Mottness, Phase String, and High-$T_c$ Superconductivity

TL;DR

This paper proposes that the phase-string effect in strongly correlated electrons fundamentally alters the low-energy physics of Mott insulators, leading to a new non-Fermi-liquid state that underpins high-$T_c$ superconductivity.

Contribution

It introduces the phase-string concept as a key factor in understanding Mottness and high-$T_c$ superconductivity, highlighting a topological gauge structure and electron fractionalization.

Findings

Identification of phase-string as a replacement for Fermi statistics in Mott insulators.

Evidence of a non-Fermi-liquid parent state with Fermi arcs and gapped spinons.

Numerical and experimental support for the emergent physics of Mottness in cuprates.

Abstract

It is a great discovery in physics of the twentieth century that the elementary particles in Nature are dictated by gauge forces, characterized by a nonintegrable phase factor that an elementary particle of charge $q$ acquires from A to B points: $$P \exp\left(i\frac{q}{\hbar c} \int_A^B A_\mu dx^\mu\right)$$ where $A_\mu$ is the gauge potential and $P$ stands for path ordering. In a many-body system of strongly correlated electrons, if the so-called Mott gap is opened up by interaction, the corresponding Hilbert space will be fundamentally changed. A novel nonintegrable phase factor known as phase-string will appear and replace the conventional Fermi statistics to dictate the low-lying physics. Protected by the Mott gap, which is clearly identified in the high-$T_c$ cuprate with a magnitude > 1.5 eV, such a singular phase factor can enforce a fractionalization of the electrons, leading to a dual world of exotic elementary particles with a topological gauge structure. A non-Fermi-liquid "parent" state will emerge, in which the gapless Landau quasiparticle is only partially robust around the so-called Fermi arc regions, while the main dynamics are dominated by two types of gapped spinons. Antiferromagnetism, superconductivity, and a Fermi liquid with full Fermi surface can be regarded as the low-temperature instabilities of this new parent state. Both numerics and experiments provide direct evidence for such an emergent physics of the Mottness, which lies in the core of a high-$T_c$ superconducting mechanism.