A strange metal with a small Fermi surface and strong collective excitations
F. H. L. Essler, A. M. Tsvelik

TL;DR
This paper proposes a hybrid state in a strongly correlated system where quasi-particles coexist with collective excitations, featuring an unconventional Fermi surface volume unrelated to electron density, emerging from coupled 1D Mott insulators.
Contribution
It introduces a novel hybrid state model with a small Fermi surface and strong collective modes, derived from coupled 1D Mott insulators, and explores its phase transition properties.
Findings
Existence of a hybrid state with a small Fermi surface
Unconventional Fermi surface volume independent of electron density
Antiferromagnetic transition at low temperatures
Abstract
We develop a theory of a hybrid state, where quasi-particles coexist with strong collective modes, taking as a starting point a model of infinitely many 1D Mott insulators coupled by a weak interchain tunneling. This state exists at an intermediate temperature range and undergoes an antiferromagnetic phase transition at temperatures much smaller than the Mott-Hubbard gap. The most peculiar feature of the hybrid state is that the volume of the Fermi surface is unrelated to the electron density. We present a self-consistent derivation of the low energy effective action for our model.
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