuO$_{4}$ x = 1/8 a strong existence of the nodal quasi-particle together with a $d$-wave energy gap along the underlying Fermi surface extending over a significant range in the momentum space before an abrupt take-off of the gap close to the antinodal region. This suggests the presence of a novel nodal metal state, which is different from the one proposed that assumes a single $d$-wave extension of the pseudogap from the antinode toward the node along the whole underlying Fermi surface. This state is compatible with the static stripe ordering but only involves a precursor pairing of the electrons away from the antinodal region. We argue that the traditional pseudogap defined exclusively for the antinodal states has a distinct origin than its new nodal counterpart, i.e., a $d$-wave gap above T$_{c}$. Moreover, this normal state gap function is found to be quantitatively very similar with those of La$_{2-x}$Sr$_{x}$CuO$_{4}$ x$\sim $1/8 (T$_{c}<<$4K) in the superconducting state, pointing to a universal doping dependence of the pairing strength for La-based cuprates, which also highlights the inherent lack of a global phase coherence in La$_{2-x}$Ba$_{x}$CuO$_{4}$ x = 1/8 that makes it a failed superconductor.

Authors

  • R.-H. He

    • Dept of Phys, Appl Phys, SSRL, Stanford Univ.
  • K. Tanaka

    • SSRL, Stanford and ALS, LBNL
  • S.-K. Mo

    • SSRL, Stanford and ALS, Berkeley
  • T. Sasagawa

    • SSRL, Stanford and Mat. and Struc. Lab,TIT, Japan
  • M. Fujita

    • Inst. of Mat. Res.,Tohoku Univ, Japan
  • N. Mannella

    • SSRL, Stanford and ALS, Berkeley
  • K. Yamada

    • Tohoku, Japan
  • Z. Hussain

    • ALS, Berkeley
  • Z.-X. Shen

    • Stanford University
    • Geballe Laboratory for Advanced Materials, Stanford University
    • SSRL, Stanford