Abstract

We present a Green’s function-based framework for modeling the scanning tunneling spectrum from the normal as well as the superconducting state of complex materials where the nature of the tunneling process—i.e., the effect of the tunneling “matrix element,” is properly taken into account. The formalism is applied to the case of optimally doped Bi₂Sr₂CaCu2=₂O8+δ (Bi2212) high-Tc superconductor using a large tight-binding basis set of electron and hole orbitals. The results show clearly that the spectrum is modified strongly by the effects of the tunneling matrix element and that it is not a simple replica of the local density of states of the Cu dₓ2₋y2 orbitals with other orbitals playing a key role in shaping the spectra. We show how the spectrum can be decomposed usefully in terms of tunneling “channels” or paths through which the current flows from various orbitals in the system to the scanning tip. Such an analysis reveals symmetry-forbidden and symmetry-enhanced paths between the tip and the cuprate layers. Significant contributions arise from not only the CuO₂ layer closest to the tip but also from the second CuO₂ layer. The spectrum also contains a longer range background reflecting the nonlocal nature of the underlying Bloch states. In the superconducting state, coherence peaks are found to be dominated by the anomalous components of Green’s function.

Notes

Originally published in Physical Review B v.80 (2009): 134509. DOI: 10.1103/PhysRevB.80.134509

Keywords

Bi₂Sr₂CaCu₂O₈₊δ, CuO₂, Block states, spectral decomposition, matrix element effects

Subject Categories

Tunneling spectroscopy

Disciplines

Physics

Publisher

American Physical Society

Publication Date

10-9-2009

Rights Information

Copyright 2009 American Physical Society

Rights Holder

American Physical Society


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