Topological Theory of Electron-Phonon Interactions in High Temperature Superconductors

TL;DR

This paper introduces a topological approach to understanding electron-phonon interactions in high-temperature superconductors, emphasizing nanoscale phase separation and quantum percolation, explaining experimental anomalies and universal features.

Contribution

It applies topological, nonperturbative methods to explain complex HTSC phenomena, including phase diagrams and spectral features, without relying on microscopic assumptions.

Findings

Explains the isotope effects and spectral anomalies in HTSC.

Describes the role of nanoscale phase separation and filamentary dopant structures.

Accounts for the universal kink energy and Fermi velocity across cuprates.

Abstract

There are large isotope effects in the phonon kinks observed in photoemission spectra (ARPES) of optimally doped cuprate high temperature superconductors (HTSC), but they are quite different (Gweon et al. 2004) from those expected for a nearly free electron metal with strong electron-phonon interactions (Tang et al. 2003). These differences, together with many other anomalies in infrared spectra, seem to suggest that other particles (such as magnons) must be contributing to HTSC. Here we use topological (non-Hamiltonian) methods to discuss the data, emphasizing nanoscale phase separation and the importance of a narrow band of quantum percolative states near the Fermi energy that is spatially pinned to a self-organized filamentary dopant array. Topological discrete, noncontinuum, nonperturbative methods have previously explained the form of HTSC phase diagrams without involving detailed microscopic assumptions, and they are especially useful in the presence of strong nanoscale disorder. These methods also explain the ``miracle'' of an ideal nearly free electron phonon kink in sharply defined nodal quasiparticle states in LSCO at the metal-insulator transition. Finally the universality of the kink energy and Fermi velocity in different cuprates is the result of the marginally elastic nature of these materials, and specifically the isostatic character of the CuO2 planes.